A circular wire loop (radiusr, resistanceR) encloses a region of uniform magnetic field,B, perpendicular to its plane. The field (occupying the shaded region in Fig. 7.56) increases linearly with timeB=αt. An ideal voltmeter (infinite internal resistance) is connected between pointsPandQ.

(a) What is the current in the loop?

(b) What does the voltmeter read? [Answer: αr2/2]

Short Answer

Expert verified

(a)The current in the loop isI=παr2R .

(b) The voltmeter reading isαr22 .

Step by step solution

01

Given information

The radius of circular wire loop is,.

The resistance of circular wire loop is, .

The uniform magnetic field inside the wire loop is, .

The relation between the magnetic field and time is, .

02

Magnetic flux

The magnetic flux inside the wire loop having magnetic field and radius is given by,

03

The current in the loop

(b)

The formula for the emf generated in the loop due to magnetic flux is given by,

Solve further as:

The negative sign indicates the emf value is decreasing.

Also, the emf using Ohm’s law,

Then equating both values,

Hence, the current in the loop is .

04

Determine the voltmeter reading value

(b)

Assume a small elemental region of radius inside the given inside the given region between points P and Q.

For a circle of radius , applying Faraday’s law for a closed area, the formula for the measured emf is given by,

In polar form,

Along the line from P to Q,

and ,

Then the voltage reading between points P and Q can be calculated as,

Hence, the voltmeter reading is .

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Most popular questions from this chapter

Question: Suppose j(r)is constant in time but ρ(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:

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Question; An atomic electron (charge q ) circles about the nucleus (charge Q) in an orbit of radius r ; the centripetal acceleration is provided, of course, by the Coulomb attraction of opposite charges. Now a small magnetic field dB is slowly turned on, perpendicular to the plane of the orbit. Show that the increase in kinetic energy, dT , imparted by the induced electric field, is just right to sustain circular motion at the same radius r. (That's why, in my discussion of diamagnetism, I assumed the radius is fixed. See Sect. 6.1.3 and the references cited there.)

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