Sample-to-sample torque fluctuations in a system of coaxial randomly charged surfaces

被引:13
|
作者
Naji, Ali [1 ,2 ]
Sarabadani, Jalal [3 ]
Dean, David S. [4 ,5 ,6 ,7 ]
Podgornik, Rudolf [4 ,5 ,8 ,9 ]
机构
[1] Inst Res Fundamental Sci IPM, Sch Phys, Tehran 193955531, Iran
[2] Univ Cambridge, Ctr Math Sci, Dept Appl Math & Theoret Phys, Cambridge CB3 0WA, England
[3] Univ Isfahan, Dept Phys, Esfahan 81746, Iran
[4] Univ Toulouse, UPS, Lab Phys Theor IRSAMC, F-31062 Toulouse, France
[5] CNRS, F-31062 Toulouse, France
[6] Univ Bordeaux, F-33400 Talence, France
[7] CNRS, UMR 5798, LOMA, F-33400 Talence, France
[8] J Stefan Inst, Dept Theoret Phys, SI-1000 Ljubljana, Slovenia
[9] Univ Ljubljana, Fac Math & Phys, Dept Phys, SI-1000 Ljubljana, Slovenia
来源
EUROPEAN PHYSICAL JOURNAL E | 2012年 / 35卷 / 03期
关键词
POLYAMPHOLYTES; DISORDER; RANGE;
D O I
10.1140/epje/i2012-12024-y
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Polarizable randomly charged dielectric objects have been recently shown to exhibit long-range lateral and normal interaction forces even when they are effectively net-neutral. These forces stem from an interplay between the quenched statistics of random charges and the induced dielectric image charges. This type of interaction has recently been evoked to interpret measurements of Casimir forces in vacuo, where a precise analysis of such disorder-induced effects appears to be necessary. Here we consider the torque acting on a randomly charged dielectric surface (or a sphere) mounted on a central axle next to another randomly charged surface and show that although the resultant mean torque is zero, its sample-to-sample fluctuation exhibits a long-range behavior with the separation distance between the juxtaposed surfaces and that, in particular, its root-mean-square value scales with the total area of the surfaces. Therefore, the disorder-induced torque between two randomly charged surfaces is expected to be much more pronounced than the disorder-induced lateral force and may provide an effective way to determine possible disorder effects in experiments, in a manner that is independent of the usual normal force measurement.
引用
收藏
页数:7
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