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Phys. Today
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Jaeger, H.M.1
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5
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85035305333
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D. Howell, R. P. Behringer, and C. Veje, in Powders & Grains 97, edited by R. P. Behringer and J. T. Jenkins (Balkema, Rotterdam, 1997), pp. 337–340
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D. Howell, R. P. Behringer, and C. Veje, in Powders & Grains 97, edited by R. P. Behringer and J. T. Jenkins (Balkema, Rotterdam, 1997), pp. 337–340.
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7
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85035260556
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See, for example, the videos at http://www.phy.duke.edu/(Formula presented)dhowell/research.html and http://mrsec.uchicago.edu/granular
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See, for example, the videos at http://www.phy.duke.edu/(Formula presented)dhowell/research.html and http://mrsec.uchicago.edu/granular
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C.S. O’Hern, S.A. Langer, A.J. Liu, and S.R. Nagel, Phys. Rev. Lett. 86, 111 (2001).
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O’Hern, C.S.1
Langer, S.A.2
Liu, A.J.3
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85035278032
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D. W. Howell (private communication)
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D. W. Howell (private communication).
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R. Khosropour, J. Zirinsky, H.K. Pak, and R.P. Behringer, Phys. Rev. E 56, 4467 (1997).
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Khosropour, R.1
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85035260491
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A. Karion, Ph.D. thesis, California Institute of Technology, Pasadena, California, 2000 (unpublished)
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A. Karion, Ph.D. thesis, California Institute of Technology, Pasadena, California, 2000 (unpublished).
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18
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85035273133
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For some examples of 3D imaging of Couette flow with x-ray tomography, see http://mrsec.uchicago.edu/granular
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For some examples of 3D imaging of Couette flow with x-ray tomography, see http://mrsec.uchicago.edu/granular
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21
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85035306830
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M. Nakagawa, S. A. Altobelli, A. Caprihan, and E. Fukushima, in Powders & Grains 93, edited by C. Thornton (Balkema, Rotterdam, 1993), p. 383
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M. Nakagawa, S. A. Altobelli, A. Caprihan, and E. Fukushima, in Powders & Grains 93, edited by C. Thornton (Balkema, Rotterdam, 1993), p. 383.
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0000047591
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J.D. Seymour, A. Caprihan, S.A. Altobelli, and E. Fukushima, Phys. Rev. Lett. 84, 266 (2000).
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25
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85035263321
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2D Couette systems, sheared under constant volume conditions, rough particles such as pentagons may actually produce a velocity profile that is very well fit by a pure exponential. Dan Howell and Bob Behringer (private communication)
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In 2D Couette systems, sheared under constant volume conditions, rough particles such as pentagons may actually produce a velocity profile that is very well fit by a pure exponential. Dan Howell and Bob Behringer (private communication).
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27
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85035265463
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Note that the work of Losert et al. defines (Formula presented) as the outer edge of glued particle layer, while we define (Formula presented) as the inner edge of the glued particle layer. Thus, a Gaussian profile centered on (Formula presented) in our experiments, as seen for disordered materials, is equivalent to a Gaussian profile centered on (Formula presented) for the experiments of Losert et al
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Note that the work of Losert et al. defines (Formula presented) as the outer edge of glued particle layer, while we define (Formula presented) as the inner edge of the glued particle layer. Thus, a Gaussian profile centered on (Formula presented) in our experiments, as seen for disordered materials, is equivalent to a Gaussian profile centered on (Formula presented) for the experiments of Losert et al.
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32
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0022794814
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D. Bideau, A. Gervois, L. Oger, and J.-P. Toadec, J. Phys. (France) 47, 1697 (1986).
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