..54.0,19.1:*
CORRSIN, S.; KARWEIT, M.*
Fluid line growth in grid-generated isotropic turbulence.*
J. Fluid Mech. 39, 87*
1969. `
..54.0,19.3:*
ORSZAG, S.A.; CROW, S.C.*
Instability of a vortex sheet leaving a semi-plate.*
Boeing Sci. Res. Lab. D1-82-0953*
1970. `
..05.0,19.2: analogy between wall law and Kolmogorov theory - also briefly in Tennekes and Lumley*
MELLOR, G.L.*
The large Reynolds number asymptotic theory of turbulent boundary layers*
Int. J. Engg Sci. 10, 851*
1972. `
..12.2,19.3,19.4:  regards unpredictability as fairly obvious - Kraichnan DIA calcs.*
HERRING, J.R.; RILEY, J.J.*
Growth of uncertainty in decaying isotropic turbulence*
J. Atmos. Sci. 30, 997*
1973. `
..19.2: disapproves of lognormal dissipation*
MANDELBROT, B. B.*
Intermittent turbulence in self-similar cascades - divergence of high moments and dimension of the carrier*
J. Fluid Mech. 62, 331*
1974. `
..19.3: asymptotic behavior of invariants*
LUMLEY, J.L.; NEWMAN, G.R.*
The return to isotropy of homogeneous turbulence*
J. FLuid Mech. 82, 161*
1977. `
..19.2,21.2: blames large-scale structures for anomalous T derivatives - small scales are isotropic*
SREENIVASAN, K.R.; ANTONIA, R.A.; BRITZ, D.*
Local isotropy and large structuress in a heated turbulent jet*
J. Fluid Mech. 94, 745*
1979. `
..19.2: zither, a.k.a. mandoline*
KELLOGG, R.M.; CORRSIN, S.*
Evolution of a spectrally local disturbance in grid-generated, nearly isotropic turbulence*
J. Fluid Mech. 96, 641*
1980. `
..19.1,42.3: Re, lambda of 60 from towed grid in vertical water tank*
DICKEY, T.D.; MELLOR, G.L.*
Decaying turbulence in neutral and stratified fluids*
J. Fluid Mech. 99, 13*
1980. `
..19.1,11.3: mandoline like*
SREENIVASAN, K.R.; TAVOULARIS, S.; HENRY, R.; CORRSIN,S.*
Temperature fluctuations and scales in grid-generated turbulence.*
J. Fluid Mech. 100, 597*
1980. `
..19.2: mu = 0.25 for Re, lambda greater than 200*
VAN ATTA, C.W.; ANTONIA, R.A.*
Reynolds number dependence of skewness and flatness factors of turbulent velocity derivatives*
Phys. Fluids 23, 252*
1980. `
..19.1,42.3: grid dropped through interface*
LINDEN, P.F.*
Mixing across a density interface produced by grid turbulence.*
J. Fluid Mech. 100, 691*
1980. `
..19.3,01.1: copious statistics*
TUNG, T.C.; ADRIAN, R.J.*
Higher order estimates of conditional eddies in isotropic turbulence.*
Phys. Fluids 23, 1469*
1980. `
..21.2,19.2:Re, lambda up to 1000 - local isotropy assumed*
ANTONIA, R.A.; SATYAPRAKASH, B.R.; HUSSAIN, A.K.M.F.*
Measurements of dissipation rate and some other characteristics of turbulent plane and circular jets*
Phys. Fluids 23, 695*
1980. `
..12.2,19.3: damped quasi-Gaussian approx - too rarefied to be useful?*
CAMBON, C.; JEANDEL, D.; MATHIEU, J.*
Spectral modelling of homogeneous non-isotropic turbulence*
J. Fluid Mech. 104, 247*
1981. `
..19.2:straight line between two curves gives mu=0.2*
ANTONIA, R.A.; CHAMBERS, A.J.; SATYAPRAKASH, B.R.*
Reynolds number dependence of high-order moments of the streamwise turbulent velocity derivatives*
Boundary-Layer Met. 21, 159*
1981. `
..19.2,43.0: correln - spectrum relation inadequate at real Re*
ANTONIA, R.A.; CHAMBERS, A.J.; SATYAPRAKASH, B.R.*
Kolmogorov constants for structure functions in turbulent shear flows*
Quart. J. Roy. Met. Soc. 107, 579*
1981. `
..19.2,24.7: vortices occupy space with dimension 2.5*
CHORIN, A.J.*
Estimates of intermittency, spectra, and blow-up in developed turbulence*
Comm. Pure Appl. Math. 34, 853*
1981. `
..11.2,19.2:eps, theta 1.5 times iso value - good balance*
ANTONIA, R.A.; BROWNE, L.W.B.; CHAMBERS, A.J.; RAJAGOPALAN, S.*
Budget of the temperature variance in a turbulent plane jet*
Int. J. Heat Mass Transf. 26, 41*
1983. `
..19.0,11.3: mainly the toaster method of producing dTdy*
SIRIVAT, A.; WARHAFT, S.*
The effect of a passive cross stream temperature gradient on the evolution of temperature variance and heat flux in grid turbulence*
J. Fluid Mech. 128, 323*
1983. `
..19.3: Lyon*
GENCE, J.N.*
Homogeneous turbulence*
Ann. Rev. Fluid Mech. 15, 201*
1983. `
..11.2,19.2,21.2: temp. var. eqn*
ANTONIA, R.A.; BROWNE, L.W.B.*
The destruction of temperature fluctuations in a turbulent plane jet*
J. Fluid Mech. 134, 67*
1983. `
..24.1,19.0:backstep - pairing inhibited after reatt.*
TROUTT, T.R.; SCHEELKE, B.; NORMAN, T.R.*
Organized structures in a reattaching separated flow field*
Mech. Engg Dept., U. of Washington paper*
1983. `
..11.2,19.3:Kolmogorov relation for u only for r<5eta*
ANTONIA, R.A.; CHAMBERS, A.J.; BROWNE, L.W.B.*
Relations between structure functions of velocity and temperature in a turbulent jet*
Expts. in Fluids 1, 213*
1983. `
..31.1,19.0: yes*
BROWNE, L.W.B.; ANTONIA, R.A.; CHAMBERS, A.J.*
Effect of the separation between cold wires on the spatial derivatives of temperature in a turbulent flow*
Boundary-Layer Met. 27, 129*
1983. `
..19.3: frequency is reciprocal of micro timescale*
SREENIVASAN, K.R.; PRABHU, A.; NARASIMHA, R.*
Zero-crossings in turbulent signals*
J. Fluid Mech. 137, 251*
1983. `
..11.2,19.2,21.3:correction to T's H do not seem warranted*
BROWNE, L.W.B.; ANTONIA, R.A.; RAJAGOPALAN, S.*
The spatial derivative of temperature in a turbulent flow and Taylor's hypothesis*
Phys. Fluids 26, 1222*
1983. `
..19.3,54.0: thin axi. layer with radially-periodic circumferential force - several vortex cells like rotating disk flow*
OBUKHOV, A.M.*
Kolmogorov flow and laboratory simulation of it*
Uspekhi Mat. Nauk / Russian Math. Surveys vol. 38, no. 4, p. 113*
1983. `
..11.2,19.2:eps, theta 1.5 times iso value - good balance*
ANTONIA, R.A.; BROWNE, L.W.B.; CHAMBERS, A.J.; RAJAGOPALAN, S.*
Budget of the temperature variance in a turbulent plane jet*
Int. J. Heat Mass Transf. 26, 41*
1983. `
..19.0,11.3: mainly the toaster method of producing dTdy*
SIRIVAT, A.; WARHAFT, S.*
The effect of a passive cross stream temperature gradient on the evolution of temperature variance and heat flux in grid turbulence*
J. Fluid Mech. 128, 323*
1983. `
..19.3: Lyon*
GENCE, J.N.*
Homogeneous turbulence*
Ann. Rev. Fluid Mech. 15, 201*
1983. `
..11.2,19.2,21.2: temp. var. eqn*
ANTONIA, R.A.; BROWNE, L.W.B.*
The destruction of temperature fluctuations in a turbulent plane jet*
J. Fluid Mech. 134, 67*
1983. `
..24.1,19.0:backstep - pairing inhibited after reatt.*
TROUTT, T.R.; SCHEELKE, B.; NORMAN, T.R.*
Organized structures in a reattaching separated flow field*
Mech. Engg Dept., U. of Washington paper*
1983. `
..11.2,19.3:Kolmogorov relation for u only for r<5eta*
ANTONIA, R.A.; CHAMBERS, A.J.; BROWNE, L.W.B.*
Relations between structure functions of velocity and temperature in a turbulent jet*
Expts. in Fluids 1, 213*
1983. `
..31.1,19.0: yes*
BROWNE, L.W.B.; ANTONIA, R.A.; CHAMBERS, A.J.*
Effect of the separation between cold wires on the spatial derivatives of temperature in a turbulent flow*
Boundary-Layer Met. 27, 129*
1983. `
..19.3: frequency is reciprocal of micro timescale*
SREENIVASAN, K.R.; PRABHU, A.; NARASIMHA, R.*
Zero-crossings in turbulent signals*
J. Fluid Mech. 137, 251*
1983. `
..11.2,19.2,21.3:correction to T's H do not seem warranted*
BROWNE, L.W.B.; ANTONIA, R.A.; RAJAGOPALAN, S.*
The spatial derivative of temperature in a turbulent flow and Taylor's hypothesis*
Phys. Fluids 26, 1222*
1983. `
..19.3,54.0: thin axi. layer with radially-periodic circumferential force - several vortex cells like rotating disk flow*
OBUKHOV, A.M.*
Kolmogorov flow and laboratory simulation of it*
Uspekhi Mat. Nauk / Russian Math. Surveys vol. 38, no. 4, p. 113*
1983. `
..19.0,13.0: eddy vis. like 2-pt closure*
DOMARADZKI, J.A.; MELLOR, G.L.*
A simple turbulence closure hypothesis for the triple velocity correlation functions in homogeneous isotropic turbulence*
J. Fluid Mech. 140, 45*
1984. `
..19.3,21.2: higher order moments diverge from log normal expectation*
ANSELMET, F.; GAGNE, Y.; HOPFINGER, E.J.; ANTONIA, R.A.*
High order velocity structure functions in turbulence shear flows*
J. Fluid Mech. 140, 63*
1984. `
..11.3,19.3,24.1:calcs show enstrophic vortex pairing*
HOLLOWAY, G.; KRISTMANNSSON, S.S.*
Stirring and transport of tracer fields by geostrophic turbulence*
J. Fluid Mech. 141, 27*
1984. `
..19.3,25.6: assumes spectral gap - but no worse than LES concept*
TSUGI, S.*
Separability into coherent and chaotic time dependences of turbulent fluctuations*
Phys. Fluids 27, 1370*
1984. `
..19.3,11.1: simple integrable vel. field can produce chaotic conc.*
AREF, H.*
Stirring by chaotic advection*
J. Fluid Mech. 143, 1*
1984. `
..19.2: easily put off by buoyancy etc.*
GARGETT, A.E.; OSBORN, T.R.; NASMYTH, P.W.*
Local isotropy and the decay of turbulence*
J. Fluid Mech. 144, 231*
1984. `
..19.2,43.1: for dissipation - from high order structure functions*
CHAMBERS, A.J.; ANTONIA, R.A.*
Atmospheric estimates of power-law exponents mu and mu, theta*
Boundary-Layer Met. 28, 343*
1984. `
..19.1: mandoline (Zither) vortex sheet - some mean shear effects*
ITSWEIRE, E.C.; VAN ATTA, C.W.*
An experimental study of the response of nearly isotropic turbulence to a spectrally local disturbance*
J. Fluid Mech. 145, 423*
1984. `
..19.3: U^3/L independent of Re, of course, for Re, lambda > 50*
SREENIVASAN, K.R.*
On the scaling of the turbulent dissipation rate*
Phys. Fluids 27, 1048*
1984. `
..19.0,24.1,54.0: phase portraits*
NEU, J.C.*
The dynamics of a columnar vortex in an imposed strain*
Phys. Fluids 27, 2397*
1984. `
..24.7,19.3:-5/3 not -2 because random sheets interact*
MOFFATT, J.K.*
Simple topological aspects of turbulent vorticity dynamics*
Turbulence and Chaotic Phenomena in Fluids (T. Tatsumi, Ed.) North-Holland, p.223*
1984. `
..19.2,13.0: meas. - rate depends on third invariant, see GENCE*
CHOI, K.S.; LUMLEY, J.L.*
Return to isotropy of homogeneous turbulence revisited*
Turbulence and Chaotic Phenomena in Fluids (T. Tatsumi, Ed.) North-Holland, p.267*
1984. `
..19.2:discussion in II, III plane*
LE PENVEN, L.; GENCE, J.N.; COMTE-BELLOT, G.*
On the approach to isotropy of homogeneous turbulence - effect of the partition of kinetic energy among the velocity components*
Frontiers in Fluid Mechanics (S.H. Davis, J.L. Lumley, Eds.) Springer, p.1*
1984. `
..19.3:society for statistical geometry*
KARWEIT, M.J.*
Random incompressible motion on two and three-dimensional lattices and its application to the walk on a random field*
Frontiers in Fluid Mechanics (S.H. Davis, J.L. Lumley, Eds.) Springer, p.22*
1984. `
..28.3: price 19.95*
SEYER, M.D.*
RS-232 made easy - connecting computers, printers, terminals, and modems*
Prentice-Hall Inc.*
1984. `
..11.2,19.2: just so - works well except in the stable atmospheric boundary layer*
FULACHIER, L.; ANTONIA, R.A.*
Spectral analogy between temperature and velocity fluctuations in several turbulent flows*
Int. J. Heat & Mass Transfer 27, 987*
1984. `
..13.0,19.3: DI for weak shear*
YOSHIZAWA, A.; KIMURA, Y.*
A statistical investigation of the modelling of a mean-shear-related term in the pressure-strain correlation of a turbulent shear flow*
J. Phys. Soc. Japan 53, 2253*
1984. `
..19.0: analytic signal etc - useful review*
SREENIVASAN, K.R. *
On the fine-scale intermittency of turbulence*
J. Fluid Mech. 151, 81*
1985. `
..19.1: -5/3 line in plot of vel. excursion vs. 1/(crossing time)*
BANDYOPADHYAY, P.; HUSSAIN, A.K.M.F.*
The universal nature of zero-crossing time and velocity scales in turbulent shear flows *
AIAA J. 23, 161*
1985. `
..25.6,19.2: small structures align with large scale strain - Rlambda up to 80*
KERR, R.M.*
Higher-order derivative correlations and the alignment of small-scale structures in isotropic numerical turbulence*
J. Fluid Mech. 153, 31*
1985. `
..19.3,25.6: test field model poor at high k*
HERRING, J.R.; McWILLIAMS, J.C.*
Comparison of direct numerical simulation of two-dimensional turbulence with two-point closure - the effects of intermittency*
J. Fluid Mech. 153, 229*
1985. `
..11.3,19.1: pulse-heated mandoline*
BUDWIG, R.; TAVOULARIS, S.; CORRSIN, S.*
Temperature fluctuations and heat flux in grid-generated isotropic turbulence with streamwise and transverse mean-temperature gradients.*
J. Fluid Mech. 153, 441*
1985. `
..25.6,19.3:hairpin vortices*
MOIN, P.; KIM, J.*
The structure of the vorticity field in turbulent channel flow. Part 1. Analysis of instantaneous fields and statistical corrrelations*
J. Fluid Mech. 155, 441*
1985. `
..07.0,19.2: 1/k laws from overlap*
PERRY, A.E.; LIM, K.L.; HENBEST, S.M.*
A spectral analysis of smooth flat-plate boundary layers*
Presented at 5th Symposium on Turbulent Shear Flows, Cornell, p. 9-29 (not in Proc.)*
1985. `
..19.1,11.3,43.1: tidal channel - see JFM 144, 231*
GARGETT, A.E.*
Evolution of scalar spectra with the decay of turbulence in a stratified fluid.*
J. Fluid Mech. 159, 379*
1985. `
..25.6,19.3:uses DI - a bit better than dim. anal.*
YOSHIZAWA, A.; HORIUTI, K.*
A statistically derived subgrid scale kinetic energy model for the large eddy simulation of turbulent flows*
J. Phys. Soc. Japan 54, 2834*
1985. `
..11.3,19.1,14.0: anisotropic eddy diffusivity from DI*
YOSHIZAWA, A.*
Statistical analysis of the anisotropy of scalar diffusion in turbulent shear flows*
Phys. Fluids 28, 3226*
1985. `
..11.3,19.2: pdf transport model*
ANAND, M.S.; POPE, S.B.*
Diffusion behind a line source in grid turbulence*
Turbulent Shear Flows 4 - Karlsruhe (L.J.S. Bradbury et al., Eds.). Springer, p.46*
1985. `
..19.3,28.1: Scripps - see also Landahl book. Vol, p are correct*
ARMI, L.; FLAMENT, P.*
Cautionary remarks on the spectral interpretation of turbulent flows*
J. Geophys. Res. 90C6, 11779*
1985. `
..19.1: review, and experiments with both signs of III*
LE PENVEN, L.; GENCE, J.N.; COMTE-BELLOT, G.*
On the approach to isotropy of homogeneous turbulence - effect of the partition of of kinetic energy among the velocity components*
Frontiers in Fluid Mechanics (S.H. Davis and J.L. Lumley, Eds., Springer), 1*
1985. `
..19.3: review*
HERRING, J.R.*
Some contributions of two-point closure to turbulence*
Frontiers in Fluid Mechanics (S.H. Davis and J.L. Lumley, Eds., Springer), 68*
1985. `
..19.2: strong departures from vel. and temp. at Re, lambda of 160*
ANTONIA, R.A.; ANSELMET, F.; CHAMBERS, A.J.*
Assessment of local isotropy using measurements in a turbulent plane jet*
J. Fluid Mech. 163, 365*
1986. `
..19.2,11.3: larger than iso by 50 to 100 percent*
ANTONIA, R.A.; BROWNE, L.W.B.*
Anisotropy of the temperature dissipation in a turbulent wake*
J. Fluid Mech. 163, 393*
1986. `
..11.3,19.2:lognormal model better than Beta model but neither good*
ANTONIA, R.A.*
Reynolds number dependence of temperature structure functions in turbulent shear flows*
Boundary-Layer Met. 34, 411*
1986. `
..19.3,12.2: yes - Liapunov exponent is positive. Strange attractor because chaotic but dissipative - O(10) modes?*
DEISSLER, R.G.*
Is Navier-Stokes turbulence chaotic?*
Phys. Fluids 29, 1453*
1986. `
..25.1,19.2: detailed ref.*
YAKHOT, V.; ORSZAG, S.A.*
Renormalization group analysis of turbulence - I. Basic theory*
J. Sci. Comp. 1, 1*
1986. `
..01.1,19.1,24.1: Aero Lib has fiche*
FOSS, J.F.; KLEWICKI, C.L.; DISIMILE, P.J.*
Transverse vorticity measurements using an array of four hot-wire probes*
NASA Contractor Report 178098*
1986. `
..25.7,19.2:extension of Kelvin's method - 2 and 3D. Relevant to vortex stretching?*
CRAIK, A.D.D.; CRIMINALE*, W.O.*
Evolution of wavelike disturbances in shear flows - a class of exact solutions of the Navier-Stokes equations*
Proc. Roy. Soc. A406, 13*
1986. `
..19.2: recurrence relations, representing cascade "chain" - useful references to Russian work. See also J. de Mec. 1988*
GLEDZER, E.B.*
Estimate of the constant in "2/3 law" of turbulence obtained by reduction of the hydrodynamic equations*
Soviet Physics JETP vol. 64, pt. 3, p. 483*
1986. `
..14.0,19.4: TSDIA leads to cross-diffusion terms in eps. equation*
YOSHIZAWA, A.*
Statistical modeling of a transport equation for the kinetic energy dissipation rate*
Phys. Fluids 30, 628*
1987. `
..14.0,19.4: DIA theory - see Yosh in sec. 19*
NISIZIMA, S,; YOSHIZAWA, A.*
Turbulent channel and Couette flows using an anisotropic k-e model*
AIAA J. 25, 414*
1987. `
..25.6,19.2: highly anisotropic - horseshoes*
ROGERS, M.M.; MOIN, P.*
The structure of the vorticity field in homogeneous turbulent flows*
J. Fluid Mech. 176, 33*
1987. `
..11.2,19.3: highly anisotropic*
KRISHNAMOORTHY, L.V.; ANTONIA, R.A.*
Temperature-dissipation measurements in a turbulent boundary layer*
J. Fluid Mech. 176, 265*
1987. `
..25.6,19.3: vorticity tends to point in the middle strain direction*
ASHURST, W.T.; KERSTEIN, A.R.; KERR, R.M.; GIBSON, C.H.*
Alignment of vorticity and scalar gradient with strain rate in simulated Navier-Stokes turbulence*
To appear in Phys. Fluids*
1987. `
..19.1: statistics of h.f. envelope*
ANTONIA, R.A.; BRITZ, D.H.; SHAH, D.A.; CHAMBERS, A.J.*
On the fine scale intermittency of turbulence*
Expts. in Fluids 5, 282*
1987. `
..20.0,19.2: strongly aniso.*
BROWNE, L.W.B.; ANTONIA, R.A.; SHAH, D.A.*
Turbulent energy dissipation in a wake*
J. Fluid Mech. 179, 307*
1987. `
..19.3: consequence of an inverse cube fit to f(r)*
ROSEN, G.*
Transformation invariance of the longitudinal velocity correlation in a grid-generated turbulence at high Reynolds numbers*
J. Fluid Mech. 180, 87*
1987. `
..19.1,50.0: review and new expts - parametric study including parallel grids*
ROACH, P.E.*
The generation of nearly isotropic turbulence by means of grids*
Int. J. Heat and Fluid Flow 8, 82*
1987. `
..19.1,54.0: helicity flatness factors large and anisotropic*
KIT, E.; TSINOBER, A.; BALINT, J.L.; WALLACE, J.M.; LEVICH, E.*
An experimental study of helicity related properties of a turbulent flow past a grid*
Phys. Fluids 30, 3323*
1987. `
..20.0,19.2: iso only at high k - Re, lambda from 40 to 80*
ANTONIA, R.A.; SHAH, D.A.; BROWNE, L.W.B.*
Spectra of velocity derivatives in a turbulent wake*
Phys. Fluids 30, 3455*
1987. `
..05.0,19.2: l/k law not really universal*
TURAN, O.; AZAD, R.S.; KASSAB, S.Z.*
Experimental and theoretical evaluation of the k-1 spectral law*
Phys. Fluids 30, 3463*
1987. `
..19.3: triad interactions - local ones fundamentally different*
BRASSEUR, J.G.; CORRSIN, S.*
Spectral evolution of the Navier-Stokes equations for low order couplings of Fourier modes*
Advances in Turbulence (G. Comte-Bellot and J. Mathieu, Eds.), Springer, p. 152*
1987. `
..12.1,13.0,19.3: k-space theory*
BERTOGLIO, J.P.; SQUIRES, K.; FERZIGER, J.H.*
EDQNM closure; A homogeneous simulation to support it. A quasi homogeneous simulation to disprove it*
Studying turbulence using numerical simulation databases, Ames/Stanford CTR-S87, p. 53*
1987. `
..19.2,25.6: transport eqn for pdf - vorticity and p.g. uncorrelated*
MORTAZAVI, M.; KOLLMANN, W.; SQUIRES, K.*
A statistical investigation of the single-point pdf of velocity and vorticity based on direct numerical simulations*
Studying turbulence using numerical simulation databases, Ames/Stanford CTR-S87, p. 147*
1987. `
..54.0,19.3: remains nearly isotropic*
SPEZIALE, C.G.; MANSOUR, N.N.; ROGALLO, R.S.*
The decay of isotropic turbulence in a rapidly rotating frame*
Studying turbulence using numerical simulation databases, Ames/Stanford CTR-S87, p. 205*
1987. `
..12.2,19.3: RNG following Yakhov*
RUBINSTEIN, R.; BARTON, J.M.*
Infrared properties of an anisotropically stirred fluid*
Phys. Fluids 30, 2987*
1987. `
..19.3: special case of weighted curdling*
MENEVEAU, C.; SREENIVASAN, K.R.*
Simple multifractal cascade model for fully developed turbulence*
Phys. Rev. Letters 59, 1424*
1987. `
..19.3: Beltrami flows not important in dissipation regions -- which are sheets*
KERR, R.M.*
Histograms of helicity and strain in numerical turbulence*
Phys. Rev. Letter 59, 783*
1987. `
..20.0,19.2: microscale Re only 40 to 80 but close to isotropy*
ANTONIA, R.A.; BROWNE, L.W.B.; SHAH, D.A.*
Characteristics of vorticity fluctuations in a turbulent wake*
J. Fluid Mech. 189, 349*
1988. `
..19.2,25.6: triad non-local, transfer local - see CTR-S88*
DOMARADSKI, J.A.*
Analysis of energy transfer in direct numerical simulations of isotropic turbulence*
Phys. Fluids 31, 2747*
1988. `
..19.3: weak vortex patch, spiralled by strong vortex, has -11/3 spectrum*
GILBERT, A.D.*
Spiral structures and spectra in two-dimensional turbulence*
J. Fluid Mech. 193, 475*
1988. `
..11.1,19.1:  statistics from DIA*
YOSHIZAWA, A.*
Statistical modelling of passive-scalar diffusion in turbulent shear flows*
J. Fluid Mech. 195, 541*
1988. `
..19.3: not the usual spectrum-relation between dimension and scaling exponent*
DEANE, A.E.; KEEFE, L.R.*
Multifractal spectra in homogeneous shear flow*
Studying turbulence using numerical simulation data bases - II, Ames/Stanford CTR-S88, p. 157*
1988. `
..19.2: USC work -- triad interaction is non-local but energy transfer is local.  Are Fourier modes a good description?*
DOMARADZKI, J.A.; ROGALLO, R.S.*
Energy transfer in isotropic turbulence at low Reynolds numbers*
Studying turbulence using numerical simulation data bases - II, Ames/Stanford CTR-S88, p. 169*
1988. `
..19.3,32.1: twinkle, twinkle*
TRUMAN, C.R.; LEE, M.J.*
Optical propagation through a homogeneous turbulent shear flow*
Studying turbulence using numerical simulation data bases - II, Ames/Stanford CTR-S88, p. 311*
1988. `
..19.3: fractal statictics of dissipation at high Re - dimension 2.87*
SREENIVASAN, K.R.; MENEVEAU, C.*
Singularities of the equations of fluid motion*
Phys. Rev. A 38, 6287*
1988. `
..19.3,11.1: intermittency exponent mu higher than for energy dissipation*
PRASAD, R.R.; MENEVEAU, C.; SREENIVASAN, K.R.*
Multifractal nature of the dissipation field of passive scalars in fully turbulent flows*
Phys. Rev. Letters 61, 74*
1988. `
..01.1,19.3: high-freq. intermittency collapses on Kolmogorov scales*
BRITZ, D.; SHAH, D.A.; ANTONIA, R.A.*
The fine-scale intermittency of turbulence*
Phys. Fluids 31, 1431*
1988. `
..19.3: analogy between temperature and energy dissipation*
ANTONIA, R.A.; SHAH, D.A.; BROWNE, L.W.B.*
Dissipation and vorticity spectra in a turbulent wake*
Phys. Fluids 31, 1805*
1988. `
..11.1,25.6,19.3: -17/3 power*
CHASNOV, J.; CANUTO, V.M.; ROGALLO, R.S.*
Turbulence spectrum of a passive temperature field - results of a numerical simulation*
Phys. Fluids 31, 2065*
1988. `
..19.3: slight tendency to Beltramization*
KRAICHNAN, R.H.; PANDA, R.*
Depression of nonlinearity in decaying isotropic turbulence*
Phys. Fluids 31, 2395*
1988. `
..19.3,25.6: K-L expansion uses orthogonal functions and random coefficients*
CHAMBERS, D.H.; ADRIAN, R.J.; MOIN, P.; STEWART, D.S.; SUNG, H.J.*
Karhunen-Loeve expansion of Burgers' model of turbulence*
Phys. Fluids 31, 2573*
1988. `
..19.3,12.2: Burgers not chaotic - new simulation system proposed, with dimension 20*
QIAN, J.*
Cascade model of turbulence*
Phys. Fluids 31, 2865*
1988. `
..19.1:  array of propellers - strong discrete frequencies so doesn't count as turbulence*
MICHARD, M.*
Study of mechanisms related to organized large structures in grid turbulence*
Ph.D. Thesis, Ecole Centrale de Lyon*
1988. `
..12.2,19.3,11.6: internal scalar interfaces - dim. 2.35 for high (? all) Sc.*
SREENIVASAN, K.R.; PRASAD, R.R.; MENEVEAU, C.; RAMSHANKAR, R.*
The fractal geometry of interfaces and the multifractal distribution of dissipation in fully turbulent flows*
To appear in J. Pure & Appl. Geophys.*
1989. `
..19.3: practical dimension of interfaces is about 7/3*
SREENIVASAN, K.R.; RAMSHANKAR, R.; MENEVEAU, C.*
Mixing, entrainment and fractal dimensions of surfaces in turbulent flows*
Proc. Roy. Soc. Lond. A421, 79*
1989. `
..12.2,19.1: RDT calcs for small-scale motion (!) and order of magnitude discussion of return to isotropy*
KIDA, S.; HUNT, J.C.R.*
Interaction between different scales of turbulence over short times*
J. Fluid Mech. 201, 411*
1989. `
..12.2,19.3:excellent review of chaos, Poincare sections and all - plus low-Re spectral theory*
DEISSLER, R.G.*
On the nature of Navier-Stokes turbulence*
NASA TM 101983 and PhD Thesis, Case W.R. Univ.*
1989. `
..11.1,19.2: 1/k temperature spectrum*
LESIEUR, M.; ROGALLO, R.*
Large-eddy simulation of passive scalar diffusion in isotropic turbulence*
Phys. Fluids A1, 718*
1989. `
..11.1,19.2: return to isotropy - decay larger than in iso. turb. (Warhaft 1980)*
NAKAUCHI, N.; OSHIMA, H.; SAITO, Y.*
A passive scalar convected by homogeneous axisymmetric turbulence*
Phys. Fluids A1, 723*
1989. `
..11.1,19.2: depends on ratio of integral length scales for velocity and scalar*
KOSALY, G.*
Scalar mixing in isotropic turbulence*
Phys. Fluids A1, 758*
1989. `
..19.3: rigorous estimates of increase*
ETEMADI, N.*
On curve and surface stretching in turbulent flow*
Ames/Stanford CTR Annual Research Briefs, 1988, p. 19*
1989. `
..54.0,19.3: reconnection*
MELANDER, M.V.*
Close interactions of 3d-vortex tubes*
Ames/Stanford CTR Annual Research Briefs, 1988, p. 39*
1989. `
..19.1: linear extrapolation to zero wire length - essentially unjustifiable*
AZAD, R.S.; KASSAB, S.Z.*
New method of obtaining dissipation*
Expts. in Fluids 7, 81*
1989. `
..19.1,54.0: EDQNM - refers to experiment at ONERA*
CAMBON, C.; JACQUIN, L.*
Spectral approach to non-isotropic turbulence subjected to rotation*
J. Fluid Mech. 202, 295*
1989. `
..11.3,19.3: cross-correlation coefficient can take either sign*
KAPLAN, H.; DINAR, N.*
The interference of two passive scalars in a homogeneous isotropic turbulent field*
J. Fluid Mech. 203, 273*
1989. `
..12.2,19.3: weak effect of shear parameter*
KEEFE, L.R.; DEANE, A.E.*
Multifractal spectra in shear flows*
7th Sympo. on Turbulent Shear Flows, Stanford Univ.*
1989. `
..11.1,19.2: measurements to prove it*
DAHM, W.J.A.; BUCH, K.A.*
Lognormality of the scalar dissipation pdf in turbulent flows*
Phys. Fluids A1, 1290*
1989. `
..25.6,19.4: Smago constant affected by Kraichnan-like Lagrangian effects*
YOSHIZAWA, A.*
Subgrid-scale modeling with a variable length scale*
Phys. Fluids A1, 1293*
1989. `
..19.2,11.3,20.0: i.e. squares of fluctuating gradients*
ANTONIA, R.A.; BROWNE, L.W.B.; SHAH, D.A.*
Instantaneous dissipations of turbulent energy and temperature in a wake*
Phys. Fluids A1, 1374*
1989. `
..24.1,50.0,19.2: large-scale intermittency*
VEERAVALLI, S.; WARHAFT, Z.*
The shearless turbulent mixing layer*
J. Fluid Mech. 207, 191*
1989. `
..11.6,19.3: pdfs are non-stationary, contradicting Batchelor 1952*
GIRIMAJI, S.S.; POPE, S.B.*
Material element deformation in isotropic turbulence*
Cornell Univ. FDA-89-14*
1989. `
..19.4: (Local-Energy-Transfer) - suggests that failure of DIA is failure to renormalize stirring forces*
McCOMB, W.D.; SHANMUGASUNDARAM, V.; HUTCHINSON, P.*
Velocity-derivative skewness and two-time velocity correlations of isotropic turbulence as predicted by the LET theory*
J. Fluid Mech. 208, 91*
1989. `
..11.1,19.3: interface mixing - get "inertial range" scaling at quite low Re in 2D cases*
VIECELLI, J.A.*
Structure of Lagrangian turbulence*
Phys. Fluids A1, 1836*
1989. `
..19.4: Kraichnan 4th author. DIA fails to capture vorticity spottiness a.k.a. high-k intermittency*
CHEN, H.; ET AL.*
Non-Gaussian statistics in isotropic turbulence*
Phys. Fluids A1, 1844*
1989. `
..11.1,19.3: published*
POPE, S.B.; YEUNG, P.K.; GIRIMAJI, S.S.*
The curvature of material surfaces in isotropic turbulence*
Phys. Fluids A1, 2010*
1989. `
..19.3: Tennekes assumed statistical independence of inertial-range and energy-range excitation - RNG contradicts this and is wrong*
CHEN, S.; KRAICHNAN, R.H.*
Sweeping decorrelation in isotropic turbulence*
Phys. Fluids A1, 2019*
1989. `
..54.0,19.3: large initial helicity in simulations reduces energy transfer*
POLIFKE, W.; SHTILMAN, L.*
The dynamics of helical decaying turbulence*
Phys. Fluids A1, 2025*
1989. `
..11.6,19.3: mapping closure -- time dependent nonlinear mapping of multivariate Gaussian to reproduce actual pdf which can be wildly non-Gaussian*
CHEN, H.; CHEN, S.; KRAICHNAN, R.H.*
Probability distribution of a stochistically advected scalar field*
Phys. Rev. Letters 63, 2657*
1989. `
..54.0,19.1:  Veeravalli-like.  Microscale Re=40* 
JACQUIN, L.; LEUCHTER, O.; GEFFROY, P.*
Experimental study of homogeneous turbulence in the presence of rotation*
Turbulent Shear Flows 6, (J.C. Andre et al., eds.), Springer, p. 46*
1989. `
..19.3: shot-noise model*
VEERAVALLI, S.V.; VEERAVALLI, V.V.*
Higher-order spectra of turbulent velocity fluctuations*
Submitted to Phys. Fluids A (unpublished?)*
1990. `
..19.1,11.1: timescale ratio determined by initial spectrum -- permanence of large eddies*
LEWALLE, J.*
Decay of velocity and temperature fluctuations in grid turbulence*
AIAA J. 28, 106*
1990. `
..19.2,12.1,54.0: nine-sensor probe*
BALINT, J.L.; VUKOSLAVCEVIC, P.; WALLACE, J.M.*
The transport of enstrophy in a turbulent boundary layer*
Near-wall Turbulence - 1988 Zaric Memorial Conf. (S.J. Kline and N.H. Afgan, eds.), Hemisphere, p. 932*
1990. `
..19.2,20.0: Re, lambda up to 25 - unsurprisingly, no inertial subrange. SV has.*
THORODDSEN, S.T.; VAN ATTA, C.W.*
Experiments on small-scale anisotropy and dissipation in stably stratified turbulence*
UCSD paper for Phys. Fluids - unpub.? but see JFM 322, 383 (1996)*
1990. `
..19.2: sweeping is Lagrangian, wrongly contradicted by RNG*
NELKIN, M.; TABOR, M.*
Time correlations and random sweeping in isotropic turbulence*
Phys.  Fluids A2, 81*
1990. `
..19.2,25.6: all the fault of Fourier or low-Re simulation? - see Meneveau, 1990, on wavelets*
DOMARADZKI, J.A.: ROGALLO, R.S.*
Local energy transfer and nonlocal interactions in homogeneous isotropic turbulence*
Phys. Fluids A2, 413*
1990. `
..19.2,12.2: potential part of omega x u much large than solenoidal part - not quite saying that p. gradient dominates?*
TSINOBER, A.*
On one property of Lamb vector in isotropic turbulent flow*
Phys. Fluids A2, 484*
1990. `
..19.3: intermittency of dissipation*
NOVIKOV, E.A.*
The effects of intermittency on statistical characteristics of turbulence and scale similarity of breakdown coefficients*
Phys. Fluids A2, 814*
1990. `
..19.3: high-k structure is probably a pair of oppositely-oriented vortex sheets*
NAKANO, T.*
A microscopic vortical structure in fully developed turbulence*
Phys. Fluids A2, 829*
1990. `
..19.2,12.2: fractal properties evaluated from 128^3 simulation*
HOSOKAWA, I.; YAMAMOTO, K.*
Intermittency exponents and generalized dimensions of a directly simulated fully developed turbulence*
Phys.  Fluids A2, 889*
1990. `
..25.6,19.2: comment on Lesieur and Rogallo closure with "hyperviscosity" -- k-dependent viscosity*
HERRING, J.R.*
Comparison of closure to spectral-based large eddy simulations*
Phys.  Fluids A2, 979*
1990. `
..19.2,54.0: mathematical -- real, non-Gaussian, non-linear turbulence is not time-reversal invariant*
DRUMMOND, I.T.; MUNCH, W.*
Turbulent stretching of line and surface elements*
J. Fluid Mech. 215, 45*
1990. `
..19.2: derivatives in x too large at Re, lambda up to 2800 in wind tunnel*
KUZNETSOV, V.R.; KARYAKIN, M.Y.; PRASKOVSKY, A.A.*
Anisotropy of turbulence fine-scale structure in high Reynolds number flows*
Presented at 3rd European Turbulence Conference, Stockholm*
1990. `
..11.1,19.2: very high Pr theory, similar to DIA - see Phys. Fluids 1985, p. 1299*
QIAN, J.*
The spectrum of a turbulent passive scalar in the viscous-convective range*
J. Fluid Mech. 217, 203*
1990. `
..18.1,19.3:just so*
LEE, S.; LELE, S.K.; MOIN, P.*
Eddy-shocklets in decaying compressible turbulence*
CTR Manuscript 117*
1990. `
..19.3: slope less than - 5/3 - modification of Gurvich and Yaglom 1967, using beta distribution*
YAMAZAKI, H.*
Breakage models - lognormality and intermittency*
J. Fluid Mech. 219, 181*
1990. `
..19.1: -1 . 300 -  literature review*
MOHAMED, M.S.; LaRUE, J.C.*
The decay power law in grid-generated turbulence*
J. Fluid Mech. 219, 195*
1990. `
..19.1: 450 x 450 mesh - automated vortex census*
McWILLIAMS, J.C.*
The vortices of two-dimensional turbulence*
J. Fluid Mech. 219, 361*
1990. `
..19.1: - see previous*
McWILLIAMS, J.C.*
The vortices of geostrophic turbulence*
J. Fluid Mech. 219, 387*
1990. `
..54.0,19.1: 30 cm, 20 m/s, 800 rpm see also TSF 6*
JACQUIN, L.; LEUCHTER, O.; CAMBON, C.; MATHIEU, J.*
Homogeneous turbulence in the presence of rotation*
J. Fluid Mech. 220, 1*
1990. `
..24.1,18.1,19.2: possibly first reference to oblique disturbances at M_c=0.8 - but no direct relation to the "pasta problem" of high-k geometry*
CHEN, J.H.; ET AL.*
A study of the topology of dissipating motions in direct numerical simulations of time-developing compressible and incompressible mixing layers*
Studying Turbulence Using Numerical Simulation Databases III (NASA Ames/Stanford Center for Turbulence Research), p. 139*
1990. `
..11.2,19.2: Batchelor scaling works at low Re - at high Re the small-scale strain rate is irrelevant*
GIBSON, C.; ROGERS, M.; CHASNOV, J.; PETRESKY, J.*
Numerical simulation of low Prandtl number turbulent mixing*
Studying Turbulence Using Numerical Simulation Databases III (NASA Ames/Stanford Center for Turbulence Research), p. 211*
1990. `
..19.2: highly intermittent local transfer resulting from non-local interaction*
DOMARADZKI, J.A.; ROGALLO, R.S.; WRAY, A.A.*
Interscale energy transfer in numerically simulated homogeneous turbulence*
Studying Turbulence Using Numerical Simulation Databases III (NASA Ames/Stanford Center for Turbulence Research), p. 319*
1990. `
..19.2,02.1,28.1: defines a scale-dependent high frequency intermittency and a spatially-local Reynolds number*
FARGE, M.; GUEZENNEC, Y.; HO. C.M.; MENEVEAU, C.*
Continuous wavelet analysis of coherent structures*
Studying Turbulence Using Numerical Simulation Databases III (NASA Ames/Stanford Center for Turbulence Research), p. 331*
1990. `
..11.1,19.2:  alternative to lognormal, for vel. or temp.*
ANDREWS, L.C.; SHIVAMOGGI, B.K.*
The gamma distribution as a model for temperature dissipation in intermittent turbulence*
Phys. Fluids A2, 105*
1990. `
..19.2,53.0:  decay rate decreases as a result of production*
JOHNSON, P.L.; JOHNSTON, J.P.*
The effect of streamline curvature on decaying grid turbulence*
Twelfth Symposium on Turbulence, Rolla*
1990. `
..19.2: not clear that anisotropy is finite at infinite wave number*
BRASSEUR, J.G.*
Comments on the Kolmogorov hypothesis of isotropy in the small scales*
AIAA-91-0230*
1991. `
..19.2,12.2:  just so*
MENEVEAU, C.; SREENIVASAN, K.R.*
The multifractal nature of turbulent energy dissipation*
J. Fluid Mech. 224, 429*
1991. `
..19.2,25.6:  240 cubed simulation at Re, lambda = 150 - elongated tubes of vorticity, strongly non-Gaussian*
VINCENT, A.; MENEGUZZI, M.*
The spatial structure and statistical properties of homogeneous turbulence*
J. Fluid Mech. 225, 1*
1991. `
..11.6,19.2:  analysis and simplified simulation - refers to Pope*
DRUMMOND, I.T.; MUNCH, W.*
Distortion of line and surface elements in model turbulent flows*
J. Fluid Mech. 225, 529*
1991. `
..12.1,19.1:  EDQNM and RDT*
CAMBON, C.*
Single and double point modeling of homogeneous turbulence*
Ames/Stanford Center for Turbulence Research, Annual Research Briefs - 1990, p. 23*
1991. `
..54.0,19.3:  cascade process weakened*
VEERAVALLI, S.V.*
An experimental study of the effects of rapid rotation on turbulence*
Ames/Stanford Center for Turbulence Research, Annual Research Briefs - 1990, p. 203*
1991. `
..19.3,28.1:  just so*
MENEVEAU, C.*
Dual spectra and mixed energy cascade of turbulence in the wavelet representation*
Ames/Stanford Center for Turbulence Research, Annual Research Briefs - 1990, p. 263*
1991. `
..19.3:  odd definition of "invariance" if integral of v dot omega is invariant*
POLIFKE, W.*
Statistics of helicity fluctuations in homogeneous turbulence*
Phys. Fluids A3, 115*
1991. `
..19.2:  very sensitive to buoyancy - explains previous anisotropy by deviations at low end of derivative spectrum*
VAN ATTA, C.*
Local isotropy of the smallest scales of turbulent scalar and velocity fields*
Proc. Roy. Soc. A434, 139*
1991. `
..19.3:  Azad technique no good*
BROWNE, L.W.B.; ZHU, Y.; ANTONIA, R.A.*
Dissipation estimates in turbulent flows using the zero-wire-length technique*
Expts. in Fluids 11, 197*
1991. `
..19.3:  anisotropic forcing by vortex array - Re, lambda = 32*
YEUNG, P.K.; BRASSEUR, J.G.*
The response of isotropic turbulence to isotropic and anisotropic forcing at the large scales*
Phys. Fluids A3, 884*
1991. `
..13.0,18.1,19.3:  model with dilatation dissipation and pressure dilatation*
ZEMAN, O.*
On the decay of compressible isotropic turbulence*
Phys. Fluids A3, 951*
1991. `
..19.2:  Gaussian, not exponential, cutoff of -5/3 spectrum gives best S*
SMITH, L.M.; REYNOLDS, W.C.*
The dissipation-range spectrum and the velocity-derivative skewness in turbulent flows*
Phys. Fluids A3, 992*
1991. `
..19.2,11.1:  LES for small Pr - temperature field fully resolved*
CHASNOV, J.R.*
Simulation of the inertial-conductive subrange*
Phys. Fluids A3, 1164*
1991. `
..19.2:  96 cubed points and Re, lambda=60 show tubelike (rod-like) regions of high enstrophy*
RUETSCH, G.R.; MAXEY, M.R.*
Small-scale features of vorticity and passive scalar fields in homogeneous isotropic turbulence*
Phys. Fluids A3, 1587*
1991. `
..19.2:  interaction over large k range does not imply energy exchange, but structure/anisotropy is modulated*
BRASSEUR, J.G.; YEUNG, P.K.*
Large and small-scale coupling in homogeneous turbulence - analysis of the Navier-Stokes equation in asymptotic limit*
Presented at 8th Symposium on Turbulent Shear Flows, Munich, paper no. 16-4*
1991. `
..05.0,19.2,31.1:  9-wire probe - resolution 6 eta at Re, theta of 2700.  Part I (HWA) on p. 25*
VUKOSLAVCEVIC, P.; WALLACE, J.M.; BALINT, J.-L.*
The velocity and vorticity vector fields of a turbulent boundary layer.  Part 2.  Statistical properties*
J. Fluid Mech. 228, 53 *
1991. `
..25.6,19.2:  rotation*
MALTRUD, M.E.; VALLIS, G.K.*
Energy spectra and coherent structures in forced two-dimensional and beta-plane turbulence*
J. Fluid Mech. 228, 321*
1991. `
..19.2,31.1:  12-wire probe.  Re, lambda up to 90*
TSINOBER, A.; KIT, E.; DRACOS, T.*
Measuring invariant (frame independent) quantities composed of velocity derivatives in turbulent flows*
Advances in Turbulence 3, (A.V. Johansson and P.H. Alfredsson, eds.), Springer*
1991. `
..18.1,19.1:  Rept. TF 50 - rms Mach no. up to 0.4.  Blames dilatational dissipation on pressure dilatation correlation*
BLAISDELL, G.A.; REYNOLDS, W.C.; MANSOUR, N.N.*
Compressibility effects on the growth and structure of homogeneous turbulent shear flow*
Presented at 8th Symposium on Turbulent Shear Flows, Munich, paper no. 1-1*
1991. `
..19.3:  simulation (e.g. Rogers and Moser mixing layer)  at low Re - relatively simple relations between II and III implying simple relation between double and triple products*
SONDERGAARD, R.; CHEN, J.; SORIA, J.; CANTWELL, B.*
Local topology of small scale motions in turbulent shear flows*
Presented at 8th Symposium on Turbulent Shear Flows, Munich, paper no. 16-1*
1991. `
..19.2,02.1:  2 page synopsis - typescript seems to misprint 1/9 for 1/3. PB has full paper*
KUZNETSOV, V.R.; PRASKOVSKY, A.A.; SABELNIKOV, V.A.*
Intermittency and fine-scale turbulence structure in shear flows*
Presented at 8th Symposium on Turbulent Shear Flows, Munich, paper no. I-8*
1991. `
..19.2,12.1,21.3:  Taylor's hypothesis not good for large strain rates*
RAHAI, H.R.; LaRUE, J.C.*
A comparison of temporal and spatial temperature derivatives in a strained turbulent flow*
Presented at 8th Symposium on Turbulent Shear Flows, Munich, poster no. I-16*
1991. `
..19.2:  multifractal spectra - denies Kolmogorov.  Just dimensional analysis*
CASTAING, B.; GAGNE, Y.; HOPFINGER, E.H.*
A new view of fully developed turbulence*
Submitted to Phys. Fluids (unpublished?)*
1991. `
..19.2:  just dimensional analysis - see Proc. Roy. Soc. A434, 89 (1991)*
FRISCH, U.; VERGASSOLA, M.*
A prediction of the multifractal model - the intermediate dissipation range*
Europhys. Lett. 14, 439*
1991. `
..19.2,12.1:  logico-deductive*
FRISCH, U.*
From global scaling, a la Kolmogorov, to local multifractal scaling in fully developed turbulence*
Proc. Roy. Soc. A434, 89*
1991. `
..19.2,25.5:  seems to follow Re^1.4 as in Tavoularis JFM 1978*
DEISSLER, R.G.*
Numerical solution for the velocity-derivative skewness of a low Reynolds-number turbulent-like decaying Navier-Stokes flow*
Computers and Fluids 20, 89*
1991. `
..13.0,19.1:  Re-dependent addition to c, eps2 has large effect - not well justified*
BERNARD, P.S.; THANGAM, S.; SPEZIALE, C.G.*
The role of vortex stretching in turbulence modeling*
Proc. ICASE/NASA Langley Summer Program*
1991. `
..19.2,02.1:  short version of 1/3 power law for gamma*
PRASKOVSKY, A.A.*
Local structure of turbulence in flows with large Reynolds numbers*
Chaos 1, 237*
1991. `
..19.2: second best to local isotropy - jets and wakes apparently axi. about x axis.  See Antonia, p. 369*
GEORGE, W.K.; HUSSEIN, H.J.*
Locally axisymmetric turbulence*
J. Fluid Mech. 233, 1*
1991. `
..11.6,19.1: in grid turbulence - pasive NO-ozone reaction*
BILGER, R.W.; SAETRAN, L.R.; KRISHNAMOORTHY, L.V.*
Reaction in a scalar mixing layer*
J. Fluid Mech. 233, 211*
1991. `
..19.2,25.6: simulation data - "chooses" x as the direction for axisymmetry.  See George, p. 1.*
ANTONIA, R.A.; KIM, J.; BROWNE, L.W.B.*
Some characteristics of small-scale turbulence in a turbulent duct flow*
J. Fluid Mech. 233, 369*
1991. `
..19.2,14.0:  reprint of Proc. Roy. Soc. A434 - see individual refs. to vol. A434*
HUNT, J.C.R.; PHILLIPS, O.M.; WILLIAMS, D. (eds.)*
Turbulence and Stochastic Processes - Kolmogorov's Ideas 50 Years On*
Royal Society, London*
1991. `
..12.2,19.3:  gives upper and (incomprehensible) lower bound for turbulence attraction*
TEMAN, R.*
Approximation of attractors, large eddy simulations and multiscale methods*
Proc. Roy. Soc. London A434, 23*
1991. `
..19.3,19.4:  renormalized perturbation theory - inc. DIA and ALHDIA - not promising.  Mapping closure may help*
KRAICHNAN, R.H.*
Turbulent cascade and intermittency growth*
Proc. Roy. Soc. London A434, 65*
1991. `
..19.3:  rare organized events are responsible for high-k intermittency - good general discussion of vorticity, etc.*
SHE, Z.S.; JACKSON, E.; ORSZAG, S.A.*
Structure and dynamics of homogeneous turbulence - models and simulations*
Proc. Roy. Soc. London A434, 101*
1991. `
..19.3,42.1,11.1:  just so*
PHILLIPS, O.M.*
The Kolmogorov spectrum and its oceanic cousins  - a review*
Proc. Roy. Soc. London A434, 125*
1991. `
..19.3,42.1,11.1:  just so - wide-ranging review*
GIBSON, C.H.*
Kolmogorov similarity hypotheses for scalar fields -  sampling intermittent turbulent mixing in the ocean and galaxy*
Proc. Roy. Soc. London A434, 149*
1991. `
..19.2,11.1:  local isotropy even more dubious for concentration than for velocity*
SREENIVASAN, K.R.*
On local isotropy of passive scalars in turbulent shear flows*
Proc. Roy. Soc. London A434, 165*
1991. `
..19.3,12.2:  including box counting for dimensions of spirals*
HUNT, J.C.R.; VASSILICOS, J.C.*
Kolmogorov's contributions to the physical and geometrical understanding of small-scale turbulence and recent developments*
Proc. Roy. Soc. London A434, 183*
1991. `
..11.6,19.2:  wrinkling and stretching*
BRAY, K.N.C.; CANT, R.S.*
Some applications of Kolmogorov's turbulence research in the field of combustion*
Proc. Roy. Soc. London A434, 217*
1991. `
..19.2,30.1:  just so - apparently w spectrum in inertial subrange follows isotropic 4/3 rule but v does not*
VEERAVALLI, S.V.; SADDOUGHI, S.G.*
A preliminary experimental investigation of local isotropy in high-Reynolds-number turbulence*
Stanford/Ames Center for Turbulence Research, Annual Research Briefs, p. 3*
1991. `
..54.0,19.2:  instability principle for spectral transfer - transfers in rotating flow are to wavenumbers perpendicular to the axis*
WALEFFE, F.*
Non-linear interactions in homogeneous turbulence with and without background rotation*
Stanford/Ames Center for Turbulence Research, Annual Research Briefs, p. 31*
1991. `
..19.2:  pasta problem - vortex tubes with core diameter appropriate to an equilibrium Burgers vortex.  "Intermediate eigenvector" of strain is obviously along vortex axis*
JIMENEZ, J.*
On small scale vortices in turbulent flows*
Stanford/Ames Center for Turbulence Research, Annual Research Briefs, p. 45*
1991. `
..19.2:  says T(k,p,q) not appropriate for discussing locality*
ZHOU, Y.*
Scaling analysis of energy transfer in the inertial range*
Stanford/Ames Center for Turbulence Research, Annual Research Briefs, p. 57*
1991. `
..19.2:  complementary to Jimenez p. 45*
DRESSELHAUS, E.*
Turbulence and vortex structures*
Stanford/Ames Center for Turbulence Research, Annual Research Briefs, p. 85*
1991. `
..19.2,62.0:  LDA meas in air with standard TSI tracker, including spectra.  Kolmogorov mu averages 0.38.  No discussion of bulk intermittency*
CATALANO, G.D.; MATHIS, J.A.; CHANG, K.S.*
Higher-order statistics of a turbulent jet in a confined crossflow*
AIAA J. 29, 2124*
1991. `
..19.5,12.2:  more rapid convergence than Fourier for instantaneous Burgers solutions - but still need many terms*
PARK, S.B.; SUNG, H.J.; CHUNG, M.K.; ADRIAN, R.J.*
Convergence of Galerkin solutions using Karhunen-Loeve expansion of inhomogeneous 1-D turbulence*
Phys. Fluids A3, 1695*
1991. `
..12.2,19.2,25.6:  Fourier decomposition with up to 836 modes - seems to be grossly inadequate since subrange constant is orders of magnitude out*
EGGERS, J.; GROSSMANN, S.*
Does deterministic chaos imply intermittency in fully developed turbulence?*
Phys. Fluids A3, 1958*
1991. `
..11.2,19.2:  from time deriv. of conc. - instantaneous peaks significant, not dominant, and non-Poisson.  Could still be log-normal.  Re up to 40000*
DOWLING, D.R.*
The estimated scalar dissipation rate in gas-phase turbulent jets*
Phys. Fluids A3, 2229*
1991. `
..54.0,19.3,12.2:  RDT shows damped oscillation of anisotropy*
MANSOUR, N.N.; SHIH, T.-H.; REYNOLDS, W.C.*
The effects of rotation on initially anisotropic homogeneous flows*
Phys. Fluids A3, 2421*
1991. `
..11.1,19.2:  shows that scalar pdf relaxes to Gaussian only for small scalar variance*
GAO, F.*
Mapping closure and non-Gaussianity of the scalar probability density functions in isotropic turbulence*
Phys. Fluids A3, 2439*
1991. `
..54.0,19.3:  each vortex of a contra-rotating pair develops a tadpole-like cross-section*
KIDA, S.; TAKAOKA, M.; HUSSAIN, F.*
Formation of head-tail structure in a two-dimensional uniform straining flow*
Phys. Fluids A3, 2688*
1991. `
..19.2:  Kolmogorov scaling inconsistent with Lagrangian statistics - must assume inertial-range fluctuations are isotropic in space-time*
VIECELLI, J.A.*
Lagrangian turbulence and the Brownian motion paradox*
Phys. Fluids A3, 2698*
1991. `
..19.3,02.1: internal intermittency - defines events by multiple peaks in (3D) plots of concentration (say)*
BRASSEUR, J.G.; LIN, W.-Q.*
Structure and statistics of intermittency in homogeneous turbulent shear flow*
Advances in Turbulence 3 (A.V. Johansson, P.H. Alfredsson, Eds.), Springer, p. 3*
1991. `
..19.2: local isotropy never a systematic approximation - but far too optimistic in analysis of dissipation transport equation*
DURBIN, P.A.; SPEZIALE, C.G.*
Local anisotropy in strained turbulence at high Reynolds number*
J. Fluids Engg 113, 707*
1991. `
..19.2,31.1: TsAGI/CAHI 14x24m tunnel - measured anisotropy rises at high k. Discussion of x-probe errors*
KUZNETSOV, V.R.; PRASKOVSKY, A.A.; KARYAKIN, M.Y.*
An experimental investigation of local isotropy in high Reynolds number laboratory turbulent flows*
Submitted to Phys. Fluids A (unpublished?)*
1992. `
..19.3:  2D turbulence relaxes to maximum-entropy configurations*
MONTGOMERY, D.; MATTHAEUS, W.H.; STRIBLING, W.T.; MARTINEZ, D.; OUGHTON, S.*
Relaxation in two dimensions and the "sinh-Poisson" equation*
Phys. Fluids A4, 3*
1992. `
..19.3,19.4:  Kraichnan's measure of nonlinearity is less for turbulence than for a Gaussian field - vorticity tends to be perpendicular to rate-of-strain eigenvector with smallest eigenvalue (aligns with intermediate eigenvalue?)*
SHTILMAN, L.*
On the solenoidality of the Lamb vector*
Phys. Fluids A4, 197*
1992. `
..24.7,19.2,54.0:  "status comparable to energy" (in inviscid flow) - doesn't address non-invariance*
MOFFATT, H.K.; TSINOBER, A.*
Helicity in laminar and turbulent flow*
Ann. Rev. Fluid Mech. 24, 281*
1992. `
..11.6,19.3: relevance to fast-chemistry flamelets - one-point description using simulation data*
GIRIMAJI, S.S.; POPE, S.B.*
Propagating surfaces in isotropic turbulence*
J. Fluid Mech. 234, 247*
1992. `
..11.1,19.3,19.4: focuses on mixed scalar derivative skewness for T, T, u - mainly a comparison of DNS and Test Field Model*
HERRING, J.R.; METAIS, O.*
Spectral transfer and bispectra for turbulence with passive scalars*
J. Fluid Mech. 235, 103*
1992. `
..42.1,19.3: birth, life and lingering death - 128^3 simulations with Schmidt no. 0.1 to 10*
BATCHELOR, G.K.; CANUTO, V.M.; CHASNOV, J.R.*
Homogeneous buoyancy-generated turbulence*
J. Fluid Mech. 235, 349*
1992. `
..19.3: satisfying continuity and Kolmogorov*
FUNG, J.C.H.; HUNT, J.C.R.; MALIK, N.A.; PERKINS, R.J.*
Kinematic simulation of homogeneous turbulence by unsteady random Fourier modes*
J. Fluid Mech. 236, 281*
1992. `
..19.3: the actual time series - looks complicated but nearly periodic*
HUMPHREY, J.A.C.; SCHULER, C.A.; RUBINSKY, B.*
On the use of the Weierstrass-Mandelbrot function to describe the fractal component of turbulent velocity*
Fluid Dynamics Research 9, 81*
1992. `
..02.1,12.2,19.2: lobed mixer not essential*
UKEILEY, L.; ET AL.*
Multifractal analysis of a lobed mixer flowfield utilizing the proper orthogonal decomposition*
AIAA J. 30, 1260*
1992. `
..53.0,19.3: growth or decay is roughly self-preserving*
HOLLOWAY, A.G.L.; TAVOULARIS, S.*
The effects of curvature on sheared turbulence*
J. Fluid Mech. 237, 569*
1992. `
..12.2,19.2: mainly a discussion of difficulties*
AURELL, E.; ET AL.*
On the multifractal properties of the energy dissipation derived from turbulence data*
J. Fluid Mech. 238, 467*
1992. `
..11.1,19.2: Pr near 1, heated cylinder experiments, and theory assuming small correlation between fine-scale velocity and temperature*
TATARSKII, V.I.; ET AL.*
Temperature fluctuation spectrum in the dissipation range for statistically isotropic turbulent flow*
J. Fluid Mech. 238, 683*
1992. `
..19.3:  1/t can exist.  Comments on eps. eqn. Was ICASE Report No. 91-58*
SPEZIALE, C.G.; BERNARD, P.S.*
The energy decay in self-preserving isotropic turbulence revisited*
J. Fluid Mech. 241, 645*
1992. `
..19.2,02.1: Kolmogorov scaling works in turbulent intervals*
KUZNETSOV, V.R.; PRASKOVSKY, A.A.; SABELNIKOV, V.A.*
Fine-scale turbulence structure of intermittent shear flows*
J. Fluid Mech. 243, 595*
1992. `
..19.3,31.1: twelve-wire probe - strong alignment between vorticity and intermediate strain-rate eigenvector*
TSINOBER, A.; KIT, E.; DRACOS, T.*
Experimental investigation of the field of velocity gradients in turbulent flows*
J. Fluid Mech. 242, 169*
1992. `
..19.2: helical modes - backscatter is produced by nonlocal interactions*
WALEFFE, F.*
The nature of triad interactions in homogeneous turbulence*
Phys. Fluids A4, 350*
1992. `
..19.3,14.0: corrections - see Yakhot and Smith*
SMITH, L.M.; REYNOLDS, W.C.*
On the Yakhot-Orszag renormalization group method for deriving turbulence statistics and models*
Phys. Fluids A4, 364*
1992. `
..19.2,25.6: simulation - allegedly inaccurate.  See maledictions of Praskovsky, Van Atta*
HOSOKAWA, I.; YAMAMOTO, K.*
Evidence against the Kolmogorov refined similarity hypothesis*
Phys. Fluids A4, 457*
1992. `
..54.0,19.3: near a strong vortex, largest principal strains are in cross-sectional plane so vorticity is automatically aligned with the intermediate one - see Cantwell, p. 782*
JIMENEZ, J.*
Kinematic alignment effects in turbulent flows*
Phys. Fluids A4, 652*
1992. `
..25.7,19.3: vorticity aligns with intermediate strain - see Jimenez p. 652*
CANTWELL, B.J.*
Exact solution of a restricted Euler equation for the velocity gradient tensor*
Phys. Fluids A4, 782*
1992. `
..19.2: simulation - six triads according to sense of energy transfer to each mode.  Largest transfer between roughly equal wave numbers, mediated by a smaller one*
OHKITANI, K.; KIDA, S.*
Triad interactions in a forced turbulence*
Phys. Fluids A4, 794*
1992. `
..19.3: alternative view - shows that expansion parameter epsilon is an adjustable constant in disguise*
LAM, S.H.*
On the RNG theory of turbulence*
Phys. Fluids A4, 1007*
1992. `
..19.3,25.6: 340^3 Fourier modes, Re,lambda = 176*
KIDA, S.; OHKITANI, K.*
Spatiotemporal intermittency and instability of a forced turbulence*
Phys. Fluids A4, 1018*
1992. `
..19.2: see Smith and Reynolds A3, 992 - inverse exponential OK in dissipating range but not just below it, which explains disagreement of skewness.  See p. 1320, 1492*
SANADA, T.*
Comment on the dissipation-range spectrum in turbulent flows*
Phys. Fluids A4, 1086*
1992. `
..19.2: suggests that extension of Kolmogorov theory to higher order spectra is not valid - Praskovsky agrees*
SANADA, T.; SHANMUGASUNDARAM, V.*
Random sweeping effect in isotropic numerical turbulence*
Phys. Fluids A4, 1245*
1992. `
..19.2: says derivative skewness data consistent with exponential spectrum. See p. 1086, 1492 and A2, 464*
MANLEY, O.P.*
The dissipation range spectrum*
Phys. Fluids A4, 1320*
1992. `
..19.2: see p. 1086, 1320 - argues that data do not go to high enough k to get skewness right, concludes that exponential decay is OK*
GEORGE, W.K.*
The decay of homogeneous isotropic turbulence*
Phys. Fluids A4, 1492*
1992. `
..19.2: Re,lambda = 186 - consistent with Kolmogorov cascade ideas*
KIDA, S.; OHKITANI, K.*
Fine structure of energy transfer in turbulence*
Phys. Fluids A4, 1602*
1992. `
..19.2,25.6: necessarily in Fourier space - suppresses cascade*
MURAKAMI, Y.; SHTILMAN, L.; LEVICH, E.*
Reducing turbulence by phase juggling*
Phys. Fluids A4, 1776*
1992. `
..19.3,12.1: not a high probability of Beltrami state*
WALLACE, J.M.; BALINT, J-L.; ONG, L.*
An experimental study of helicity density in turbulent flows*
Phys. Fluids A4, 2013*
1992. `
..19.2: large scales produce intermittent large strain rate, where small-scale transfer occurs*
DOMARADZKI, J.A.*
Nonlocal triad interactions and the dissipation range of isotropic turbulence*
Phys. Fluids A4, 2037*
1992. `
..11.3,19.1: PDF has exponential tails only at high Re*
WARHAFT, J.Z.*
Probability distribution, conditional dissipation, and transport of passive temperature fluctuations in grid-generated turbulence*
Phys. Fluids A4, 2292*
1992. `
..11.6,19.3: relevant to combustion*
GIRIMAJI, S.S.*
On the modeling of scalar diffusion in isotropic turbulence*
Phys. Fluids A4, 2529*
1992. `
..28.1,19.3: small scale vorticity is rodlike, large scale more disklike*
BRASSEUR, J.G.; WANG, Q.*
Structural evolution of intermittency and anisotropy at different scales analyzed using three-dimensional wavelet transforms*
Phys. Fluids A4, 2538*
1992. `
..19.2,13.0: optimum Rotta constant increases with log Re up to k2/nu eps of 100 at least*
HALLBACK, M.; MALINOWSKY, L.; JOHANSSON, A.V.*
Numerical simulations of return to isotropy in homogeneous turbulence - Reynolds number dependence*
Abstracts, 4th European Turbulence Conf., p. 62*
1992. `
..19.2,11.3,42.3: density-gradient PDF's exponential, density PDF's Gaussian - "velocity-gradient statistics are at the heart of the non-linear dynamics of turbulence*
THORODDSEN, S.T.; VAN ATTA, C.W.*
Exponential tails and skewness of density-gradient probability density functions in stably stratified interactions*
J. Fluid Mech. 244, 547*
1992. `
..19.2: 80x120 experiments*
SADDOUGHI, S.G.*
Local isotropy in high Reynolds number turbulent shear flows*
NASA Ames/Stanford Center for Turb. Research, Ann. Res. Briefs, p. 237*
1992. `
..31.1,19.2: triple four-wire probe for velocity gradients - data still being analysed*
WALLACE, J.M.; ONG, L.; BALINT, J.-L.*
An investigation of small scales of turbulence in a boundary layer at high Reynolds numbers*
NASA Ames/Stanford Center for Turb. Research, Ann. Res. Briefs, p. 263*
1992. `
..19.2: exponential tails with log. dec. varying as r^0.15*
PRASKOVSKY, A.A.*
Probability density distribution of velocity differences at high Reynolds numbers*
NASA Ames/Stanford Center for Turb. Research, Ann. Res. Briefs, p. 269*
1992. `
..19.2: deductions from LES - energy transfer function nearly self-similar*
ZHOU, Y.*
The "ideal" Kolmogorov inertial range and constant*
NASA Ames/Stanford Center for Turb. Research, Ann. Res. Briefs, p. 277*
1992. `
..19.2: points out that energy transfer function is partly a Fourier artifact*
WALEFFE, F.*
The helical decomposition and the instability assumption*
NASA Ames/Stanford Center for Turb. Research, Ann. Res. Briefs, p. 285*
1992. `
..11.3,19.2: small, as expected from local isotropy*
MI, J.; ANTONIA, R.A.*
Joint statistics between temperature and the temperature dissipation components in a turbulent round jet*
Proceedings, 11th Australasian Fluid Mechanics Conference*
1992. `
..54.0,19.3: spectral transfer inhibited.  Comparisons with EDQNM*
MANSOUR, N.N.; CAMBON, C.; SPEZIALE, C.G.*
Theoretical and computational study of rotating isotropic turbulence*
Studies in Turbulence (T.B. Gatski et al., eds.) Springer, p. 59*
1992. `
..19.2: experiments on low - Re wake*
BENZI, R.; ET AL.*
Extended self similarity in turbulent flows*
Phys. Rev. vol. E 48, no. 1, p. R29*
1992. `
..19.2,11.6: log spirals up to 4 or 5 turns - no significant contribution to box-counting dimension.  Refers to Lundgren (1982)*
EVERSON, R.M.; SREENIVASAN, K.R.*
Accumulation rates of spiral-like structures in fluid flows*
Proc. R. Soc. A 437, 391*
1992. `
..19.2: checks on Kolmogorov RSH - scaling with local dissipation*
KARYAKIN, M.Y.; KUZNETSOV, V.R.; PRASKOVSKY, A.A.*
Random variability of scaling exponents in the inertial range power-law approximation*
Abstract for 9th Symposium on Turbulent Shear Flows (not presented)*
1993. `
..31.1,19.2: x wire plus two parallel.  Empirical formula for rms vorticity from two wires*
RAJAGOPALAN, S.; ANTONIA, R.A.*
RMS spanwise vorticity measurements in a turbulent boundary layer*
Expts. in Fluids 14, 142*
1993. `
..19.2,25.6: DNS comparison with random chaotic spectrum - useful review*
SHTILMAN, L.; SPECTOR, M.; TSINOBER, A.*
On some kinematic versus dynamic properties of homogeneous turbulence*
J. Fluid Mech. 247, 65*
1993. `
..19.2: not exactly valid - but subrange universal*
PRASKOVSKY, A.A.; ET AL.*
The sweeping decorrelation hypothesis and energy-inertial scale interaction in high Reynolds number flows*
J. Fluid Mech. 248, 493*
1993. `
..19.3: increase in dissipation rate*
SCHRECK, S.; KLEIS, S.J.*
Modification of grid-generated turbulence by solid particles*
J. Fluid Mech. 249, 665*
1993. `
..11.3,19.3: nearly isotropic - contribution of spatially coherent temperature jumps is small*
ANTONIA, R.A.; MI, J.*
Temperature dissipation in a turbulent round jet*
J. Fluid Mech. 250, 531*
1993. `
..19.5: mapping closure and DNS*
GOTOH, T.; KRAICHANAN, R.H*
Statistics of decaying Burgers turbulence*
Phys. Fluids A5, 445*
1993. `
..19.0,14.0: leads to k, eps., h model - admits non-invariance*
YOKOI, N.; YOSHIZAWA, A.*
Statistical analysis of the effects of helicity in inhomogeneous turbulence*
Phys. Fluids A5, 464*
1993. `
..19.2: mu approx. 0 . 25 from atmospheric data*
SREENIVASAN, K.R.; KAILASNATH, P.*
An update on the intermittency exponent in turbulence*
Phys. Fluids A5, 512*
1993. `
..19.3: exponential fits to tails of dissipation and enstrophy pdf's have different damping constants*
BERSHADSKII, A.; KIT, E.; TSINOBER, A.*
On universality of geometrical invariants in turbulence - experimental results*
Phys. Fluids A5, 1523*
1993. `
..19.3: collapse if normalized by density and wave no. at peak of dissipation spectra - consistent with Kolmogorov or multifractals*
SHE, Z.-S.; JACKSON, E.*
On the universal form of energy spectra in fully developed turbulence*
Phys. Fluids A5, 1526*
1993. `
..19.2,25.6: local transfer - forward and back scatter.  Simulation of Taylor-Green vortex*
DOMARADZKI, J.A.; LIU, W.; BRACHET, M.E.*
An analysis of subgrid-scale interactions in numerically simulated isotropic turbulence*
Phys. Fluids A5, 1747*
1993. `
..11.1,19.3: Exactly soluble examples with prescribed Gaussian velocity field*
MAJDA, A.*
The random uniform shear layer. An explicit example of turbulent diffusion with broad tall probability distributions*
Phys. Fluids A5, 1963*
1993. `
..19.3: In the inertial subrange - contradicts theory of Frisch and others*
PAK, H.K.; GOLDBURG, W.I.*
The absence of inactive regions in turbulent flow. Evidence from light scattering experiments*
Phys. Fluids A5, 2004*
1993. `
..19.3,12.2: model for Q(R) contours developed from solutions of restricted Euler system*
CANTWELL, B.*
On the behavior of velocity gradient tensor invariants in direct numerical simulations of turbulence*
Phys. Fluids A5, 2008*
1993. `
..19.2: argues that box-counting dimension is near enough constant to be useful, despite Miller and Dimotakis - but no wide range of constant D*
PRASKOVSKY, A.A.; FOSS, J.F.; KLEIS, S.J.; KARYAKIN, M.Y.*
Fractal properties of isovelocity surfaces in high Reynolds number laboratory shear flows*
Phys. Fluids A5, 2038*
1993. `
..19.2: not done well but you are surprised to see it done at all. mainly on centerline where uv=0*
KIM, J.; ANTONIA, R.A.*
Isotropy of the small scales of turbulence at low Reynolds number*
J. Fluid Mech. 251, 219*
1993. `
..60.0,18.1,19.3: TKE and vorticity enhanced, length scales decreased - some shock wrinkling*
LEE, S.; LELE, S.K.; MOIN, P.*
Direct numerical simulation of istropic turbulence interacting with a weak shock wave*
J. Fluid Mech. 251, 533*
1993. `
..19.3: mainly relating to curvature - Pope et al. 1989*
DRUMMOND, I.T.*
Stretching and bending of line elements in random flows*
J. Fluid Mech. 252, 479*
1993. `
..19.3: vortex dynamics model based on nonlin. random D.E.*
LIU, T.*
A note on the probability distribution of the dissipation rate in locally isotropic turbulence*
Phys. Fluids A5, 2234*
1993. `
..19.3,13.0: pressure effects*
RISTORCELLI, J.R.; LUMLEY, J.L.*
The dependence of the dissipation on rotation*
Phys. Fluids A5, 2304*
1993. `
..19.3,25.6: implications for Germano model*
SCOTTI, A.; MENEVEAU, C.; LILLY, D.*
Generalized Smagorinsky model for anisotropic grids*
Phys. Fluids A5, 2306*
1993. `
..11.4,19.2: cold-wire data agree with simulation when corrected for wire separation*
ZHU, Y.; ANTONIA, R.A.*
Temperature dissipation measurements in a fully developed turbulent channel flow*
Expts. in Fluids 15, 191*
1993. `
..14.0,13.0,19.4: adds non-linear terms and helicity effects*
YOSHIZAWA, A.*
Bridging between eddy-viscosity-type and second-order models using a two-scale DIA*
Presented at 9th Sympo. on Turbulent Shear Flows, Kyoto, paper 23-1*
1993. `
..19.3: discussion based on DNS - Re simply too low to be useful*
ANTONIA, R.A.; KIM, J.*
Isotropy of small scale turbulence*
Presented at 9th Sympo. on Turbulent Shear Flows, Kyoto, paper 24-1*
1993. `
..19.4,13.0: DIA leading to LRR*
RUBINSTEIN, R.*
Time dependent turbulence modeling and analytical theories of turbulence*
NASA TM 106379*
1993. `
..19.2: goes as t^0.25 approx.-  LES, Re not stated*
CHASNOV, J.R.*
Computation of the Loitsianski integral in decaying isotropic turbulence*
Phys. Fluids A5, 2579*
1993. `
..19.3: DNS at microscale Re of 250. DIA surprisingly accurate but test field method has errors*
HERRING, J.R.; KERR, R.M.*
Development of enstrophy and spectra in numerical turbulence*
Phys. Fluids A5, 2792*
1993. `
..19.2: not wholly conclusive*
GILBERT, A.D.*
A cascade interpretation of Lundgren's stretched spiral vortex model for turbulent fine structure*
Phys. Fluids A5, 2831*
1993. `
..12.2,19.3: one scale depending on large eddies, one on (microscale) Re*
KAILASNATH, P.; SREENIVASAN, K.R.*
Zero crossings of velocity fluctuations in turbulent boundary layers*
Phys. Fluids A5, 2879*
1993. `
..19.2: "worms", radius of order eta, length of order integral length scale - prob. dists. increasingly non-Gaussian with increasing Re*
JIMENEZ, J.; WRAY, A.A.; SAFFMAN, P.G.; ROGALLO, R.S.*
The structure of intense vorticity in isotropic turbulence*
J. Fluid Mech. 255, 65*
1993. `
..24.1,19.2: just so*
FOSS, J.F.; BOHL, D.G.; KLEIS, S.J.*
Vorticity-vorticity correlation functions in a two-stream mixing layer*
APS Bull. 38, 2246*
1993. `
..11.1,19.2: maximum near extrema of concentration - partly attributable to large-scale intermittency?*
KAILASNATH, P.; SREENIVASAN, K.R.; SAYLOR, J.R.*
Conditional scalar dissipation rates in turbulent wakes, jets, and boundary layers*
Phys. Fluids A5, 3207*
1993. `
..18.1,19.3: DNS - reduced growth rate attributed to dissipation via pressure-dilatation correlation*
BLAISDELL, G.A.; MANSOUR, N.N.; REYNOLDS, W.C.*
Compressibility effects on the growth and structure of homogeneous turbulent shear flow*
J. Fluid Mech. 256, 443*
1993. `
..19.2: concentric spiral vortex threads wrapped round roller*
MELANDER, M.V.; HUSSAIN, F.*
Coupling between a coherent structure and fine-scale turbulence*
Phys. Rev. E 48, 2669*
1993. `
..11.3,19.1: scalar prod./diss. up to 3*
GIBSON, M.M.; DAKOS, T.*
Production of temperature fluctuations in grid turbulence - Wiskind's experiment revisited*
Expts. in Fluids 16, 146*
1993. `
..54.0,19.3: strong tendency to two dimensionality*
SQUIRES, K.D.: ET AL.*
Investigation of the asymptotic state of rotating turbulence using large-eddy simulation*
Nasa Ames/Stanford Univ. Center for Turbulence Research, Annual Research Briefs 1993 (P. Moin and W.C. Reynolds, eds), 157* 
1993. `
..19.2,12.1: Seyed's silo*
SADDOUGHI, S.G.*
Local isotropy in strained turbulent boundary layers at high Reynolds number*
Nasa Ames/Stanford Univ. Center for Turbulence Research, Annual Research Briefs 1993 (P. Moin and W.C. Reynolds, eds), 347* 
1993. `
..12.2,19.2: more severe test than one-point statistics*
O'NEIL, J.; MENEVEAU, C.*
Spatial correlations in turbulence. Predictions from the multifractal formalism and comparison with experiments*
Phys. Fluids A5, 158*
1993. `
..19.2: experiments on low-Re wake*
BENZI, R.; ET AL.*
Extended self similarity in turbulent flows*
Phys. Rev. E vol. 48, no. 1, p. R29*
1993. `
..13.0,19.3: eddy-viscosity closure of Karman-Howarth equation*
OBERLACK, M.; PETERS, N.*
Closure of the two-point correlation equation as a basis for Reynolds stress models*
Advances in Turbulence IV (F.T.M. Nieuwstadt, ed.), Kluwer, Dordrecht (also Appl. Sci. Res. Vol. 51), p. 533*
1993. `
..19.2,13.0: optimum Rotta constant increases with log Re up to k2/nu eps of 100 at least*
HALLBACK, M.; JOHANSSON, A.V.*
Modeling of pressure-strain rate in homogeneous turbulencee*
Advances in Turbulence IV (F.T.M. Nieuwstadt, ed.), Kluwer, Dordrecht (also Appl. Sci. Res. Vol. 51), p. 495*
1993. `
..19.2: 80x120 measurements*
VEERAVALLI, S.V.; SADDOUOGHI, S.G.; PRASKOVSKY, A.A.; BRADSHAW, P.*
A note on local isotropy in high-Reynolds-number turbulence*
New Approaches and Concepts in Turbulence, Monte Verita (T. Drakos and A. Tsinober, eds.) Birkhauser, Basel, p. 377*
1993. `
..19.3: produced by shear instabilities as important as vortex stretching. Simulation at microscale Re of 150*
VINCENT, A.; MENEGUZZI, M.*
The dynamics of vorticity tubes in homogeneous turbulence*
J. Fluid Mech. 258, 245*
1994. `
..19.3: deviation from Kolmogorov theory, K41 - high-k intermittency*
GROSSMAN, S.; LOHSE, D.*
Scale resolved intermittency in turbulence*
Phys. Fluids 6, 611*
1994. `
..19.3,11.1,28.1: invariant representation of "shape", see also 652*
KERSTEIN, A.R.; SCHEFER, R.W.; NAMAZIAN, M.*
A conditional similarity concept for turbulent shear flow, with application to mixing in a round jet*
Phys. Fluids 6, 642*
1994. `
..19.2,25.6: Karhunen-Loeve eigenfuntions better than Fourier*
MOSER, R.D.*
Kolmogorov inertial range specture for inhomogeneous turbulence*
Phys. Fluids 6, 794*
1994. `
..19.2,14.0: simulations - c, eps, 2 and derivative skewness as function of Re, lambda*
MANSOUR, N.N.; WRAY, A.A.*
Decay of isotropic turbulence at low Reynolds number*
Phys. Fluids 6, 808*
1994. `
..19.2: detailed paper - local-to-nonlocal (up to 10 to 1) interactions isotropize, but distant interactions affect small scales directly*
BRASSEUR, J.G.; WEI, C.-H.*
Interscale dynamics and local isotropy in high Reynolds number turbulence within triadic interactions*
Phys. Fluids 6, 842*
1994. `
..19.3: analytic form of correlation or spectrum*
SIROVICH, L.; SMITH, L.; YAKHOT, V.*
Energy spectrum of homogeneous and isotropic turbulence in far dissipation range*
Phys. Rev. Letters 72, 344*
1994. `
..19.3: fine structures assumed to be "intermittent filaments"*
SHE, Z.-S.; LEVEQUE, E.*
Universal scaling laws in fully developed turbulence*
Phys. Rev. Letters 72, 336*
1994. `
..54.0,19.2: nonaxisymmetric correlation between entsrophy and dissipation only 0 . 19*
MOFFATT, H.K.; KIDA, S.; OHKITANI, K.*
Stretched vortices - the sinews of turbulence. Large-Reynolds-number asymptotics*
J. Fluid Mech. 259, 241*
1994. `
..19.3,54.0: nearly-2D state, i.e., 2-component also*
HOSSAIN, M.*
Reduction in the dimensionality of turbulence due to a strong rotation*
Phys. Fluids 6, 1077*
1994. `
..19.2: accounts for the hump on the spectrum - molecular viscosity suppresses turbulent viscosity*
FALKOVICH, G.*
Bottleneck phenomenon in developed turbulence*
Phys. Fluids 6, 1441*
1994. `
..19.2: "octave-to-octave" transfer - but low Re simulations*
DOMARADSKI, J.A.; ET AL.*
Energy transfer in numerically simulated wall-bounded turbulent flows*
Phys. Fluids 6, 1583*
1994. `
..19.2: don't get an inertial subrange - see Ghosal CTR 151*
SULLIVAN, N.P.; MAHALINGAM, S.; KERR, R.A.*
Deterministic forcing of homogeneous, isotropic turbulence*
Phys. Fluids 6, 1612*
1994. `
..19.2,25.6: kinematic relations, relevant to SGS models - 11-fold integrals*
PULLIN, D.I.; SAFFMAN, P.G.*
Reynolds stresses and one-dimensional spectra for a vortex model of homogeneous anisotropic turbulence*
Phys. Fluids 6, 1787*
1994. `
..11.1,19.3: analysis of homo. flow with Gaussian velocity and scalar gradient explains deviations from local-isotropy arguments*
HOLZER, M.; SIGGIA, E.D.*
Turbulent mixing of a passive scalar*
Phys. Fluids 6, 1820*
1994. `
..19.3: axi. expansions important in dissipation process*
LUND, T.S.; ROGERS, M.M.*
An improved measure of strain state probability in turbulent flows*
Phys. Fluids 6, 1838*
1994. `
..11.1,19.3: pdfs Gaussian for large scales, exponential for small scales*
CHRISTIE, S.L.; DOMARADZKI, J.A.*
Scale dependence of the statistical character of turbulent fluctuations in thermal convection*
Phys. Fluids 6, 1848*
1994. `
..21.2,19.2: flying hot wire for mean-square derivatives*
HUSSEIN, H.J.*
Evidence of local axisymmetry in the small scales of a turbulent planar jet*
Phys. Fluids 6, 2058*
1994. `
..11.1,19.2: microscale Re up to 130*
TONG, C.; WARHAFT, Z.*
On passive scalar derivative statistics in grid turbulence*
Phys. Fluids 6, 2165*
1994. `
..19.2: dissipating range remains isotropic*
SADDOUGHI, S.G.; VEERAVALLI, S.V.*
Local isotropy in turbulent boundary layers at high Reynolds number*
J. Fluid Mech. 268, 333*
1994. `
..19.3: two high-k scalar modes coupled by one low-k velocity mode*
YEUNG, P.K.*
Spectral transfer of self-similar passive scalar fields in isotropic turbulence*
Phys. Fluids 6, 2245*
1994. `
..19.1: the "nearly" spoils it - both sustained and decaying turbulence considered*
DE SILVA, I.P.D.; FERNANDO, H.J.S.*
Oscillating grids as a source of nearly isotropic turbulence*
Phys. Fluids 6, 2455*
1994. `
..19.2,05.0: increases as Re decreases, even in inner layer*
ANTONIA, R.A.; DJENIDI, L.; SPALART, P.R.*
Anisotropy of the dissipation tensor in a turbulent boundary layer*
Phys. Fluids 6, 2475*
1994. `
..43.1,19.3: wavelet expansions of field data at UC Davis*
KATUL, G.G.; PARLANGE, M.B.; CHU, C.R.*
Intermittency, local isotropy, and non-Gaussian statistics in atmospheric surface layer turbulence*
Phys. Fluids 6, 2480*
1994. `
..19.2,25.6: Kraichnam k-dependent eddy viscosity in 64^3 simulation*
BRISCOLINI, M.; SANTANGELO, P.*
The non-Gaussian statistics of the velocity field in low-resolution large-eddy simulations of homogeneous turbulence*
J. Fluid Mech. 270, 199*
1994. `
..19.3: analysis of DNS supports traditional view of spatially-distinct eddies cascading to smaller scales*
MENEVEAU, C.; LUND, T.S.*
On the Lagrangian nature of the turbulence energy cascade*
Phys. Fluids 6, 2820*
1994. `
..19.2: Kolmogorov's constant goes as Re, lambda to - 0.1 power*
PRASKOVSKY, A.; ONCLEY, S.*
Measurements of the Kolmogorov constant and intermittency exponenent at very high Reynolds numbers*
Phys. Fluids 6, 2886*
1994. `
..19.3,13.0: transport equation for modal rms, with empirical tranfer term*
LEWALLE, J.; TAVLARIDES, L.L*
A cascade-transport model for turbulent shear flows*
Phys. Fluids 6, 3109*
1994. `
..19.3,11.1: at large t, square of separation distance has chi-square pdf*
YEUNG, P.K.*
Direct numerical simulation of two-particle relative diffusion in isotropic turbulence*
Phys. Fluids 6, 3416*
1994. `
..19.3: 128^3 DNS - near-longitudinal vortex tubes have vorticity vector about 10 deg. from vortex axis, leading indirectly to stretching of spanwise vorticity*
KIDA, S.; TANAKA, M.*
Dynamics of vortical structures in a homogenous shear flow*
J. Fluid Mech. 274, 43*
1994. `
..19.3: small-scale anisotropy peaks soon after start of anisotropic low-k forcing, then decreases*
ZHOU, Y.; YEUNG, P.K.; BRASSEUR, J.G.*
Scale disparity and spectral transfer in anisotropic numerical turbulence*
Penn. State Univ. paper*
1994. `
..19.3: DNS. Microscale Re from 5 to 50. Faster decay index at lower Re but not "final period"*
HUANG, M.-J.; LEONARD, A.*
Power-law decay of homogeneous turbulence at low Reynolds numbers*
Phys. Fluids 6, 3765*
1994. `
..19.3,28.1: mainly review*
WANG, Q.; BRASSEUR, J.G.*
Relationship between scale and structure in turbulence analyzed using three-dimensional wavelet transforms*
From the Ph.D. Thesis of Qunzhen Wang, Penn State Univ.*
1994. `
..19.2: Up to 8th order (105 isotropic tensors)*
PHAN-THIEN, N.; ANTONIA, R.A.*
Isotropic Cartesian tensors of arbitrary even orders and velocity gradient correlation functions*
Phys. Fluids 6, 3818*
1994. `
..19.3: DNS - large gradients become rarer as Re increases, but not explicity stated that they become larger*
PUMIR, A.*
Small-scale properties of scalar and velocity differences in 3-D turbulence*
Phys. Fluids 6, 3974*
1994. `
..18.2,50.0,19.1: Merzkirch-like experiment with grid in shock tube*
HONKAN, A.; WATKINS, C.B.; ANDREOPOULOS, J.*
Experimental study of interactions of shock wave with free-stream turbulence*
J. Fluids Engg. 116, 763*
1994. `
..54.0,19.3: complete spectral similarity prevented by reverse energy cascade in 2D, 2C motion*
SQUIRES, K.D.; CHASNOV, J.R.; MANSOUR, N.N.*
On the asymptotic similarity of rotating homogeneous turbulence*
NASA Ames/Stanford Center for Turbulence Research, Summer Program 1994, 383*
1994. `
..54.0,19.3: LES results - 2 types of critical Rossby number*
CAMBON, C.; MANSOUR, N.N.; SQUIRES, K.D.*
Anisotropic structure of homogeneous turbulence subjected to uniform rotation*
NASA Ames/Stanford Center for Turbulence Research, Summer Program 1994, 397*
1994. `
..19.2,61.0: "low" means microscale Re of 560 or more. Sequel to 1993 report on high Re - further analysis in progress. Kolmogorov OK at high Re*
SADDOUGHI, S.G.*
Small-scale behavior in distorted turbulent boundary layers at low Reynolds number*
NASA Ames/Stanford Center for Turbulence Research, Ann. Research Briefs, 243*
1994. `
..19.2: description of equipment - no results presented*
FOSS, J.F.; ET AL.*
Traverse vorticity measurements in the NASA Ames 80 ft x 120 ft wind tunnel boundary layer*
NASA Ames/Stanford Center for Turbulence Research, Ann. Research Briefs, 263*
1994. `
..19.2: atmospheric BL and CAHI (TsAGI) tunnel - no final conclusions, as "isotropic" assumption for dissipation is suspect*
PRASKOVSKY, A.*
Experimental and numerical study of the intermittency exponent mu*
NASA Ames/Stanford Center for Turbulence Research, Ann. Research Briefs, 269*
1994. `
..19.2: fraction of volume occupied by vortex "worms" decreases as (microscale Re)^(-2) - "somewhat misleading" result since diameter goes as eta.*
JIMENEZ, J.; WRAY, A.A.*
On the dynamics of small-scale vorticity in isotropic turbulence*
NASA Ames/Stanford Center for Turbulence Research, Ann. Research Briefs, 287*
1994. `
..19.2,31.1: need step size of 1.5 eta to get sixth moment of pdf, but 3 eta OK through fourth moment*
JIMENEZ, J.*
Resolution requirements for velocity gradients in turbulence*
NASA Ames/Stanford Center for Turbulence Research, Ann. Research Briefs, 357*
1994. `
..12.2,19.3: interesting exercise on c, mu etc.*
SCHUMANN, U.*
On relations between constants in homogeneous turbulence models and Heisenberg's spectral model*
Beitr. Phys. Atmosph. 67, 141*
1994. `
..19.2,22.2: useful review of small-scale structure*
NELKIN, M.*
Universality and scaling in fully developed turbulence*
Advances in Physics 43, 143*
1994. `
..19.2: "distant" interactions (more than 10 to 1 in k) cause differential advection and distortion of small-scale vorticity*
YEUNG, P.K.; BRASSEUR, J.G.; WANG, Q.*
Dynamics of direct large-small scale couplings in coherently forced turbulence - concurrent physical- and Fourier-space views*
J. Fluid Mech. 283, 43*
1995. `
..19.3: perturbation analysis*
PASSOT, T.; ET AL.*
Instability of strained vortex layers and vortex tube formation in homogeneous turbulence*
J. Fluid Mech. 282, 313*
1995. `
..54.0,19.3: LES return to isotropy for k^4 low-wave number initial spectrum, not for k^2*
CHASNOV, J.R.*
The decay of axisymmetric homogeneous turbulence*
Phys. Fluids 7, 600*
1995. `
..12.1,54.0,19.3: Koh's form of Poisson eqn, plus experiment in a "cell"*
CADOT, O; DOUADY, S.; COUDER, Y.*
Characterization of low-pressure filaments in a three-dimensional turbulent shear flow*
Phys. Fluids 7, 630*
1995. `
..19.2: says previous experiments got the right answer only by evaluating dissipation from du/dt*
THORODDSEN, S.T.*
Reevaluation of the experimental support for the Kolmogorov refined similiarity hypothesis*
Phys. Fluids 7, 691*
1995. `
..11.1,19.3: ratio of velocity to scalar time scale varies widely, contrary to eddy-breakup model*
FOX, R.O.*
The spectral relaxation model of the scalar dissipation rate in homogeneous turbulence*
Phys. Fluids 7, 1082*
1995. `
..16.1,25.6: repeat of Spalart scrubbing flow, JFM 205, 319. Reynolds-stress angle 8 deg. from shear stress at wall*
WU, X.; SQUIRES, K.D.*
Large-eddy simulation of a canonical three-dimensional boundary layer*
To be presented at 10th Sympo. on Turbulent Shear Flows*
1995. `
..19.2, 05.0: independent of y outside the buffer layer - but is this just approx. law of the wall scaling?*
DINAVAHI, S.P.G.; BREUER, K.S.; SIROVICH, L*
Universality of probability density functions in turbulent channel flow*
Phys. Fluids 7, 1122*
1995. `
..19.3: rigorously established analytical results*
DOERING, C.R.; TITI, E.S.*
Exponential decay rate of the power spectrum for solutions of the Navier-Stokes equations*
Phys. Fluids 7, 1384*
1995. `
..19.3: wave packets rather than Fourier modes - energy transfer acquires a noise term*
OLLA, P.*
A closure model for intermittency in 3-D incompressilbe turbulence*
Phys. Fluids 7, 1599*
1995. `
..19.3,11.1,43.1: with measurements in a circular jet (microscale Re = 250) and PBL (7200)
ZHU, Y.; ANTONIA, R.A.; HOSOKAWA, I.*
Refined similarity hypotheses for turbulent velocity and temperature fields*
Phys. Fluids 7, 1637*
1995. `
..12.2,19.3: discussion of techniques, then evaluation of 80x120 data etc. Dimension approx. 5/3 as per theory*
SCOTTI, A.; MENEVEAU, C.; SADDOUGHI, S.G.*
Fractal dimension of velocity signals in high-Reynolds-number hydrodynamic turbulence*
Am. Phys. Review 51, 51*
1995. `
..19.2: absolute value of velocity difference goes as separation^{-0.55} (Kolmogorov says -1/2) but Re only 2.4 times Re for subcritical transition*
MALERUD, S.; ET AL.*
Measurements of turbulent velocity fluctuations in a planar Couette cell*
Phys. Fluids 7, 1949*
1995. `
..19.2: oscillating grid - Re, lambda up to 300. Filaments more frequent near tank walls*
VILLERMAUX, E.; SIXOU, B.; GAGNE, Y.*
Intense vortical structures in grid-generated turbulence*
Phys. Fluids 7, 2008*
1995. `
..19.2: different techniques (Kuo-Corrsin inspection and Sreenivasan envelope) give different answers*
ZUBAIR, L.*
On the characteristics of the fine-scale intermittency of turbulence*
Phys. Fluids 7, 2089*
1995. `
..54.0,19.3: uses Kraichnan MHD theory*
ZHOU, Y.*
A phenomenological treatment of rotating turbulence*
Phys. Fluids 7, 2092*
1995. `
..19.2: painstaking review - no Re trend of -5/3 tangent to longitudinal spectra*
SREENIVASAN, K.R.*
On the universality of the Kolmogorov constant*
Phys. Fluids 7, 2778*
1995. `
..19.2,28.1: arbitrary simplifications but no empirical constant. Gives -5/3 (just dimensions?)*
ZIMIN, V.; HUSSAIN, F.*
Wavelet based model for small-scale turbulence*
Phys. Fluids 7, 2925*
1995. `
..19.5: "stretched exponentials"*
AVELLANEDA, M; RYAN, R.; WEINAN E.*
PDFs for velocity and velocity gradients in Burgers' turbulence*
Phys. Fluids 7, 3067*
1995. `
..12.2,07.0,19.2: Re-dependent corrections to K41?*
BARENBLATT, G.I.; GOLDENFELD, N.*
Does fully developed turbulence exist? Reynolds number independence versus asymptotic covariance*
Phys. Fluids 7, 3078*
1995. `
..21.3,19.2,11.2: correlation 0.74 for Sc >> 1 in jet*
SOUTHERLAND, K.B.; DAHM, W.J.A.*
Experimental assessment of Taylor's hypothesis and its applicability to dissipation estimates in turbulent flows*
Presented at 10th Sympo. on Turbulent Shear Flows, Penn. State, paper 1-13*
1995. `
..22.2,19.2: mainly Kolmogorov and backscatter*
KADANOFF, L.P.*
A model of turbulence*
Physics Today, vol. 48, no. 9, p. 11*
1995. `
..11.1,19.2: analogy with Kolmogorov 1962 - supported  by data in a wake at moderate Re*
STOLOVITZKY, G.; KAILASNATH, P.; SREENIVASAN, K.R.*
Refined similarity hypotheses for passive scalars mixed by turbulence*
J. Fluid Mech. 297, 275*
1995. `
..54.0,19.3: steady state can be reached under oscillating strain with zero mean*
VERZICCO, R.; JIMENEZ, J.; ORLANDI, P.*
On steady columnar vortices under local compression*
J. Fluid Mech. 299, 367*
1995. `
..19.3:new  "considerable simplifications" of correlation tensor -  simple scalar function. No explicit reference to irrotational flow*
LINDBORG, E.*
Kinematics of homogeneous axisymmetric turbulence*
J. Fluid Mech. 302, 179*
1995. `
..18.1,19.4: stripped-down two-scale DIA - spectral theory not needed. No compressibility effects at eddy-viscosity level*
YOSHIZAWA, A.*
Simplified statistical method for modelling complex turbulent flows, effects of compressibility*
Proceedings, International Symposium on Mathematical Modelling of Turbulent Flows, Tokyo, (H. Daiguji and Y, Mitake, eds.), Japan Soc. of CFD, p. 111*
1995. `
..19.2: 2D and 3D.  Empirical correction to -5/3 law*
BOWMAN, J.C.*
On inertial-range scaling laws*
J. Fluid Mech. 306, 167*
1996. `
..19.3: body force cos x in a box - hyperviscosity to simulate high Re*
BORUE, V.; ORSZAG, S.A.*
Numerical study of three-dimensional Kolmogorov flow at high Reynolds number*
J. Fluid Mech. 306, 293*
1996. `
..24.2,19.3: transition by rollup of vortex sheets into vortex tubes*
LUNDGREN, T.S.; MANSOUR, N.N.*
Transition to turbulence in an elliptic vortex*
J. Fluid Mech. 307, 43*
1996. `
..19.3: up to 36 - too low for Kolmogorov theory but "extended self similarity" exists*
CAMUSSI, R.; GUJ, G.*
Experimental analysis of scaling laws in low Re grid-generated turbulence*
Expts. in Fluids 20, 199*
1996. `
..19.2,25.6: Brasseur group, 512^3 DNS on CM5. K=1.68*
WANG, L.-P.; ET AL.*
Examination of hypotheses in the Kolmogorov refined turbulence theory through high-resolution simulations. Part 1. Velocity field*
J. Fluid Mech. 309, 113*
1996. `
..24.1,50.0,19.2: DNS - good agreement with Veeravalli.  Turbulence models also tested*
BRIGGS, D.A.; ET AL.*
Entrainment in a shear-free turbulent mixing layer*
J. Fluid Mech. 310, 215*
1996. `
..19.3,05.0: Kim's Re, tau = 395  DNS. Vorticity tends to be aligned with intermediate principal strain rate.  General behavior simular to other flows even if not isotropic*
BLACKBURN, H.M.; MANSOUR, N.N.; CANTWELL, B.J.*
Topology of fine-scale motions in turbulent channel flow*
J. Fluid Mech. 310, 269*
1996. `
..19.3: depends on Re even after proper scaling - but low Re/simulation data*
ANTONIA, R.A.; RAJAGOPALAN, S.; ZHU, Y.*
Scaling of mean square vorticity in turbulent flows*
Expts in Fluids 20, 393*
1996. `
..19.1: just so*
SRDIC, A.; FERNANDO, H.J.S.; MONTENEGRO, L.*
Generation of nearly isotropic turbulence using two oscillating grids*
Expts in Fluids 20, 395*
1996. `
..19.3,12.2: of velocity gradients*
JIMENEZ, J.*
Algebraic probability density tails in decaying isotropic two-dimensional turbulence*
J. Fluid Mech. 313, 223*
1996. `
..11.1,19.3: exponential tails*
JABERI, F. A.; ET AL.* 
Non-Gaussian scalar statistics in homogeneous turbulence*
J. Fluid Mech. 313, 241*
1996. `
..07.0,05.0,19.2: says the analogy is well known*
BARENBLATT, G. I.; CHORIN, A.J.*
Small viscosity asymptotics for the inertial range of local structure and for the wall region of wall-bounded turbulent shear flow*
Proc. Nat. Acad. Sci. 93, 6749*
1996. `
..09.5,19.2: addition of helical high-k energy increases decay rate*
SUZUKI, Y.; YAMADA, S.; NAGANO, Y.*
Controlling helical/non-helical turbulence with small-scale energy input*
Abstract for Workshop on Flow Control, Corsica*
1996. `
..19.2: using DNS data - topology*
CHENG, W.-P.*
Study of the velocity gradient tensor in turbulent flow*
SUDAAR Rept. 685, Ph.D. thesis, Aero/Astro Dept, Stanford Univ.*
1996. `
..11.6,19.2,21.2: Sc = 2000. Scalar dissipation in sheet-like diffusion layers*
BUCH. K.A.; DAHM, W.J.A.*
Experimental study of the fine-scale structure of conserved scalar mixing in turbulent shear flows.  Part 1. Sc >> 1*
J. Fluid Mech. 317, 21*
1996. `
..11.6,19.1: extra spreading due to chemical reaction is small*
LI, J.D.; BILGER, R. W.*
The diffusion of conserved and reactive scalars behind line sources in homogeneous turbulence*
J. Fluid Mech. 318, 339*
1996. `
..19.2: microscale Re up to 473, using Makita "active grid". Discussion of K41 theory*
MYDLARSKI, L.; WARHAFT, Z.*
On the onset of high-Reynolds-number grid-generated wind tunnel turbulence*
J. Fluid Mech. 320, 331*
1996. `
..20.0,19.2,31.1: correction of 4-wire probe measurements*
ANTONIA, R.A.; ZHU, Y.; SHAFI, H.S.*
Lateral vorticity measurements in a turbulent wake*
J. Fluid Mech. 323, 173*
1996. `
..19.2: iso. DNS - fine scale identified by second invariant of vel. gradient*
TANAHASHI, M.; MIYAUCHI, T.; YOSHIDA, T.*
Characteristics of small scale vortices related to turbulent energy dissipation*
Proc 9th Int. Sympo. on Transport Phenomena (S.H. Winoto, Y.T. Chew and N.E. Wijeysundera, eds.), Pacific Ctr of Thermal-Fluids Engg, Maui, Hawaii, vol. 2, p. 1256*
1996. `
..11.1,19.2: universal -5/3 spectrum found in shear flows only for microscale Re>1000, but in iso. turb. even at modest Re. O-C constant about 0.4*
SREENIVASAN, K.R.*
The passive scalar spectrum and the Obukhov-Corrsin constant*
Phys. Fluids 8, 189*
1996. `
..19.2,25.6: DNS results show correlation between regions of vorticity production and of SGS transfer*
KERR, R.M.; DOMARADZKI, J.A.; BARBIER, G.*
Small-scale properties of nonlinear interactions and subgrid-scale energy transfer in isotropic turbulence*
Phys. Fluids 8, 197*
1996. `
..12.1,19.2: axisymmetry about x axis is better approx than local isotropy near duct center line*
ZHU, Y.; ANTONIA, R.A.; KIM, J.*
Two-point velocity and vorticity correlations for axisymmetric turbulence*
Phys. Fluids 8, 838*
1996. `
..11.1,19.2: confirms Richardson's law, variance = 0.062 eps. t 3*
ELLIOTT, F.W.; MAJDA, A.J.*
Pair dispersion over an inertial range spanning many decades*
Phys. Fluids 8, 1052*
1996. `
..19.1: microscale Re from 37 to 82. Hot wire measurements behind grid. "Inhomogeneous" refers to transverse variations at x/M = 9*
CAMUSSI, R.; ET AL.*
Transverse and longitudinal scaling laws in non-homogeneous low Re turbulence*
Phys. Fluids 8, 1181*
1996. `
..11.1,19.3: calculation for Gaussian velocity pdf shows that increasing  horizontal intensity reduces vertical transport*
VINCENT, A.; MICHAUD, G.; MENEGUZZI, M.*
On the turbulent transport of a passive scalar by anisotropic turbulence*
Phys. Fluids 8, 1312*
1996. `
..19.2,20.0: inferred from lateral vorticity measurements in cylinder wake*
ANTONIA, R.A.; SHAFI, H.S.; ZHU, Y.*
A note on the vorticity spectrum*
Phys. Fluids 8, 2196*
1996. `
..19.2,23.0: volume integral of difference depends on boundary conditions - relevant to integral of pressure equation*
RAYNAL, F.*
Exact relation between spatial mean enstrophy and dissipation in confined incompressible flows*
Phys. Fluids 8, 2242*
1996. `
..19.2: suggests that longitudinal derivative gives an adequate estimate for exponent mu*
SHAFI, H.S.; ZHU, Y.; ANTONIA, R.A.*
Intermittency of vorticity in a turbulent shear flow*
Phys. Fluids 8, 2245*
1996. `
..19.1: oscillating grid - depth of turbulent layer increases as time^(1/2)*
VOROPAYEV, S.I.; FERNANDO, H.J.S.*
Propagation of grid turbulence in homogenous fluids*
Phys. Fluids 8, 2435*
1996. `
..19.2: same exponents govern return to isotropy and scaling of correlations in isotropic turbulence. Suggestions for experiments*
L'VOV,V.; PROCACCIA, L.*
The universal scaling exponents of anisotropy in turbulence and their measurement*
Phys. Fluids 8, 2565*
1996. `
..23.0,19.3: suggested benchmark for pressure-term modeling*
HILL, R.J.*
Pressure-velocity-velocity statistics in isotropic turbulence*
Phys. Fluids 8, 3085*
1996. `
..19.2: implied if dissipating events are very rare - log-normal if there are many regions with roughly equal dissipation rates*
GLEDZER, E; ET AL.*
On the log-Poisson statistics of the energy dissipation field and related problems of developed turbulence*
Phys. Fluids 8, 3367*
1996. `
..19.2: derivation from transport equation for two-point covariance (generalized Karman-Howarth)*
LINDBORG, E.*
A note on Kolmogorov's third-order structure-function law, the local isotropy hypothesis and the pressure-velocity correlation*
J. Fluid Mech. 326, 343*
1996. `
..12.1,19.2; scalars with Sc>>1. Dissipation is fractal, level crossings are not*
FREDERIKSEN, R.D.; DAHM, W.J.A.; DOWLING, D.R.*
Experimental assessment of fractal scale-similarity in turbulent flows. Part 1. One-dimensional intersections*
J. Fluid Mech. 327, 35*
1996. `
..19.2: iso. DNS  - time scale identified by second invariant of vel. gradient*
TANAHASHI, M.; MIYAUCHI, T.; YOSHIDA, T.*
Characteristics of small scale vortices related to turbulent energy dissipation*
Proc. 9th Symposium on Transport Phenomena 2, 1256*
1996. `
..19.2: TIT - 2nd invariant of vel. gt.*
TANAHASHI, M.; MIYAUCHI, T.; YOSHIDA, T.*
Fine scale coherent structure in turbulence*
Presented at 1996 Mtg of Japan Society of Fluid Mech., preprint volume p. 55*
1996. `
..19.2: sheets, spirals, tubes, finally worms*
OIDE, S.-I.; ET AL.*
DNS of worm generation in isotropic turbulence*
Presented at 1996 Mtg of Japan Society of Fluid Mech., preprint volume p. 189*
1996. `
..19.2,18.1: M_t up to 1.1. Shear layers accompanied by shocklets*
MAEKAWA, H.; NATSUO, Y.; HIYAMA, T.*
Structures of high enstrophy in numerically simulated compressible isotropic turbulence*
Presented at 1996 Mtg of Japan Society of Fluid Mech., preprint volume p. 287*
1996. `
..19.3: vortex-tube identification. Title phrase unclear*
VASSILICOS, J.C.; BRASSEUR, J.G.*
Kolmogorov capacities of streamlines around turbulent vortex tubes*
Advances in Turbulence 6 (ETC  Lausanne), (S. Gavrilakis, L. Machiels, and P.  Monkewitz, eds.), Kluwer, p. 145*
1996. `
..19.2: non-Gaussian economics - probability functions. inter-dealer trading is the cascade*
GHASHGHAIE, S.; ET AL.*
Turbulence and financial markets*
Advances in Turbulence 6 (ETC  Lausanne), (S. Gavrilakis, L. Machiels, and P.  Monkewitz, eds.), Kluwer, p. 167*
1996. `
..19.3: high-Re gamma poorly described by low-Re correlation*
KUS'MIN, G.A.*
Small scale intermittency and the renormalization group*
Advances in Turbulence 6 (ETC  Lausanne), (S. Gavrilakis, L. Machiels, and P.  Monkewitz, eds.), Kluwer, p. 243*
1996. `
..19.3,13.0: intercomponent transfer in large eddies only*
LINDBORG, E.*
On Kolmogorov's third order structure function law, the local isotropy hypothesis and the pressure-velocity correlation*
Advances in Turbulence 6 (ETC  Lausanne), (S. Gavrilakis, L. Machiels, and P.  Monkewitz, eds.), Kluwer, p. 247*
1996. `
..19.3: better alignment with intermediate rate at hi Re*
OOI, A.; CHONG, M.S.; SORIA, J.*
Reynolds number dependence of the vorticity alignment with the three principal rates of strain*
Advances in Turbulence 6 (ETC  Lausanne), (S. Gavrilakis, L. Machiels, and P.  Monkewitz, eds.), Kluwer, p. 255*
1996. `
..19.3,61.0,31.1: rotating disks up to Re, lambda = 3200. Helium. Miniature hot wire*
WILLAIME, H.; ET AL.*
High Reynolds number experiment - transition and structures*
Advances in Turbulence 6 (ETC  Lausanne), (S. Gavrilakis, L. Machiels, and P.  Monkewitz, eds.), Kluwer, p. 271*
1996. `
..19.3: Mexican hat identifies inflections. See Proc. Roy Soc. A 447, 341*
NICOLLEAU, F.; VASSILICOS, J.C.*
Wavelet analysis of high-resolution turbulence data*
Advances in Turbulence 6 (ETC Lausanne), (S. Gavrilakis, L. Machiels, and P. Monkewitz, eds.), Kluwer, p. 279*
1996. `
 ..13.0,19.3: special case - do not need to measure p*
SJOGREN, T.I.A.; JOHANSSON, A.V.*
Measurement of pressure-strain through two-point velocity correlations in homogeneous axisymmetric turbulence*
Advances in Turbulence 6 (ETC Lausanne), (S. Gavrilakis, L. Machiels, and P. Monkewitz, eds.), Kluwer, p. 491*
1996. `
..19.3,13.0: homo. diss. well correlated. Full, and iso., diss. less so.*
ZHU, Y.; ANTONIA, R.A.*
Correlation between the enstrophy and the energy dissipation rate in a turbulent wake*
Advances in Turbulence 6 (ETC  Lausanne), (S. Gavrilakis, L. Machiels, and P.  Monkewitz, eds.), Kluwer, p. 507*
1996. `
....19.1: Makita active (flapping) grid. Well-defined transition to high-Re spectrum shape at microscale Re between 100 and 200*
MYDLARSKI, L.; WARHAFT, Z.*
Experiments on the Reynolds number dependence of grid generated turbulence*
Engg Turb. Modelling and Expt. 3 (W. Rodi and G. Bergeles, eds.), Elsevier, p. 581*
1996. `
..46.0,19.2: Q,R plots etc.*
HUSER, A.; BIRINGEN, S.*
Simulation of turbulent square-duct flow - dissipation and small-scale motion*
AIAA J. 34, 2509*
1996. `
..18.1,19.2: development of Yoshizawa 2-scale DIA. Relies mainly on homo. strain DNS*
HAMBA, F.*
Modeling of inhomogeneous compressible turbulence using a two-scale statistical theory*
NASA Ames/Stanford Center for Turbulence Research Annual Research Briefs, p. 53*
1996. `
..62.0: 19.3mm jets in 70mm walls 406mm apart. Normal stresses only*
FERNANDES, R.L.J.; SOBIESIAK, A.; POLLARD, A.*
Opposed round jets issuing into a small aspect ratio channel cross flow*
Exptl. Thermal and Fluid Sci. 13, 374*
1996. `
..19.2,20.0: du/dy has higher flatness factor than dv/dx, "therefore more intermittent". Re_lambda 60 to 250*
SHAFI, H.S.; ZHU, Y.; ANTONIA, R.A.*
Statistics of du/dy in a turbulent wake (?)*
Fluid Dyn. Res. 19. 169*
1997. `
..19.2,21.2: high-k intermittency. Circular jet at microscale Re up to 300*
CAMUSSI, R.; BARBAGALLO, D.*
Experimental analysis of transverse intermittency in a turbulent jet flow*
Expts. in Fluids 22, 268*
1997. `
..12.2,19.3: appears to demolish it*
NAGANO, Y.; ITAZU, Y.*
Renormalization group theory for turbulence assessment of the Yakhot-Orszag-Smith theory*
Proceedings, Int'l Sympo. on Math. Modelling of Turbulent Flows, Tokyo, (H. Daiguji and Y. Mitake, eds.), Japan Soc. of CFD, 1995. Fluid Dynamics Research 20, 157*
1997. `
..19.2: tube-like - identified by second invariant of velocity gradient tensor. See Lyngby IUTAM mtg*
TANAHASHI, M.; MIYAUCHI, T.; IKEDA, J.*
Scaling law of coherent fine scale structure in homogeneous isotropic turbulence*
Presented at the Eleventh Sympo. on Turbulent Shear Flows, Grenoble, paper 4-17*
1997. `
..19.2: K. slightly generalized. 1949 Yaglom paper in DAN*
ANTONIA, R.A.; ET AL.*
Analogy between predictions of Kolmogorov and Yaglom*
J. Fluid Mech. 332, 395*
1997. `
..19.3: anisotropy increases with wave number - but microscale Re only about 30*
SHEBALIN, J.V.; WOODRUFF, S.L.*
Kolmogorov flow in three dimensions*
Phys. Fluids 9, 164*
1997. `
..19.3,25.7: eigenvalues of strain tensor and pressure Hessian - viscous analog to Euler work*
ANDREOTTI, B.*
Studying Burgers' models to investigate the physical meaning of the alignments statistically observed in turbulence*
Phys Fluids 9, 735*
1997. `
..19.2: expt. in jet verifies "recurrence relation" with nonlinear exponent - She, Phys. Rev. Lett. 72, 336, 1994*
CAMUSSI, R.; BENZI, R.*
Hierarchy of transverse structure functions*
Phys. Fluids 9, 257*
1997. `
..19.2: 300 cubed DNS - deviations from K-41*
BORATIAV, O.N.; PELZ, R.B.*
Structures and structure functions in the inertial range of turbulence*
Phys. Fluids 9, 1400*
1997. `
..19.2: scaling exponents etc. - as small departures from Kolmogorov theory*
SREENIVASAN, K.R.; ANTONIA, R.A.*
The phenomenalogy of small-scale turbulence*
Ann. Rev. Fluid Mech. 29, 435*
1997. `
..54.0,19.2: review and model for derivative skewness. Parameter is "micro-Ro", ratio of rms vorticity to meas, surprise*
CAMBON, C.; MANSOUR, N.N.; GODEFERD, F.S.*
Energy transfer in rotating turbulence*
J. Fluid Mech. 337, 303*
1997. `
..19.2: tube-like - identified by second invariant of velocity gradient tensor. See TSF 11, Grenoble*
TANAHASHI, M.; MIYAUCHI, T.; IKEDA, J.*
Identification of coherent fine scale structure in turbulence*
Presented at IUTAM Sympo. on Simulation and Identification of Organized Structures in Flows, Lyngby*
1997. `
..19.5: numerical problems in "shocks"*
ZHANG, D.S.; ET AL.*
Burgers' equation with high Reynolds number*
Phys. Fluids 9, 1853*
1997. `
..12.1,19.2: DNS of isotropic turbulence (Southerland)*
FREDERIKSEN, R.D.; DAHM, W.J.A.; DOWLING, D.R.*
Experimental assessment of fractal scale similarity in turbulent flows. Part 2. Higher-dimensional intersections and non-fractal inclusions*
J. Fluid Mech. 338, 89*
1997. `
..12.1,19.2: parts I and II are 327, 35 and 338, 89*
FREDERIKSEN, R.D.; DAHM, W.J.A.; DOWLING, D.R.*
Experimental assessment of fractal scale similarity in turbulent flows. Part 3. Multifractal scaling*
J. Fluid Mech. 338, 127*
1997. `
..19.2,32.2: apparently very good accuracy and repeatability*
NOULLEZ, A.; ET AL.*
Transverse velocity increments in turbulent flow using the relief technique*
J. Fluid Mech. 339, 287*
1997. `
..59.2,54.0,19.2: trailing vortex pair in atmosphere, or model of vortex stretching*
RISSO, F.; CORJON, A.; STOESSEL, A.*
Direct numerical simulations of wake vortices in intense homogeneous turbulence*
AIAA J. 35, 1030*
1997. `
..60.0,19.3: TKE amplification tends to saturate above M_1 = 3, for M_t approx. 0.1. Most length scales tend to decrease*
LEE, S; LELE, S.K.; MOIN, P.*
Interaction of isotropic turbulence with shock waves - effect of shock strength*
J. Fluid Mech. 340, 225*
1997. `
..07.0,19.2: various topics, mainly the limit of NS as viscosity tends to zero. See earlier papers*
BARENBLATT, G.I.; CHORIN, A.J.*
New perspectives in turbulence - scaling laws, asymptotic, and intermittency*
Univ. of CA, Berkeley, PAM-701*
1997. `
..19.3: analytic and simulations - intermediate "asymptotic" states*
CHASNOV. J.R.*
On the decay of inhomogeneous turbulence*
J. Fluid Mech. 342, 335*
1997. `
..11.1,19.2: Pr = 3,5,7 - homogeneous isotropic flow. Re_lambda 25 - 77 but Kolmogorov/Batchelor scaling works*
BOGUCKI, D.; DOMARADZKI, J.A.; YEUNG, P.K.*
Direct numerical simulations of passive scalars with Pr>1 advected by turbulent flow*
J. Fluid Mech. 343, 111*
1997. `
..19.5: random solutions in the limit of vanishing viscosity. Frisch group*
GURBATOV, S.N.; ET AL.*
On the decay of Burgers turbulence*
J. Fluid Mech. 344, 339*
1997. `
..19.2: marginally better data fit than Kolmogorov*
OULD-ROUIS, M.; ET AL.*
Relation between third-order and second-order velocity structure functions for axisymmetric turbulence*
Presented at 11th Sympo. on Turbulent Shear Flows, Grenoble, Paper 4-7*
1997. `
..19.2,25.6: using DNS to check on high-k rescaling*
MCCOMB, W.D.; ET AL.*
Investigation of renormalization group methods for the numerical simulation of isotropic turbulence*
Presented at 11th Sympo. on Turbulent Shear Flows, Grenoble, Paper 4-23*
1997. `
..19.2: k goes as x^-1.25, mean square vorticity as x^-2 not -2.25*
ZHU, Y.; AHOU, T.; ANTONIA, R.A.*
Vorticity measurements in a turbulent grid flow*
Presented at 11th Sympo. on Turbulent Shear Flows, Grenoble, Paper 10-16*
1997. `
..19.4:  integro-differential equations for response functions*
KIDA, S.; GOTO, S.*
A Lagrangian direct-interaction approximation for homogeneous isotropic turbulence*
J. Fluid Mech. 345, 307*
1997. `
..28.1,19.2:  high-wave-number intermittency.  Universal properties down to microscale Reynolds number of 10*
CAMUSSI, R.; GUJ, G.*
Orthonormal wavelet decomposition of turbulent flows - intermittency and coherent structures*
J. Fluid Mech. 348, 177*
1997. `
..19.2,12.1:  BL disturbed by vertical cylinder.  One decade of local isotropy for timescale ratio not more than 0.01*
SADDOUGHI, S.G.*
Local isotropy in complex turbulent boundary layers at high Reynolds number*
J. Fluid Mech. 348, 201*
1997. `
..19.2,12.1,31.1:  three triple hot wires.  Mom. thickness Re = 2790 so some advantage over DNS*
HONKAN, A.; ANDREOPOULOS, Y.*
Vorticity, strain-rate and dissipation characteristics in the near-wall region of turbulent boundary layers*
J. Fluid Mech. 350, 29*
1997. `
..19.2:  from Aachen thesis*
OBERLACK, M.*
Non-isotropic dissipation in non-homogeneous turbulence*
J. Fluid Mech. 350, 351*
1997. `
..28.1,19.2:  stands for Peak-Valley-Counting, to give the (longitudinal) microscale.  No good for dissipation itself in anisotropic flows*
HO, C.-H.; ZOHAR, Y.*
The PVC technique - a method to estimate the dissipation length scale in turbulent flows*
J. Fluid Mech. 352, 135*
1997. `
..19.1,18.2:  M up to 0.7.  Decay index first decreases (below 1) then increases*
ZWART, P.J.; BUDWIG, R.; TAVOULARIS, S.*
Grid turbulence in compressible flow*
Expts. in Fluids 23, 520*
1997. `
..19.2:  question of whether you have to assume local isotropy to prove the results.  Answer generally no*
HILL, R.J.*
Applicability of Kolmogorov's and Monin's equations of turbulence*
J. Fluid Mech. 353, 67*
1997. `
..24.7,19.2:  heavy math leading to asymptotic solutions*
KAWAHARA, G.; ET AL.*
Wrap, tilt and stretch of vorticity lines around a strong thin straight vortex tube in a simple shear flow*
J. Fluid Mech. 353, 115*
1997. `
..19.2: Lagrangian evolution of Q and R in Spalart boundary layer*
CHACIN, J.; CANTWELL, B.*
Study of turbulence structure using the invariants of the velocity gradient tensor*
Mech. Engg Dept., Stanford Univ., Rept. TF-70*
1997. `
..19.2:  experiments and DNS - dissipative scales approach isotropy when mean shear small*
ANTONIA, R.A.; ZHOU, T.; ROMANO, G.P.*
Second- and third-order longitudinal velocity structure functions in a fully developed turbulent channel flow*
Phys. Fluids 9, 3465*
1997. `
..19.1,44.2,30.2:  when spacing is small, turbulence becomes 2D.  Relevance to honeycombs*
GRAHAM, J.M.R.*
The effect of a two-dimensional cascade of thin streamwise plates on homogeneous turbulence*
J. Fluid Mech. 356, 125*
1998. `
..54.0,19.3:  T-P theorem applies only to statistically-stationary (non-decaying) flow (?if that?)*
SPEZIALE, C.G.*
On rotating isotropic turbulence and the Taylor-Proudman theorem in an inertial frame*
Boston Univ. TR AM-98-012*
1998. `
..11.3,19.1:  experiments in air - microscale Pe up to 512.  Structure functions depend less on Re (or Pe) than for velocity field*
MYDLARSKI, L.; WARHAFT, Z.*
Passive scalar statistics in high-Peclet-number grid turbulence*
J. Fluid Mech. 358, 135*
1998. `
..53.0,19.1:  "substantial", even for S-bend with strain-rate ratio as small as 1/20*
CHEBBI, B.; HOLLOWAY, A.G.L.; TAVOULARIS, S.*
The response of sheared turbulence to changes in curvature*
J. Fluid Mech. 358, 223*
1998. `
..19.2: 35-page review*
ZHOU, Y.; SPEZIALE, C.G.*
Advances in the fundamental aspects of turbulence - energy transfer, interacting scales, and self-preservation in isotropic decay*
Appl. Mech. Rev. 51, 267*
1998. `
..01.2,19.2,11.6:  "combustion disc" impinging jet pair.  Scalar fluctuations and their dissipation strongly correlated*
SARDI, K.; TAYLOR, A.M.K.P.; WHITELAW, J.H.*
Conditional scalar dissipation statistics in a turbulent counterflow*
J. Fluid Mech. 361, 1*
1998. `
..19.2,43.2:  from neutrally-buoyant floats.  -2 frequency spectrum in inertial subrange 
LIEN, R.-C.; D'ASARO, E.A.; DAIRIKI, G.T.*
Lagrangian frequency spectra of vertical velocity and vorticity in high-Reynolds-number oceanic turbulence*
J. Fluid Mech. 362, 177*
1998. `
..18.1,19.2:  DNS with rms M=0.5.  No direct comparison with incompressible flow*
PORTER, D.H.; WOODWARD, P.R.; POUQUET, A.*
Inertial range structures in decaying compressible turbulent flows*
Phys. Fluids 10, 237*
1998. `
..19.2,13.0:  kurtosis of vorticity exceeds kurtosis of strain rate by 4/15 if 4th order velocity moments are quasi-normal - even if dissipation = nu x enstrophy*
CHEN, H.; CHEN, S.*
Kinematic effects on local energy dissipation rate and local enstrophy in fluid turbulence*
Phys. Fluids 10, 312*
1998. `
..19.2:  ratio of integral scale to dissipation length scale decreases with microscale Re up to 100 and always depends on the large-scale structure/forcing*
SREENIVASAN, K.R.*
An update on the energy dissipation rate in isotropic turbulence*
Phys. Fluids 10, 528*
1998. `
..19.2:  approx.-homo. shear at microscale Re up to 390.  du/dy skewness goes as Re({-0.6}*
GARG, S.; WARHAFT, Z.*
On the small scale structure of simple shear flow*
Phys. Fluids 10, 662*
1998. `
..19.2:  HWA up to Re, lambda = 3000 (Modame tunnel)  Deep analysis of pdf's and cumulants of structure functions.  Relevance to high-k intermittency is distant*
KAHALERRAS, H.; ET AL.*
Intermittency and Reynolds number*
Phys. Fluids 10, 910*
1998. `
..25.6,19.2:  energy transfer through grid scale (from DNS) highly intermittent.  Scaling does not follow Kolmogorov*
CERUTTI, S.; MENEVEAU, C.*
Intermittency and relative scaling of subgrid-scale energy dissipation in isotropic turbulence*
Phys. Fluids 10, 928*
1998. `
..19.2,11.1:  at high Sc and low Re, Batchelor scaling applies only in special cases*
CHASNOV, J.R.*
The viscous-convective subrange in nonstationary turbulence*
Phys. Fluids 10, 1191*
1998. `
..19.3:  exact NS solution in confluent hypergeometric functions - planar jet in strain field*
ISHIHARA, T.; KANEDA, Y.*
Fine-scale structure of thin vortical layers*
J. Fluid Mech. 364, 297*
1998. `
..19.2,25.6:  recommends tensor eddy viscosity - SGS stress scales on <u_i,k u_j,k>*
BORUE, V.; ORSZAG, S.A.*
Local energy flux and subgrid-scale statistics in three-dimensional turbulence*
J. Fluid Mech. 366, 1*
1998. `
..19.2:  9-wire probe at mom.-thickness Re = 1070, for y^+ < 90 only*
ONG, L.; WALLACE, J.M.*
Joint probability density analysis of the structure and dynamics of the vorticity field of a turbulent boundary layer*
J. Fluid Mech. 367, 291*
1998. `
..07.0,19.2:  intermediate asymptotics - vel profile and Kolmogorov scaling*
BARENBLATT, G.I.; CHORIN A.J.*
New perspectives in turbulence - scaling laws, asymptotics, and intermittency*
SIAM Rev. 40, 265*
1998. `
..19.3:  continuation of J.J. et al. 1993.  Vortices have diameter of order Kolmogorov scale but vel. differences of order rms vel. - effectively Burgers vortices, probably unstable, negligible dissipation*
JIMENEZ, J.; WRAY, A.A.*
On the characteristics of vortex filaments in isotropic turbulence*
J. Fluid Mech. 373, 255*
1998. `
..19.2,31.1:  four cross-wire probes.  Mesh Re 20300.  Vorticity more nearly isotropic than velocities.  Discussion of spatial resolution*
ANTONIA, R.A.; ZHOU, T.; ZHU, Y.*
Three-component vorticity measurements in a turbulent grid flow*
J. Fluid Mech. 374, 29*
1998. `
..13.0,19.1:  pressure-strain terms from integrals of measured double and triple correlations.  Theory from Lindborg 1995*
SJOGREN, T.; JOHANSSON, A.V.*
Measurement and modelling of homogeneous axisymmetric turbulence*
J. Fluid Mech. 374, 59*
1998. `
..19.3:  if spectrum slope steeper than -1 (so low -k modes dominate)*
JIMENEZ, J.*
Turbulent velocity fluctuations need not be Gaussian*
J. Fluid Mech. 376, 139*
1998. `
..19.3:  final decay - would need a wind tunnel one light-year long*
CLARK, T.T.; ZEMACH, C.*
Symmetries and the approach to statistical equilibrium in isotropic turbulence*
Phys. Fluids 10, 2846*
1998. `
..11.3,19.1:  experiments at microscale Re from 200 to 500.  "Ramp-cliff" temperature fronts dominate statistics*
MYDLARSKI, L.; WARHAFT, Z.*
Three-point statistics and the anisotropy of a turbulent passive scalar*
Phys. Fluids 10, 2885*
1998. `
..54.0,19.3:  weakened spectral transfer leads to increase in TKE, k^-2 spectrum*
YEUNG, P.K.; ZHOU, Y.*
Numerical study of rotating turbulence with external forcing*
Phys. Fluids 10, 2895*
1998. `
..19.2,05.0:  i.e. departure of 2-point velocity differences from K41 theory*
ANTONIA, R.A.; ORLANDI, P.; ROMANO, G.P.*
Scaling of longitudinal velocity increments in a fully developed turbulent channel flow*
Phys. Fluids 10, 3239*
1998. `
..19.2: conditional analysis of DNS*
NOMURA, K.K.; POST, G.K.*
The structure and dynamics of vorticity and rate of strain in incompressible homogeneous turbulence*
J. Fluid Mech. 377, 65*
1998. `
..12.2,07.0,19.2:  vanishing-viscosity asymptotics for wall layer and structure functions - see also Meccanica 33,445 (1998)*
CHORIN, A.J.*
New perspectives in turbulence*
Quart. Appl. Math. 56,767*
1998. `
..19.2,06.0:  microscale Re about 230.  Large grid roughness, similar to Krogstad*
ANTONIA, R.A.; SHAFI, H.S.*
Small scale intermittency in a rough wall turbulent boundary layer*
Expts. in Fluids 26, 145*
1999. `
..19.2: Lagrangian tracing using DNS*
OOI, A.; ET AL.*
A study of the evolution and characteristics of the invariants of the velocity-gradient tensor in isotropic turbulence*
J. Fluid Mech. 381, 141*
1999. `
..19.2:  defined in terms of wavelet coefficients.  Big differences in pdf between "intermittent" and "non-intermittent" regions*
GUJ, G.; CAMUSSI, R.*
Statistical analysis of local turbulent energy fluctuations*
J. Fluid Mech. 382, 1*
1999. `
..19.2:  meaning the coefficient 4/5 of the third-order structure function, and the streamwise variation of mean dissipation*
LINDBORG, E.*
Correction to the four-fifths law due to variations of the dissipation*
Phys. Fluids 11, 510*
1999. `
19.3:  acceleration variance normalized by Kolmogorov variables is not constant but goes as Re_lambda^1/2.  Larger-scale pressure gradients are blamed*
VEDULA, P.; YEUNG, P.K.*
Similarity scaling of acceleration and pressure statistics in numerical simulations of isotropic turbulence*
Phys. Fluids 11, 1208*
1999. `
..19.3,05.0:  Kolmogorov similarity observed over wider range of scales if third-order structure function is used to normalize instead of r. Examples down to y+ = 31*
BENZI, R.; ET AL.*
Intermittency and scaling laws for wall bounded turbulence*
Phys. Fluids 11, 1284*
1999. `
..19.2:  tubular. Homo. DNS at microscale Re up to 90*
TANAHASHI, M.; MIYAUCHI, T.; IKEDA, J.*
Identification of coherent fine scale structure in turbulence*
Proceedings, IUTAM Symposium on Simulation and Identification of Organized Structures in Flows, p. 131 (J.N. Sorensen, E.J. Hopfinger and N. Aubry, Eds.), Kluwer *
1999. `
..19.2:  measurements in grid turbulence and jet - analysis in terms of multifractals*
VAN DE WATER, W.; HERWEIJER, J.A.*
High-order structure functions of turbulence*
J. Fluid Mech. 387, 3*
1999. `
..19.2,25.6;  experiments on "compressed" grid turbulence*
LIU, S.; KATZ, J.; MENEVEAU, C.*
Evolution and modelling of subgrid scales during rapid straining of turbulence*
J. Fluid Mech. 387, 281*
1999. `
..19.2: or the pressure spectrum misbehaves (most of August issue is Kraichnan 70th birthday sympo.)*
NELKIN, M.*
Enstrophy and  dissipation must have the same scaling exponent in the high Reynolds number limit of fluid turbulence*
Phys. Fluids 11, 2202*
1999. `
..19.2:  self-similar cascade imeni Kolmogorov perturbed by noise of slightly larger scale.  Basic questions are raised*
JIMENEZ, J.*
Coherence in the turbulent cascade*
NASA Ames/Stanford Center for Turbulence Research, Annual Research Briefs, p. 215*
1999. `
..11.1,19.2:  departures from local isotropy attributed to decay*
DANAILA, L.; ET AL.*
A generalization of Yaglom's equation which accounts for the large-scale forcing in heated decaying turbulence*
J. Fluid Mech. 391, 359*
1999. `
..54.0,19.2:  various oscillatory axial strains.  Survival if oscillation frequency small compared to strain rate*
VERZICCO, R.; JIMENEZ, J.*
On the survival of strong vortex filaments in 'model' turbulence*
J. Fluid Mech. 394, 261*
1999. `
..19.2,23.0:  pressure-gradient variance, in Kolmogorov scaling, varies as (microscale Re)^(1/2)*
GOTOH, T.; ROGALLO, R.S.*
Intermittency and scaling of pressure at small scales in forced isotropic turbulence*
J. Fluid Mech. 396, 257*
1999. `
..19.2:  "shear-stress fluctuation" less intermittent than dissipation*
TSUJI, Y.; DHRUVA, B.*
Intermittency feature of shear stress fluctuation in high-Reynolds-number turbulence*
Phys. Fluids 11, 3017*
1999. `
..19.2:  neat vector analysis*
RASMUSSEN, H.O.*
A new proof of Kolmogorov's 4/5-law*
Phys. Fluids 11, 3495*
1999. `
..14.0,19.3:  replaces transport equation for anisotropy tensor by three equations for invariants (not I, II, III)*
JONGEN, T.; GATSKI, T.B.*
A unified analysis of planar homogeneous turbulence using single-point closure equations*
J. Fluid Mech. 399, 117*
1999. `
..19.2:  Forced DNS and LES up to 512^3 points.  Pr 0.7 or 1.0.  Scalar field is more intermittent at high k than velocity field. Pt. 1 is JFM 309, 113 (1996)*
WANG, L.-P.; CHEN, S.; BRASSEUR, J.G.*
Examination of hypotheses in the Kolmogorov refined turbulence theory through high-resolution simulations.  Part 2.  Passive scalar field*
J. Fluid Mech. 163, 163*
1999. `
..19.3,54.0:  rotating but not specifically geophysical - initially isotropic turbulence reduces to longitudinal vortices.  "Coherent-vortex" analysis*
MCWILLIAMS, J.C.; WEISS, J.B.; YAVNEH, I.*
The vortices of homogeneous geostrophic turbulence*
J. Fluid Mech. 401, 1*
1999. `
..19.2,42.3:  from Kelvin-Helmholtz instability.  DNS - main interest is in coefficients of theoretical scalar spectra*
SMYTH, W.D.*
Dissipation-range geometry and scalar spectra in sheared stratified turbulence*
J. Fluid Mech. 401, 209*
1999. `
..19.3,25.6:  EDQNM etc.*
LESIEUR, M.; ET AL.*
From two-point closures of isotropic turbulence to LES of shear flows*
Flow, Turb. and Comb. 63, 247*
1999. `
..19.2:  "near-asymptotics" analysis.  Spectrum k^(-5/3+mu) where mu goes to zero at high Re (no connection with the structure-function mu)*
GAMARD, S.; GEORGE, W.K.*
Reynolds number dependence of energy spectra in the overlap region of isotropic turbulence*
Flow, Turb. and Comb. 63, 443*
1999. `
..13.0,19.2:  exact equation for dissipation covariance*
HAYOT, F.; JAYAPRAKASH, C.*
Relations between intermittency and structure function exponents in turbulence*
Phys. Fluids 12, 327*
2000. `
..13.0,19.1,11.2:  experiments to find power laws of decay.*
ZHOU, T.; ET AL.*
Transport equations for the mean energy and temperature dissipation rates in grid turbulence*
Expts. in Fluids 28, 143*
2000. `
..19.2,43.1:  "unexpected non-Gaussian character"*
ALISSE, J.-R.; SIDI, C.*
Experimental probability density functions of small-scale fluctuations in the stably stratified atmosphere*
J. Fluid Mech. 402, 137*
2000. `
..25.6,19.2:  forcing to give large inertial subrange. Microscale Re up to 516 with 256^3 points*
ALVELIUS, K.; JOHANSSON, A.V.*
LES computations and comparison with Kolmogorov theory for two-point pressure-velocity correlations and structure functions for globally anisotropic turbulence*
J. Fluid Mech. 403, 23*
2000. `
..04.0,19.2:Spalart DNS - invariants of velocity-gradient tensor*
CHACIN, J.M.; CANTWELL, B.J.*
Dynamics of a low Reynolds number turbulent boundary layer*
J. Fluid Mech. 404, 47*
2000. `
..19.2:  transverse vorticity probe for microscale Re up to 100.  Spectra agree with "isotropic" relations to within +/- 10% (large scales are more anisotropic in grid turbulence).  Need different moment-scaling exponents for strain rate and vorticity?*
ZHOU, T.; ANTONIA, R.A.*
Reynolds number dependence of the small-scale structure of grid turbulence*
J. Fluid Mech. 406, 81*
2000. `
..19.3,25.6:  DNS at microscale Re = 110.  Long-range interactions in k-space all low-intensity "forward scatter".  Local interactions can produce intense scatter in either direction, localized in physical space*
AKHAVAN, R.; ET AL.*
Subgrid-scale interactions in a numerically simulated planar turbulent jet and implications for modelling*
J. Fluid Mech. 408, 83*
2000. `
..19.2:  not exclusively turbulence.  Non-local interaction may be non-universal.  Multiplicative theory of cascades is kinematics, not dynamics*
JIMENEZ, J.*
Intermittency and cascades*
J. Fluid Mech. 409, 99*
2000. `
..19.2,32.2:  experiments using "collective light scattering" (CLS) to measure refractive-index (density) fluctuations at given wave number by light scattering from gas molecules*
HONORE, C.; GRESILLON, D.*
Turbulence cascade and dynamical exchange between spatial scales*
J. Fluid Mech. 411, 187*
2000. `
..19.1:  triple-wire meas.  Mesh Re up to 35000. Isotropy checked by measurements of vw, etc.*
TRESSO, R.; MUNOZ, D.R.*
Homogeneous, isotropic flow in grid generated turbulence*
J. Fluids Engg 122, 51*
2000. `
..12.2,19.2:  "predominant misalignment" of vorticity vector w.r.t. principal axes of strain rate.  See 941 and 1166*
NOMURA, K.K.; DIAMESSIS, P.J.*
The interaction of vorticity and rate-of-strain in homogeneous sheared turbulence*
Phys. Fluids 12, 846*
2000. `
..19.2,25.6:  square duct.  Filtered vorticity aligns with intermediate strain-rate eigendirection.  Relevant to SGS modeling.  See 846 and 1166*
TAO, B.; KATZ, J.; MENEVEAU, C.*
Geometry and scale relationships in high Reynolds number turbulence determined from three-dimensional holographic velocimetry*
Phys. Fluids 12, 941*
2000. `
..19.2,25.6:  measurements with quad. x-probes (allowing cross-stream spatial filtering too).  Relevant to SGS modeling*
CERUTTI, S.; MENEVEAU, C.*
Statistics of filtered velocity in grid and wake turbulence*
Phys. Fluids 12, 1143*
2000. `
..19.2:  directional preferences.  See 846 and 941*
DIAMESSIS, P.J.; NOMURA, K.K.*
Interaction of vorticity, rate-of-strain, and scalar gradient in stratified homogeneous sheared turbulence*
Phys. Fluids 12, 1166*
2000. `
..42.3,24.1,19.2:  dissipation range appears to become isotropic for buoyancy Re of order 10^5 defined as (dissipation)/nu N^2*
SMYTH, W.D.; MOUM, J.N.*
Anisotropy of turbulence in stably stratified mixing layers*
Phys. Fluids 12, 1343*
2000. `
..23.0,19.2:  obvious but neat - tail of pressure pdf is exponential, varying more rapidly with Re than rms p (possible internal intermittency)*
LA PORTA, A.; ET AL.*
Using cavitation to measure statistics of low-pressure events in large-Reynolds-number turbulence*
Phys. Fluids 12, 1485*
2000. `
..19.1,30.2,44.2:  grid turbulence passes through thick streamwise plates, so mixing is increased*
GUILLAUME, D.W.; LA RUE, J.C.*
Temporal and spatial unmixedness downstream of a plate array*
Phys. Fluids 12, 1497*
2000. `
..19.2:  scaling exponents increase with Re, lambda (max. 500)*
ANTONIA. R.A.; ZHOU, T.; XU, G.*
Second-order temperature and velocity structure functions - Reynolds number dependence*
Phys. Fluids 12, 1509*
2000. `
..11.1,19.2:  reverse spectral transfer due to very-high-k velocity modes may be important at high Sc*
YEUNG, P.K.; SYKES, M.C.; VEDULA, P.*
Direct numerical simulation of differential diffusion with Schmidt numbers up to 4.0*
Phys. Fluids 12, 1601*
2000. `
..19.2,23.0:  DNS results*
BIFERALE, L.; GUALTIERI, P.; TOSCHI, F.*
Statistics of pressure and of pressure-velocity correlations in isotropic turbulence*
Phys. Fluids 12, 1836*
2000. `
..19.3:  body force is delta function(s) in time, with arbitrary spatial distribution - usually deterministic and periodic*
BEE, J.; FRISCH, U.; KHANIN, K.*
Kicked Burgers turbulence*
J. Fluid Mech. 416, 239*
2000. `
..19.5:  inviscid, with white noise as initial condition*
FRACHEBOURG, L.; MARTIN, PH. A.*
Exact statistical properties of the Burgers equation*
J. Fluid Mech. 417, 323*
2000. `
..28.1,19.2:  special attention to velocity-gradient tensor and other alternatives to Reynolds decomposition*
ADRIAN, R.J.; CHRISTENSEN, K.T.; LIU, Z.-C.*
Analysis and interpretation of instantaneous turbulent velocity fields*
Expts. in Fluids 29, 275*
2000. `
..19.2,31.1:  4 x-probes to measure dissipation spectrum - results "support general trends of classical two-point closures"*
CERUTTI, S.; MENEVEAU, C.; KNIO, O.M.*
Spectral and hyper eddy viscosity in high-Reynolds-number turbulence*
J. Fluid Mech. 421, 307*
2000. `
..19.2:  axisymmetric version of Monin's equation for isotropic turbulence ("electronic journal" at jot.iop.org)*
ANSELMET, F.; ANTONIA, R.A.; OULD-ROUIS, M.*
Relations between third-order and second-order structure functions for axisymmetric turbulence*
J. Turbulence 1, paper 003*
2000. `
..19.2:  L's invariant not quite conserved but variation negligible ("electronic journal" at jot.iop.org)*
DAVIDSON, P.A.*
Was Loitsyansky correct?  A review of the arguments*
J. Turbulence 1, paper 006*
2000. `
..11.1,19.2:  significant skewness of dT'/dy in a shear flow - theoretical model compared with Tavoularis (JFM 104,349,1981)*
GONZALEZ, M.*
Study of the anisotropy of a passive scalar field at the level of dissipation*
Phys. Fluids 12, 2302*
2000. `
..19.2:  longl. derivative skewness increases with Re for microscale Re between 140 and 660 - but transverse skewness decreases*
FERCHICHI, M.; TAVOULARIS, S.*
Reynolds number effects on the fine structure of uniformly sheared turbulence*
Phys. Fluids 12, 2942*
2000. `
..19.2:  "active grid" and shear-generating screen.  du'/dy skewness goes as (Re_lambda)^-0.5 but 7th moment increases with Re*
SHEN, X.; WARHAFT, Z.*
The anisotropy of the small scale structure in high Reynolds number (Re_lambda~1000) turbulent shear flow*
Phys. Fluids 12, 2976*
2000. `
..19.2:  scaling exponents (in r-power laws for powers of velocity differences u(x+r)-u(x)) increase with Re*
ANTONIA, R.A.; PEARSON, B.R.; ZHOU, T.*
Reynolds number dependence of second-order velocity structure functions*
Phys. Fluids 12, 3000*
2000. `
..11.1,19.2:  microscale Re < 80 so "constant" still increasing with Re*
WEINMAN, K.A.; KLIMENKO, A.Y.*
Estimation of the Kolmogorov constant C_theta by direct numerical simulation of a continuous scalar*
Phys. Fluids 12, 3205*
2000. `

..13.0,19.4,18.1: eddy vis., with transport equations for TKE, dissipation and density variance derived from Yoshizawa Direct Interaction model. No details*
DURANTII, S.; PITTALUGA, F.*
Navier-Stokes prediction of internal flows with a three-equation turbulence model*
AIAA J. 38, 1098*
2000. `
..19.2,43.1:  i.e. relations between n th and (n+1)th order.  Here n=3 and the relation involves velocity/pressure-gradient structure functions. Tested in atmos. surface layer*
HILL, R.J.; BORATAV, O.N.*
Next-order structure-function equations*
Phys. Fluids 13, 276*
2001. `
..19.2,11.1:  blob of scalar with radius corresponding to a wavelength in the inertial range is converted into sheets with a k^-1 spectrum at times "appreciably smaller" than Kolmogorov cascade time*
VILLERMAUX, E.; INNOCENTI, C.; DUPLAT, J.*
Short circuits in the Corrsin-Obukhov cascade*
Phys. Fluids 13, 284*
2001. `
..19.2,43.1:  z=10 m, slightly-unstable ABL over 20 cm high grass.  All 9 derivatives with 20-hot-wire probe*
KHOLMYANSKY, M.; TSINOBER, A.; YORISH, S.*
Velocity derivatives in the atmospheric surface layer at Re_lambda=10^4*
Phys. Fluids 13, 311*
2001. `
..19.2: just so - NOAA work. Refers to a 2001 Yakhot paper*
HILL, R.J.*
Equations for structure functions of all orders*
J. Fluid Mech. 434, 379*
2001. `
..19.1:  1980s results.  Highly non-linear, far from Rotta's model.  Tendency of plane distortion and axi. contraction/expansion to axisymmetry stronger than tendency to isotropy*
CHOI, K.-S.; LUMLEY, J.L.*
The return to isotropy of homogeneous turbulence*
J. Fluid Mech. 436, 59*
2001. `
..19.2,21.2:  significant - explains disagreement between previous results*
ROMANO, G.P.; ANTONIA, R.A.*
Longitudinal and transverse structure functions in a turbulent round jet -  effect of initial conditions and Reynolds number*
J. Fluid Mech. 436, 231*
2001. `
..18.2,19.1:  grid in shock tube.  Mach number fluctuations of order 0.02.  Reduction in decay exponent may be the result of compressibility in the initial mixing layers from the grid rods (open-area ratio 0.56 to 0.74)*
BRIASSULIS, G.; AGUI, J.H.; ANDREOPOULOS, Y.*
The structure of weakly compressible grid-generated turbulence*
J. Fluid Mech. 432, 219*
2001. `
..19.2,21.2:  12 million HWA velocity samples in a jet.  Longitudinal velocity increment is Markovian and leads to Fokker-Planck equation for its p.d.f.*
RENNER, C.; PEINKE, J.; FRIEDRICH, R.*
Experimental indications for Markov properties of small-scale turbulence*
J. Fluid Mech. 433, 383*
2001. `
..12.2,19.2:  Kolmogorov's equation relating second- and third-order moments, with extra terms to allow for diffusion*
DANAILA, L.; ET AL.*
Turbulent energy scale budget equations in a fully developed channel flow*
J. Fluid Mech. 430, 87*
2001. `
..19.2,12.1:  PIV in core of channel flow.  Series of "swirling motions" (spanwise vorticity) on lines at 12-13 deg. to the wall*
CHRISTENSEN, K.T.; ADRIAN, R.J.*
Statistical evidence of hairpin vortex packets in wall turbulence*
J. Fluid Mech. 431, 433*
2001. `
..43.1,25.6,19.2:  "competition between waves and turbulence".  LES forced by internal waves*
CARNEVALE, G.F.; BRISCOLINI, M.; ORLANDI, P.*
Buoyancy- to inertial-range transition in forced stratified turbulence*
J. Fluid Mech. 427, 205*
2001. `
..19.2,11.1:  scalar fluctuation has longer time scale than velocity - opposite sense to Eulerian frame.  Schmidt nos. between 1/8 and 1*
YEUNG, P.K.*
Lagrangian characteristics of turbulence and scalar transport in direct numerical simulations*
J. Fluid Mech. 427, 241*
2001. `
..19.2,12.1:  further analysis of H & A, JFM 350, 29 (1997).  All invariants of gradient tensors are highly intermittent*
ANDREOPOULOS, Y.; HONKAN, A.*
An experimental study of the dissipative and vortical motion in turbulent boundary layers*
J. Fluid Mech. 439, 131*
2001 .`
..19.2:  higher moments anisotropic*
SCHUMACHER, J.*
Derivative moments in stationary homogeneous shear turbulence*
J. Fluid Mech. 441, 109*
2001. `
..19.2,21.2:  high k.  Camussi jet data (e.g. EF 22, 268, 1997)*
NIKORA, V.; GORING, D.; CAMUSSI, R.*
Intermittency and interrelationships between turbulence scaling exponents - phase-randomization tests*
Phys. Fluids 13, 1404*
2001. `
..19.2:  5th-derivative skewness effectively independent of Re - trend in Ferchichi (PF 12, 2942, 2000) not significant*
WARHAFT, Z.; SHEN, X.*
Some comments on the small scale structure of turbulence at high Reynolds number*
Phys. Fluids 13, 1532*
2001. `
..11.1,19.2:  DNS results include no classical isotropy at small scales*
CELANI, A.; ET AL.*
Fronts in passive scalar turbulence*
Phys. Fluids 13, 1768*
2001. `
..19.2:  structure-function exponents converge only at separation much larger than eta, depending on Re. Experiments and DNS*
KERR, R.M.; MENEGUZZI, M.; GOTOH, T.*
An inertial range crossover in structure functions*
Phys. Fluids 13, 1985*
2001. `
..19.2:  DNS - neglecting local interactions in k-space leads to more high-k energy, intense vortices and stronger intermittency,  i.e. local interactions moderate the effect of nonlocal*
LAVAL, J-P.; DUBRULLE, B.; NAZARENKO, S.*
Nonlocality and intermittency in three-dimensional turbulence*
Phys. Fluids 13, 1995*
2001. `
..19.2:  moments increase with microscale Re in all regions of spectrum.  40 < Re < 4250 (atmospheric BL)*
PEARSON, B.R.; ANTONIA, R.A.*
Reynolds-number dependence of turbulent velocity and pressure increments*
J. Fluid Mech. 444, 343*
2001. `
..19.2,43.1:  atmos. BL data.  Skewnesses of scalar increments and derivatives are inherently anisotropic and not a useful test for isotropy*
KURIEN, S.; AIVALIS, K.G.; SREENIVASAN, K.R.*
Anisotropy of small-scale scalar turbulence*
J. Fluid Mech. 448, 279*
2001. `
..19.2:  incomplete similarity and no 1/k range*
MORRISON, J.F.; ET AL.*
Reynolds number dependence of streamwise velocity spectra in turbulent pipe flow*
Phys. Review Letters 88, 214501-1*
2002. `
..19.2,05.0:  "anisotropy parameter" in actually proportional to Re_lambda*
TSUJI, Y.
Large scale anisotropy and small scale universality over the rough wall turbulent boundary layers*
To appear in Phys. Fluids*
2002. `