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

A Nichrome wire 30 cm long and 0.25 mm in diameter is connected to a 1.5 V flashlight battery. What is the electric field inside the wire? Why you don’t have to know how the wire is bent? How would your answer change if the wire diameter change were 0.35 mm? (Not that the electric field in the wire is quiet small compared to the electric field near a charged tape.)

In the few nanoseconds before the steady state is established in a circuit consisting of a battery, copper wires, and a single bulb, is the current the same everywhere in the circuit? Explain.

In a circuit with one battery, connecting wires, and a 12cmlength of Nichrome wire, a compass deflection of 6°is observed. What compass deflection would you expect in a circuit containing two batteries in a series, connecting wires and a36cm length of thicker Nichrome wire (double the cross-sectional area of the thin piece)? Explain.

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.

Question: Three identical light bulbs are connected to two batteries as shown in Figure 18.106. (a) To start the analysis of this circuit you must write energy conservation (loop) equations. Each equation must involve a round-trip path that begins and ends at the same location. Each segment of the path should go through a wire, a bulb, or a battery (not through the air). How many valid energy conservation (loop) equations is it possible to write for this circuit? (b) Which of the following equations are valid energy conservation (loop) equations for this circuit? E1refers to the electric field in bulb 1; L refers to the length of a bulb filament. Assume that the electric field in the connecting wires is small enough to neglect.

(1) +E2L-E3L=0, (2) E1L-E3L=0, (3)+2emf-E2L-E3L=0, (4)E1L-E2L=0, (5)+2emf-E1L-E2L=0, (6)+2emf-E1L-E3L=0, (7)+2emf-E1L-E2L-E3L=0. (c) It is also necessary to write charge conservation equations (node) equations. Each such equation must relate electron current flowing into a node to electron current flowing out of a node. Which of the following are valid charge conservation equations for this circuit? (1)i1=i3, (2)i1=i2, (3)i1=i2+i3. Each battery has an emf of 1.5V. The length of the tungsten filament in each bulb is 0.008m. The radius of the filament is5×10-6m(it is very thin!). The electron mobility of tungsten is localid="1668588909714" 1.8×10-3(m/s)/(V/m). Tungsten has localid="1668588927161" 6×1028mobile electrons per cubic meter. Since there are three unknown quantities, we need three equations relating these quantities. Use any two valid energy conservation equations and one valid charge conservation equation to solve for localid="1668588943223" E1,E2,i1and localid="1668588965567" i2.

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