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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 48 cm long and 0.25 mm in diameter is connected to a 1.6 V flashlight battery. What is the electric field inside the wire? Why you donโ€™t have to know how the wire is bent? How would your answer change if the wire diameter change were 0.20 mm? (Not that the electric field in the wire is quiet small compared to the electric field near a charged tape.)

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

Why does the brightness of a bulb not change noticeably when you use longer copper wires to connect it to the battery? (1) Very little energy is dissipated in the thick connecting wires. (2) The electric field in connecting wires is very small, so emfโ‰ˆEbulbLbulb. (3) Electric field in the connecting wires is zero, so emfโ‰ˆEbulbLbulb. (4) Current in the connecting wires is smaller than current in the bulb. (5) All the current is used up in the bulb, so the connecting wires donโ€™t matter.

A steady-state current flows through the Nichrome wire in the circuit shown in Figure 18.90. Before attempting to answer the following questions, draw a copy of this diagram. All of the locations indicated by letters are inside the wire.

(a)On your diagram, show the electric field at the locations indicated, paying attention to relative magnitude.

(b)Carefully draw pluses and minuses on your diagram to show the approximate surface charge distribution that produces the electric field you drew. Make your drawing show clearly the differences between regions of high surface charge density and regions of low surface-charge density. Use your diagram to determine which of the following statements about this circuit are true.

(1) There is some excess negative charge on the surface of the wire near location B.

(2) Inside the metal wire the magnitude of the electric field is zero.

(3) The magnitude of the electric field is the same at locations Gand C.

(4) The electric field points to the left at location G.

(5) There is no excess charge on the surface of the wire.

(6) There is excess charge on the surface of the wire near the batteries but nowhere else.

(7) The magnitude of the electric field inside the wire is larger at location Gthan at location C.

(8) The electric field at location Dpoints to the left.

(9) Because the current is not changing, the circuit is in static equilibrium.

Inside a chemical battery it is not actually individual electrons that are transported from the + end to the โ€“ end. At the + end of the battery an โ€œacceptorโ€ molecule picks up an electron entering the battery, and at the โ€“ end a different โ€œdonorโ€ 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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