Chapter 7: Q24P (page 327)
Find the self-inductance per unit length of a long solenoid, of radius R , carrying n turns per unit length.
Short Answer
The self-inductance per unit length of the solenoid is .
Chapter 7: Q24P (page 327)
Find the self-inductance per unit length of a long solenoid, of radius R , carrying n turns per unit length.
The self-inductance per unit length of the solenoid is .
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Get started for freeQuestion: The preceding problem was an artificial model for the charging capacitor, designed to avoid complications associated with the current spreading out over the surface of the plates. For a more realistic model, imagine thin wires that connect to the centers of the plates (Fig. 7.46a). Again, the current I is constant, the radius of the capacitor is a, and the separation of the plates is w << a. Assume that the current flows out over the plates in such a way that the surface charge is uniform, at any given time, and is zero at t = 0.
(a) Find the electric field between the plates, as a function of t.
(b) Find the displacement current through a circle of radius in the plane mid-way between the plates. Using this circle as your "Amperian loop," and the flat surface that spans it, find the magnetic field at a distance s from the axis.
Figure 7.46
(c) Repeat part (b), but this time uses the cylindrical surface in Fig. 7.46(b), which is open at the right end and extends to the left through the plate and terminates outside the capacitor. Notice that the displacement current through this surface is zero, and there are two contributions to Ienc.
A toroidal coil has a rectangular cross section, with inner radius a , outer radius , and height h . It carries a total of N tightly wound turns, and the current is increasing at a constant rate . If w and h are both much less than a , find the electric field at a point z above the center of the toroid. [Hint: Exploit the analogy between Faraday fields and magnetostatic fields, and refer to Ex. 5.6.]
Problem 7.61 The magnetic field of an infinite straight wire carrying a steady current I can be obtained from the displacement current term in the Ampere/Maxwell law, as follows: Picture the current as consisting of a uniform line charge moving along the z axis at speed v (so that ), with a tiny gap of length E , which reaches the origin at time . In the next instant (up to ) there is no real current passing through a circular Amperian loop in the xy plane, but there is a displacement current, due to the "missing" charge in the gap.
(a) Use Coulomb's law to calculate the z component of the electric field, for points in the xy plane a distances from the origin, due to a segment of wire with uniform density - . extending from toto .
(b) Determine the flux of this electric field through a circle of radius a in the xy plane.
(c) Find the displacement current through this circle. Show that is equal to I , in the limit as the gap width goes to zero.
Where is nonzero in Figure 7.21(b)? Exploit the analogy between Faraday's law and Ampere's law to sketch (qualitatively) the electric field.
In the discussion of motional emf (Sect. 7.1.3) assumed that the wire loop (Fig. 7.10) has a resistance ; the current generated is then . But what if the wire is made out of perfectly conducting material, so that is zero? In that case, the current is limited only by the back emf associated with the self-inductance of the loop (which would ordinarily be negligible in comparison with ). Show that in this regime the loop (mass ) executes simple harmonic motion, and find its frequency. [Answer: ].
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