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

A current flows to the right through a rectangular bar of conducting material, in the presence of a uniform magnetic fieldBpointing out of the page (Fig. 5.56).

(a) If the moving charges are positive, in which direction are they deflected by the magnetic field? This deflection results in an accumulation of charge on the upper and lower surfaces of the bar, which in turn produces an electric force to counteract the magnetic one. Equilibrium occurs when the two exactly cancel. (This phenomenon is known as the Hall effect.)

(b) Find the resulting potential difference (the Hall voltage) between the top and bottom of the bar, in terms ofB,v(the speed of the charges), and the relevant dimensions of the bar.23

(c) How would your analysis change if the moving charges were negative? [The Hall effect is the classic way of determining the sign of the mobile charge carriers in a material.]

Short Answer

Expert verified

(a) The positive charges are deflected in the downwards direction by the magnetic field.

(b) The resulting potential difference between the top and the bottom of the bar is .

(c) The negative charge is deflected downwards and the top plate gets the higher potential.

Step by step solution

01

Identification of given data

The given data is listed below as:

  • The conducting material has a current I.
  • The uniform magnetic field of the conducting bar is,B
  • The width of the bar is,w
  • The length of the bar is,I
  • The thickness of the bar is,t
02

Significance of the magnetic field

The magnetic field is described as a particular region that helps a magnetic material to exert a magnetic force on other objects. Moreover, this magnetic field

is also termed as a vector field that is beneficial for describing the magnetic influence on the moving charges.

03

(a) Determination of the direction the moving charges got deflected by the magnetic field

According to the hall effect, if the positive charges mainly flow to the right, then the bottom plate also acquires a positive charge. Hence, due to flowing in the right direction, the positive charges are also deflected downwards.

Thus, the positive charges are deflected in the downwards direction by the magnetic field.

04

(b) Determination of the resulting potential difference between the top and bottom of the bar

The equation of the force at the top of the bar is expressed as:

F=qvB …(i)

Here,qis the electric charge,vis the velocity of the bat andBis the uniform magnetic field.

The equation of the force at the bottom of the bar is expressed as:

F=qE …(i)

Here, qis the electric charge andEis the electric field.

As the force on the top and the bottom of the bar is equal. Then the equation (i) and (ii) is also equal.

Equating the equation (i) and (ii).

qvB=qEE=vB …(iii)

The equation of the potential difference between the top and the bottom of the bar is expressed as:

V1-V2=Et

Here,V1is the potential at the top andV2is the potential at the bottom of the bar andtis the thickness of the bar.

Substitute vBfor Efrom the equation (iii) in the above equation.

V1-V2=vBt

Thus, the resulting potential difference between the top and the bottom of the bar isvBt .

05

(c) Determination of the change in the analysis

According to the Hall effect, if the negative charges mainly flow to the left, then the negative charge is also deflected downwards and the bottom plate becomes negatively charged. Moreover, the difference in potential between the two plates is the same but the top plate mainly acquires a higher potential.

Thus, the negative charge is deflected downwards and the top plate gets the higher potential.

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

Suppose you have two infinite straight line chargesλ, a distance d apart, moving along at a constant speed υ(Fig. 5.26). How great would have tobe in order for the magnetic attraction to balance the electrical repulsion? Work out the actual number. Is this a reasonable sort of speed?

(a) Prove that the average magnetic field, over a sphere of radius R, due to steady currents inside the sphere, is

Bave=μ042m˙4

where mbis the total dipole moment of the sphere. Contrast the electrostatic result, Eq. 3.105. [This is tough, so I'll give you a start:

Bave=14π3R3fBd

Write BUas ×A, and apply Prob. 1.61(b). Now put in Eq. 5.65, and do the surface integral first, showing that

1rd43,

(b) Show that the average magnetic field due to steady currents outside the sphere is the same as the field they produce at the center.

Magnetostatics treats the "source current" (the one that sets up the field) and the "recipient current" (the one that experiences the force) so asymmetrically that it is by no means obvious that the magnetic force between two current loops is consistent with Newton's third law. Show, starting with the Biot-Savart law (Eq. 5.34) and the Lorentz force law (Eq. 5.16), that the force on loop 2 due to loop 1 (Fig. 5.61) can be written as

F2=μ04πl1l2r^r2dl1dl2

Figure 5.60

Figure 5.61

In this form, it is clear that F2=-F1, since role="math" localid="1657622030111" r^changes direction when the roles of 1 and 2 are interchanged. (If you seem to be getting an "extra" term, it will help to note thatdl2r^=dr.)

(a) Prove that the average magnetic field, over a sphere of radius R,due to steadycurrents inside the sphere, is

Bave=μ04π2mR3

wheremis the total dipole moment of the sphere. Contrast the electrostatic

result, Eq. 3.105. [This is tough, so I'll give you a start:

Bave=143πR3Bdτ

WriteBas×A ,and apply Prob. 1.61(b). Now put in Eq. 5.65, and do the

surface integral first, showing that

1rda=43πr'

(b) Show that the average magnetic field due to steady currents outsidethe sphere

is the same as the field they produce at the center.

(a) Check Eq. 5.76 for the configuration in Ex. 5.9.

(b) Check Eqs. 5.77 and 5.78 for the configuration in Ex. 5.11.

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