Suppose that a wire leads into another, thinner wire of the same material that has only half the cross-sectional area. In the steady state, the number of electrons per second flowing through the thick wire must be equal to the number of electrons per second flowing through the thin wire. If the electric field \({E_1}\) in the thick wire is \(1 \times 1{0^{ - 2}}\;N/C\), what is the electric field \({E_2}\) in the thinner wire?

Short Answer

Expert verified

The electric field in the thinner wire is \(2 \times {10^{ - 2}}\;{\rm{N/C}}\).

Step by step solution

01

Given information

The cross-sectional area of the thick wire is, \({A_1}\).

The cross-sectional area of the thinner wire is, \({A_2} = \frac{{{A_1}}}{2}\).

The number of electrons per second flowing through the thick wire is, \({n_1}\).

The number of electrons per second flowing through the thinner wire is, \({n_2} = {n_1}\).

The electric field in the thick wire is, \({E_1} = 1 \times {10^{ - 2}}\;{\rm{N/C}}\).

The electric field in the thinner wire is, \({E_2}\).

02

Electron current in a wire

When a certain amount of current is supplied to a conducting wire, the electric current in the wire is carried by the mobile electrons.

The speed of the electrons flowing in the conducting wire changes with the current supplied, the cross-sectional area of the wire, the electric field in the wire, and the mobility of the electrons.

03

The electric field in the thinner wire

According to the question, the thick wire leads into another thinner wire of the same material so the same current flows through both the wires.

Then, the formula for the current flowing through the thick wire is given by,

\(\begin{array}{c}{i_1} = {i_2}\\{n_1}{A_1}{u_1}{E_1} = {n_2}{A_2}{u_2}{E_2}\end{array}\)

Putting, \({n_1} = {n_2}\), \({A_2} = \frac{{{A_1}}}{2}\), and assuming the same mobility in both wires \({u_1} = {u_2}\),

\(\begin{array}{c}{n_1}{A_1}{u_1}{E_1} = {n_1}\frac{{{A_1}}}{2}{u_1}{E_2}\\{E_2} = 2{E_1}\\{E_2} = 2\left( {1 \times {{10}^{ - 2}}\;{\rm{N/C}}} \right)\\{E_2} = 2 \times {10^{ - 2}}\;{\rm{N/C}}\end{array}\)

Hence, the electric field in the thinner wire is \(2 \times {10^{ - 2}}\;{\rm{N/C}}\).

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Most popular questions from this chapter

Since there is an electric field inside a wire in a circuit, why don’t the mobile electrons in the wire accelerate continuously?

In the circuit shown in Figure 18.110, the two thick wires and the thin wire are made of Nichrome.

(a) Show the steady-state electric field at indicated locations, including in the thin wire. (b) Carefully draw pluses and minuses on your own diagram to show the approximate surface-charge distribution in the steady state. Make your drawing show the differences between regions of high surface-charge density and regions of low surface-charge density. (c) The emf of the battery is1.5V. In Nichrome, there are n=9×1028 mobile electrons per m3, and the mobility of mobile electrons is μ=7×10-5(m/s)(V/m). Each thick wire has a length of L1 =20cm=0.2m and a cross-sectional area of A1 =9×10-8 m2. The thin wire has a length of L2=5cm=0.05m and a cross-sectional area of A2=1.5×10-8m2. (The total length of the three wires is 45cm)Calculate the number of electrons entering the thin wire every second in the steady state. Do not make any approximations, and do not use Ohm’s law or series-resistance equations. State briefly where each of your equations comes from.

What is the most important general difference between a system in steady state and a system in equilibrium?

What would be the potential difference VC-VBacross the thin resistor in Figure 18.103 if the battery emf is3.5V ? Assume that the electric field in the thick wires is very small (so that the potential differences along the thick wires are negligible). Do you have enough information to determine the current in the circuit?

Inside a chemical battery it is not actually individual electrons that are transported from the + end to the – end. At the + end of the battery an “acceptor” molecule picks up an electron entering the battery, and at the – end a different “donor” molecule gives up an electron, which leaves the battery. Ions rather than electrons move between the two ends to support the charge inside the battery.

When the supplies of acceptor and donor molecules are used up in a chemical battery, the battery is dead because it can no longer accept or electron. The electron current in electron per second times the number of seconds of battery life, is equal to the number of donor molecules in the battery.

A flashlight battery contains approximately half a mole of donor molecules. The electron current through a thick filament bulb powered by two flashlight batteries in series is about 0.3 A. About how many hours will the batteries keep this bulb lit?

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