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Suppose that wire A and wire B are made of different metals and are subjected to the same electric field in two different circuits. Wire B has the 6 times the cross sectional area, 1.3 times as many mobile electrons per cubic centimetre and 4 times the mobility of wire A. In the steady state \({\bf{2 \times 1}}{{\bf{0}}^{{\bf{18}}}}\) electrons enters wire A every second. How many electrons enter wire B every second?

Short Answer

Expert verified

The number of electrons enter in wire B per second are \(6.24 \times {10^{19}}\;{\rm{electrons}}/{\rm{s}}\).

Step by step solution

01

Identification of given data

The electric field for circuits of wire A and wire B is\({E_A} = {E_B}\)

The cross sectional area of the wire B is\({A_B} = 6{A_A}\)

The number of electrons per cubic centimetre for wire B is\({n_B} = 1.3{n_A}\)

The mobility of wire B is\({\mu _B} = 4{\mu _A}\)

The number of electrons enters in wire A per second is\({I_A} = 2 \times {10^{18}}\;{\rm{electrons}}/{\rm{s}}\)

The number of electrons entering in wire B per second is calculated by equating the electric field for both metal wires.

02

Determination of expression to find the electrons enter in wire B per second

The electric field for both metals are same so,

\(\begin{array}{c}{E_A} = {E_B}\\\frac{{{V_A}}}{{{L_A}}} = \frac{{{V_B}}}{{{L_B}}}\\\frac{{{I_A}{R_A}}}{{{L_A}}} = \frac{{{I_B}{R_B}}}{{{L_B}}}\\\frac{{{I_A}}}{{{L_A}}}\left( {\frac{{{L_A}}}{{{\sigma _A}{A_A}}}} \right) = \frac{{{I_B}}}{{{L_B}}}\left( {\frac{{{L_B}}}{{{\sigma _B}{A_B}}}} \right)\end{array}\)

\(\begin{array}{c}\frac{{{I_A}}}{{{L_A}}}\left( {\frac{{{L_A}}}{{{n_A}{\mu _A}{A_A}}}} \right) = \frac{{{I_B}}}{{{L_B}}}\left( {\frac{{{L_B}}}{{{n_B}{\mu _B}{A_B}}}} \right)\\\frac{{{I_A}}}{{{n_A}{\mu _A}{A_A}}} = \frac{{{I_B}}}{{{n_B}{\mu _B}{A_B}}}\end{array}\)

03

Determination of electrons enter in wire B per second

Substitute all the values in above equation.

\(\begin{array}{c}\frac{{\left( {2 \times {{10}^{18}}\;{\rm{electrons}}/{\rm{s}}} \right)}}{{{n_A}{\mu _A}{A_A}}} = \frac{{{I_B}}}{{\left( {1.3{n_A}} \right)\left( {4{\mu _A}} \right)\left( {6{A_A}} \right)}}\\{I_B} = 6.24 \times {10^{19}}\;{\rm{electrons}}/{\rm{s}}\end{array}\)

Therefore, the number of electrons enter in wire B per second are \(6.24 \times {10^{19}}\;{\rm{electrons}}/{\rm{s}}\).

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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.)

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

The emf of a particular flashlight battery is 1.7 V. If the battery is 4.5 cm long and radius of cylindrical battery is 1 cm, estimate roughly the amount of charge on the positive end plate of the battery.

Question: A circuit is constructed from two batteries and two wires, as shown in Figure 18.104. Each battery has an emf of 1.3V. Each wire is26cmlong and has a diameter of 7×10-4m. The wires are made of a metal that has7×1028mobile electrons per cubic meter; the electron mobility is 5×10-5(m/s)/(V/m). A steady current runs through the circuit. The locations marked by ×and labeled by a letter are in the interior of the wire. (a) Which of these statements about the electric field in the interior of the wires, at the locations marked by ×'s, are true? List all that apply. (1) The magnitude of the electric field at location G is larger than the magnitude of the electric field at location F. (2) At every marked location the magnitude of the electric field is the same. (3) At location B the electric field points to the left. (b) Write a correct energy conservation (round-trip potential difference) equation for this circuit, along a round-trip path starting at the negative end of battery 1 and traveling counterclockwise through the circuit (that is, traveling to the left through the battery, and continuing on around the circuit in the same direction). (c) What is the magnitude of the electric field at location B? (d) How many electrons per second enter the positive end of battery 2? (e)If the cross-sectional area of both wires were increased by a factor of 2, what would be the magnitude of the electric field at location B? (f) Which of the diagrams in Figure 18.105 best shows the approximate distribution of excess charge on the surface of the circuit?

In the circuit shown in Figure 18.87, bulbs 1 and 2 are identical in mechanical construction (the filaments have the same length and the same cross-sectional area), but the filaments are made of different metals. The electron mobility in the metal used in bulb 2 is three times as large as the electron mobility in the metal used in bulb 1, but both metals have the same number of mobile electrons per cubic meter. The two bulbs are connected in series to two batteries with thick copper wires (like your connecting wires).

(a)In bulb 1, the electron current is i1and the electric field is E1. In terms of these quantities, determine the corresponding quantities i2and E2for bulb 2, and explain your reasoning.

(b)When bulb 2 is replaced by a wire, the electron current through bulb 1 is i0and the electric field in bulb 1 is E0. How big is i1 in terms of i0? Explain your answer, including explicit mention of any approximations you must make. Do not use ohms or series-resistance equations in your explanation, unless you can show in detail how these concepts follow from the microscopic analysis introduced in this chapter.

(c)Explain why the electric field inside the thick copper wires is very small. Also explain why this very small electric field is the same in all of the copper wires, if they all have the same cross-sectional area.

(d)Figure 18.88 is a graph of the magnitude of the electric field at each location around the circuit when bulb 2 is replaced by a wire. Copy this graph and add to it, on the same scale, a graph of the magnitude of the electric field at each location around the circuit when both bulbs are in the circuit. The very small field in the copper wires has been shown much larger than it really is in order to give you room to show how that small field differs in the two circuits.

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