APhO 2007, Теория — Задача 2B. Dielectric spheres inside an external electric field

Theoretical problem 2 · 3 т.

Условие

By immersing a number of small dielectric particles inside a fluid of low-viscosity, you can get the resulting system as a suspension. When an external electric field is applied on the system, the suspending dielectric particles will be polarized with electric dipole moments induced. Within a very short period of time, these polarized particles aggregate together through dipolar interactions so that the effective viscosity of the whole system enhances significantly (the resulting system can be approximately viewed as a solid). This type of phase transition is called “electrorheological effect”, and such a system is called “electrorheological fluid” correspondingly. Such an effect can be applied to fabricate braking devices in practice, since the response time of such a phase transition is shorter than conventional mechanism by several orders of magnitude. Through solving several problems in the following, you are given a simplified picture to understand the inherent mechanism of the electrorheological transition.

1.(1) When there are many identical dielectric spheres of radius aa immersed inside the fluid, we assume that the dipole moment of each sphere p⃗\vec{p}, is induced solely by the external field E⃗0\vec{E}_0, independent of any of the other spheres (Note: p⃗∥E⃗0\vec{p}\parallel\vec{E}_0).

When two identical small dielectric spheres exist inside the fluid and contact with each other, while the line connecting their centers makes an angle θ\theta with the external field direction (see Fig. 2-6), write the expression of the energy of dipole-dipole interaction between the two small contacting dielectric spheres, in terms of pp, aa and θ\theta. (Note: In your calculations each polarized dielectric sphere can be viewed as an electric dipole located at the center of the sphere) [0,5 т.]

Two touching grey spheres, each with an upward dipole arrow at its centre; the line joining the centres makes angle θ with the vertical; a long vertical arrow on the left labelled E0 shows the field direction.
Fig. 2-6
Three three-sphere configurations in a vertical field E0, all dipoles pointing up: (d) two spheres stacked vertically with a third touching both on the right, (e) three spheres in a vertical column, (f) three spheres in a horizontal row.
Fig. 2-8

1.(2) Calculate the dipole-dipole interaction energies for the three configurations shown in Fig. 2-7. [0,75 т.]

Three two-sphere configurations in a vertical field E0, all dipoles pointing up: (a) spheres stacked vertically, (b) spheres side by side horizontally, (c) the line of centres at 45° to the field.
Fig. 2-7

1.(3) Identify which configuration of the system is the most stable one. [0,25 т.]

(Note: In your calculations each polarized dielectric sphere can be viewed as an electric dipole located at the center of the sphere, and the energy of dipole-dipole interaction can be expressed in terms of pp and aa.)

2.(1) In the case that three identical spheres exist inside the fluid, based on the same assumption as in question 1,

calculate the dipole-dipole interaction energies for the three configurations shown in Fig. 2-8; [0,9 т.]

2.(2) identify which configuration of the system is the most stable one; [0,3 т.]

2.(3) identify which configuration of the system is the most unstable one. [0,3 т.]

(Note: In your calculations each polarized dielectric sphere can be viewed as an electric dipole located at the center of the sphere, and the energy of dipole-dipole interaction can be expressed in terms of pp and aa.)

Отговори

Решение


Оригинал в Архива: 2.pdf · официални решения: 2_sol.pdf