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Volumn 57, Issue 2, 1998, Pages 1962-1970

Structure and formation of a gel of colloidal disks

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EID: 85006406315     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.57.1962     Document Type: Article
Times cited : (196)

References (48)
  • 1
    • 0003625785 scopus 로고
    • North-Holland, Amsterdam, J. P. Hansen, D. Levesque, J. Zinn Justin
    • P. N. Pusey, in Liquids, Freezing and Glass Transition, edited by J. P. Hansen, D. Levesque, and J. Zinn Justin (North-Holland, Amsterdam, 1991), p. 765.
    • (1991) Liquids, Freezing and Glass Transition , pp. 765
    • Pusey, P.N.1
  • 4
    • 0003625785 scopus 로고
    • North-Holland, Amsterdam, J. P. Hansen, D. Levesque, J. Zinn Justin
    • D. Frenkel, in Liquids, Freezing and Glass Transition, edited by J. P. Hansen, D. Levesque, and J. Zinn Justin (North-Holland, Amsterdam, 1991), p. 689.
    • (1991) Liquids, Freezing and Glass Transition , pp. 689
    • Frenkel, D.1
  • 6
    • 85037225740 scopus 로고    scopus 로고
    • Laponite (RD) is manufactured by Laporte Absorbents, P.O. Box 2, Cheshire, UK
    • Laponite (RD) is manufactured by Laporte Absorbents, P.O. Box 2, Cheshire, UK.
  • 32
    • 85037234909 scopus 로고    scopus 로고
    • the limit [Formula Presented] the first factor on the rhs of Eq. (2) becomes equal to unity. In the limit of large [Formula Presented], Eq. (3) can be rewritten as an integral over the decaying Bessel function squared. This gives a constant divided by the remaining factor [Formula Presented]
    • In the limit H→0 the first factor on the rhs of Eq. (2) becomes equal to unity. In the limit of large q, Eq. (3) can be rewritten as an integral over the decaying Bessel function squared. This gives a constant divided by the remaining factor q2.
  • 38
    • 85037210861 scopus 로고    scopus 로고
    • We have divided all two-dimensional patterns by the last pattern recorded [Formula Presented] h), because (i) [Formula Presented] spans almost three orders of magnitude, which obscures small variations, (ii) uncertainties in the background level and local detector overload introduce additional inaccuracies when dividing [Formula Presented] by the form factor, (iii) a few days is well beyond the restoring time of the gel, thus the figure shows the relative deviation from the constant (relaxed) signal
    • We have divided all two-dimensional patterns by the last pattern recorded (T=50 h), because (i) Is(q) spans almost three orders of magnitude, which obscures small variations, (ii) uncertainties in the background level and local detector overload introduce additional inaccuracies when dividing Is(q) by the form factor, (iii) a few days is well beyond the restoring time of the gel, thus the figure shows the relative deviation from the constant (relaxed) signal.
  • 39
  • 41
    • 0004081849 scopus 로고
    • Elsevier, Amsterdam, L. Pietronero, E. Tosatti
    • D. W. Schaeffer and K. D.Keefer, in Fractals in Physics, edited by L. Pietronero and E. Tosatti (Elsevier, Amsterdam, 1986), p. 39.
    • (1986) Fractals in Physics , pp. 39
    • Schaeffer, D.W.1    D.Keefer, K.2
  • 43
  • 46
    • 0003995896 scopus 로고
    • North-Holland, Amsterdam, A. Aharony, J. Feder
    • E. Courtens, in Fractals in Physics, edited by A. Aharony and J. Feder (North-Holland, Amsterdam, 1989).
    • (1989) Fractals in Physics
    • Courtens, E.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.