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.

Short Answer

Expert verified

The amount of charge on the positive end of the battery plate is1.051×10-13C

Step by step solution

01

Identification of given data

The emf of the flashlight battery is ε=1.7V

The length of battery is l=4.5cm

The radius of cylindrical battery isr=1cm

The amount of charge at the positive end of battery plate is found by the product of the capacitance and emf of the battery.

02

Determination of formula for amount of charge on the positive end of battery plate

The capacitance of the cylindrical battery is given as:C=ε0πr2l

Here, ε0is the permeability of free space and its value is8.854×10-12C2/N·m2 .

03

Determination of amount of charge on the positive end of battery plate

Substitute all the values in above equation.

C=8.854×10-12C2/N·m2π1cm1m100cm24.5cm1m100cmC=6.18×10-14F

The amount of charge on the positive end of the battery plate is given as:

q=Cε

Substitute all the values in above equation.

q=6.18×10-14F1.7Vq=1.051×10-13C

Therefore, the amount of charge on the positive end of the battery plate is1.051×10-13C

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Most popular questions from this chapter

Criticize the statement below on theoretical and experimental grounds. Be specific and precise. Refer to your own experiments, or describe any new experiments you perform: “A flashlight battery always puts out the same amount of current, no matter what is connected to it.”

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?

Compare the direction of the average electric field inside a battery to the direction of the electric field in the wires and resistors of a circuit.

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?

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.

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