/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Q12P Derive Eq. 8.43. [Hint: Use the ... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Derive Eq. 8.43. [Hint: Use the method of Section 7.2.4, building the two currents up from zero to their final values.]

Short Answer

Expert verified

The equation 8.43 is derived asW=12Lala+12Lblb+MLalb .

Step by step solution

01

Expression for the power delivered to the two loops:

Write the expression for the power delivered to the two loops.

W=12Ll2

Here, L is the inductance, and I is the current.

02

Derive equation 8.43 as W=12LaIa2+12LbIb2+MIaIb

Write the expression for the total energy stored in the pair of coils.

dWdt=-εala-εblb........(1)

Where,

εa=-Ladldt-Mdladt=-Lbdlbdt-Mdlbdt

Substitute the known values in equation (1).

dWdt=-(-Ladladt-Mdladt)-(-Ladldt-Mdlbdt)dWdt=-(-Laladladt-Mladlbdt)+(Lbdldt+Mdlbdt)dWdt=ddt(-12Lala2+12Lalb2+Mlalb)

Integrate with respect to t.

W=-12Lala2+12Lblb2+Mlalb

Therefore, equation 8.43 is derived asW=-12Lala2+12Lblb2+Mlalb .

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Question: A circular disk of radius R and mass M carries n point charges (q), attached at regular intervals around its rim. At time t=0the disk lies in the xy plane, with its center at the origin, and is rotating about the z axis with angular velocity Ó¬0, when it is released. The disk is immersed in a (time-independent) external magnetic field role="math" localid="1653403772759" Bs,z=k-ssÁåž+2zzÁåž, where k is a constant.

(a) Find the position of the center if the ring, zt, and its angular velocity, Ó¬t, as functions of time. (Ignore gravity.)

(b) Describe the motion, and check that the total (kinetic) energy—translational plus rotational—is constant, confirming that the magnetic force does no work.

Consider the charging capacitor in Prob. 7.34.

(a) Find the electric and magnetic fields in the gap, as functions of the distance s from the axis and the timet. (Assume the charge is zero at t=0).

(b) Find the energy density uemand the Poynting vector S in the gap. Note especially the direction of S. Check that Eq.8.12is satisfied.

(c) Determine the total energy in the gap, as a function of time. Calculate the total power flowing into the gap, by integrating the Poynting vector over the appropriate surface. Check that the power input is equal to the rate of increase of energy in the gap (Eq 8.9—in this case W = 0, because there is no charge in the gap). [If you’re worried about the fringing fields, do it for a volume of radius b<awell inside the gap.]

Two concentric spherical shells carry uniformly distributed charges +Q(at radius a) and -Q (at radius ). They are immersed in a uniform magnetic field B=B0z^.

(a) Find the angular momentum of the fields (with respect to the center).

(b) Now the magnetic field is gradually turned off. Find the torque on each sphere, and the resulting angular momentum of the system.

Calculate the power (energy per unit time) transported down the cables of Ex. 7.13 and Prob. 7 .62,, assuming the two conductors are held at potential difference V, and carry current I (down one and back up the other).

An infinitely long cylindrical tube, of radius a, moves at constant speed v along its axis. It carries a net charge per unit length λ, uniformly distributed over its surface. Surrounding it, at radius b, is another cylinder, moving with the same velocity but carrying the opposite charge -λ. Find:

(a) The energy per unit length stored in the fields.

(b) The momentum per unit length in the fields.

(c) The energy per unit time transported by the fields across a plane perpendicular to the cylinders.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.