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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

State your own theoretical and experimental objections to the following statement: In a circuit with two thick-filament bulbs in series, the bulb farther from the negative terminal of the battery will be dimmer, because some of the electron current is used up in the first bulb. Cite relevant experiments.

How can there be a nonzero electric field inside a wire in a circuit? Isn’t the electric field inside a metal always zero?

Question: Some students intended to run a light bulb off two batteries in series in the usual way, but they accidentally hooked up one of the batteries backwards, as shown in Figure 18.89 (the bulb is shown as a thin filament).

(a)Use+’s and -’s to show the approximate steady-state charge distribution along the wires and bulb.

(b)Draw vectors for the electric field at the indicated locations inside the connecting wires and bulb.

(c)Compare the brightness of the bulb in this circuit with the brightness the bulb would have had if one of the batteries hadn’t been put in backwards.

(d)Try the experiment to check your analysis. Does the bulb glow about as you predicted?

Describe the following attributes of a metal wire in steady

state vs. equilibrium:

Metal Wire

Steady-state

Equilibrium

Location of excess charge

Motion of mobile electrons

inside the metal wire

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.

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