A rectangular loop of wire is situated so that one end (height h) is between the plates of a parallel-plate capacitor (Fig. 7.9), oriented parallel to the field E. The other end is way outside, where the field is essentially zero. What is the emf in this loop? If the total resistance is R, what current flows? Explain. [Warning: This is a trick question, so be careful; if you have invented a perpetual motion machine, there's probably something wrong with it.]


Short Answer

Expert verified

The emf inside the current is 0V and current is 0A.

Step by step solution

01

Write the given data from the question:

The electric field is E.

Th total resistance is R.

The height between the plates is h.

02

Calculate the emf in the loop and current in the loop.

The emf of the loop is given by,

ε=E-dI …… (1)

For all the electrostatic field, the emf is equal to zero.

Therefore,

E.dI=0

The electric field due to the length of the loop parallel to the capacitor plate is zero because the dIis perpendicular to the electric field. The electric field outside the capacitor is zero. Therefore, the emf due to the wire containing the resistance is zero. The electric field is existed only because of the wire inside the capacitor and parallel to the plates.

The field inside the conductor is E=σε0

Substitute the σε0for and for into equation (1).

ε=σε0h

The electric field is not constant inside the capacitor, and due to fringing, not all the field lines are perpendicular to the field; therefore, the electrostatic field inside the capacitor becomes zero. Therefore, the emf of the loop is zero.

ε=0V

The current in the loop is given by,

I=εR

Substitute 0V for εinto above equation.

I=0RI=0A

Hence, the emf inside the current is 0V and current is 0A.

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Most popular questions from this chapter

A circular wire loop (radius r , resistance R ) 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 time(B=t)An ideal voltmeter (infinite internal resistance) is connected between points P and Q.

(a) What is the current in the loop?

(b) What does the voltmeter read? Answer:[r2/2]

A square loop, side a , resistance R , lies a distance from an infinite straight wire that carries current l (Fig. 7.29). Now someone cuts the wire, so l drops to zero. In what direction does the induced current in the square loop flow, and what total charge passes a given point in the loop during the time this current flows? If you don't like the scissors model, turn the current down gradually:

I(t)={(1-t)I0for0t1/afort>/a

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 ?

Suppose a magnetic monopole qm passes through a resistanceless loop of wire with self-inductance L . What current is induced in the loop?

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.]

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