Superconducting Frame in Magnetic Field

A superconducting square rigid frame of mass m, inductance L, and side a is cooled down (in a magnetic field) to a temperature below the critical temperature. The frame is kept horizontal (parallel to the x-y plane) and constrained to move in the z direction in a non-uniform but constant

Figure 1.1

magnetic field described by a vector potential A = (-B₀ y, αxz, 0) and a uniform gravitational field given by the acceleration g. The thickness of the frame is much smaller than a (see Figure 1.1). Initially, the frame is at rest, with its center coinciding with the origin. Find the equations of motion of the frame and solve for the position of the frame as a function of time.

SOLUTION

Find the magnetic field from the vector potential

The magnetic flux Φ through the surface of the superconducting frame is constant (see Figure 1.2). Φ is composed of the flux from the external

Figure 1.2

magnetic field Φ_e and the flux Φ_i produced by the current I flowing in the frame:

At t = 0, z = 0 and Φ = Φ₀ = B₀a². At later times,

So for the current we have

The force on the frame due to the interaction with the magnetic field is given by the general formula

In this problem, due to the physical constraint, we need only the component in the z direction

Therefore, the equation of motion becomes

or

This equation describes oscillatory motion with  and the solution is

where

From the initial conditions z(0) = 0 and  we find that A = -z₀ and φ₀ = 0. The complete solution for the position of the frame along the z-axis at time t is

مواضيع ذات صلة

مصطلحات الفيزياء النووية

إزاحة حمراء REDSHIFT

المركبات النانوية (Nanocomposites)

مولد فان دي جراف الالكتروستاتي

التطويرات التقنية الحديثة في المعجلات الالكتروستاتية

معجلات الالكترونات الالكتروستاتية

معجلات الفان دي جراف الترادفية

الحد من زيادة الطاقة في معجل فان دي جراف

أنبوبة التعجيل قي معجلات الجسيمات من نوع فان دي جراف

ارتكاز معجل فان دي جراف

مبدأ تشغيل معجل الفان دي جراف

القضايا الأخلاقية المتعلقة بتكنولوجيا النانو