a)Consider the case of a point test charge q moving with velocity u parallel to an infinitely long straight current. Let λ be the proper charge density of the positive ions and v be the drift velocity of the electrons in the wire. Calculate the charge density of the wire relative to the rest-frame of the test charge q. b) Prove that the force ˜f the test charge feels in its rest-frame corresponds exactly to the force f on it in the rest-frame of the wire, when force transformation formulas are employed.
a)Consider the case of a point test charge q moving with velocity u parallel to an...
a)Consider the case of a point test charge q moving with velocity u parallel to an infinitely long straight current (as in Section 7.7 of Rindler). Let λ be the proper charge density of the positive ions and v be the drift velocity of the electrons in the wire. Calculate the charge density of the wire relative to the rest-frame of the test charge q. b) Prove that the force ˜f the test charge feels in its rest-frame corresponds exactly...
Consider the case of a point test charge q moving with velocity u parallel to an infinitely long straight current (as in Section 7.7 of Rindler). Let λ be the proper charge density of the positive ions and v be the drift velocity of the electrons in the wire. Calculate the charge density of the wire relative to the rest-frame of the test charge q.
1. A particle with charge Q=+3nC and initial velocity enters a region with a uniform, constant electric field as shown in the figure. At which location would vou most expect to find the particle some time later, after it enters the electric field region? E-feid region a. Point A b. Point B C. Point C d. Point D Particle P Charge- a and velocity v 2. In the distribution of charge below, the uniform line of charge is 6cm long....
Consider a point charge q moving arbitrar ily along a trajectory described by vector function of time r (t). The velocity of the charge is thus V(t)- di,(t)/dt. Suppose Q and Q'represent points on the trajectory where the charge is at time t and was at an earlier time t'. Let R(t) F r,(t) be the vector from the charge to the fixed point P as shown in the figure of particle re volume element de r" a) Prove the...
Consider a point charge q moving arbitrar ily along a trajectory described by vector function of time r (t). The velocity of the charge is thus V(t)- di,(t)/dt. Suppose Q and Q'represent points on the trajectory where the charge is at time t and was at an earlier time t'. Let R(t) F r,(t) be the vector from the charge to the fixed point P as shown in the figure of particle re volume element de r" a) Prove the...
Consider a cylindrical capacitor like that shown in Fig. 24.6. Let d = rb − ra be the spacing between the inner and outer conductors. (a) Let the radii of the two conductors be only slightly different, so that d << ra. Show that the result derived in Example 24.4 (Section 24.1) for the capacitance of a cylindrical capacitor then reduces to Eq. (24.2), the equation for the capacitance of a parallel-plate capacitor, with A being the surface area of...