Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

Question: Assuming that "Coulomb's law" for magnetic charges ( qm) reads

F=μ04πqm1qm2r2r^

Work out the force law for a monopole moving with velocity through electric and magnetic fields E and B.

Short Answer

Expert verified

Answer

The value of the magnetic charge isF=qmB-μ0ε0υ×E
.

Step by step solution

01

Write the given data from the question.

Assuming that "Coulomb's law" for magnetic charges (qm ) reads.

02

Determine the formula of the magnetic charge qm.

Write the formula of the magnetic charge.

F=qmμ04πQmr2r^

Here, qm is magnetic charge, Qm is magnetic charge and r is radius.

03

Determine the magnetic charge qm.

Determine the magnetic charge qm due to magnetic charge Qm is given by:

F=qmμ04πQmr2r^

It is seen that magnetic field is given by Bμ04πQmr2r^. By analogy replace by E and Bby -μ0ε0E(Griffiths page 339). Total force is given by

role="math" localid="1658304974224" F=qmB-μ0ε0υ×E

Therefore, the value of the magnetic charge qm is F=qmB-μ0ε0υ×E.

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 Vaia!

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

Where is Btnonzero in Figure 7.21(b)? Exploit the analogy between Faraday's law and Ampere's law to sketch (qualitatively) the electric field.

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 ?

An infinite cylinder of radius R carries a uniform surface charge σ. We propose to set it spinning about its axis, at a final angular velocity ω. How much work will this take, per unit length? Do it two ways, and compare your answers:

(a) Find the magnetic field and the induced electric field (in the quasistatic approximation), inside and outside the cylinder, in terms of ω,ω,ands(the distance from the axis). Calculate the torque you must exert, and from that obtain the work done per unit length(W=Ndϕ).

(b) Use Eq. 7.35 to determine the energy stored in the resulting magnetic field.

The magnetic field outside a long straight wire carrying a steady current I is

B=μ02πIsϕ^

The electric field inside the wire is uniform:

E=Iρπa2z^,

Where ρis the resistivity and a is the radius (see Exs. 7.1 and 7 .3). Question: What is the electric field outside the wire? 29 The answer depends on how you complete the circuit. Suppose the current returns along a perfectly conducting grounded coaxial cylinder of radius b (Fig. 7.52). In the region a < s < b, the potential V (s, z) satisfies Laplace's equation, with the boundary conditions

(i) V(a,z)=Iρzπa2 ; (ii) V(b,z)=0

Figure 7.52

This does not suffice to determine the answer-we still need to specify boundary conditions at the two ends (though for a long wire it shouldn't matter much). In the literature, it is customary to sweep this ambiguity under the rug by simply stipulating that V (s,z) is proportional to V (s,z) = zf (s) . On this assumption:

(a) Determine (s).

(b) E (s,z).

(c) Calculate the surface charge density σ(z)on the wire.

[Answer: V=(-Izρ/πa2) This is a peculiar result, since Es and σ(z)are not independent of localid="1658816847863" zas one would certainly expect for a truly infinite wire.]

Two long, straight copper pipes, each of radius a, are held a distance 2d apart (see Fig. 7.50). One is at potential V0, the other at -V0. The space surrounding the pipes is filled with weakly conducting material of conductivity σ. Find the current per unit length that flows from one pipe to the other. [Hint: Refer to Prob. 3.12.]

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.

Sign-up for free