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Q7.53P

Page 349

The current in a long solenoid is increasing linearly with time, so the flux is proportional t:.ϕ=αtTwo voltmeters are connected to diametrically opposite points (A and B), together with resistors ( R1and R2), as shown in Fig. 7.55. What is the reading on each voltmeter? Assume that these are ideal voltmeters that draw negligible current (they have huge internal resistance), and that a voltmeter register --∫abE×dlbetween the terminals and through the meter. [Answer: V1=αR1/(R1+R2). Notice that V1≠V2, even though they are connected to the same points]

Q7.59P

Page 351

An infinite wire runs along the z axis; it carries a current I (z) that is a function ofz(but not of t ), and a charge density λ(t) that is a function of t (but not of z ).

(a) By examining the charge flowing into a segment dz in a time dt, show that dλ/dt=-di/dz. If we stipulate that λ(0)=0and I(0)=0, show that λ(t)=kt, I(z)=-kz, where k is a constant.

(b) Assume for a moment that the process is quasistatic, so the fields are given by Eqs. 2.9 and 5.38. Show that these are in fact the exact fields, by confirming that all four of Maxwell's equations are satisfied. (First do it in differential form, for the region s > 0, then in integral form for the appropriate Gaussian cylinder/Amperian loop straddling the axis.)

Q7.60P

Page 351

Question: Suppose j(r)is constant in time but ÒÏ(r,t)is not-conditions that

might prevail, for instance, during the charging of a capacitor.

(a) Show that the charge density at any particular point is a linear function of time:

ÒÏ(r,t)=ÒÏ(r,0)+ÒÏ(r,0)t

whereÒÏ(r,0)is the time derivative of at . [Hint: Use the continuity equation.]

This is not an electrostatic or magnetostatic configuration: nevertheless, rather surprisingly, both Coulomb's law (Eq. 2.8) and the Biot-Savart law (Eq. 5.42) hold, as you can confirm by showing that they satisfy Maxwell's equations. In particular:

(b) Show that

B(r)=μ04π∫J(r')×r^r2dτ'

obeys Ampere's law with Maxwell's displacement current term.

Q7P

Page 310

A metal bar of mass m slides frictionlessly on two parallel conducting rails a distance l apart (Fig. 7 .17). A resistor R is connected across the rails, and a uniform magnetic field B, pointing into the page, fills the entire region.


(a) If the bar moves to the right at speed V, what is the current in the resistor? In what direction does it flow?

(b) What is the magnetic force on the bar? In what direction?

(c) If the bar starts out with speedV0at time t=0, and is left to slide, what is its speed at a later time t?

(d) The initial kinetic energy of the bar was, of course,12mv2Check that the energy delivered to the resistor is exactly 12mv2.

Q8P

Page 311

A square loop of wire (side a) lies on a table, a distance s from a very long straight wire, which carries a current I, as shown in Fig. 7.18.

(a) Find the flux of B through the loop.

(b) If someone now pulls the loop directly away from the wire, at speed, V what emf is generated? In what direction (clockwise or counter clockwise) does the current flow?

(c) What if the loop is pulled to the right at speed V ?

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