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Vitek1552 [10]
3 years ago
15

Two fully charged cylindrical capacitors are connected to two identical batteries. The capacitors are identical except that the

radius of the outer plate of capacitor A is four times the radius of the outer plate of capacitor B. Both inner plates have a radius that is half the outer radius of capacitor B.
(a) What is the relative capacitance of each capacitor? Express your answer as a ratio CA/CB.

(b) What is the relative energy stored by each capacitor? Express your answer as a ratio UA/UB.

(c) What is the relative charge stored by each capacitor? Express your answer as a ratio QA/QB.

Physics
1 answer:
Leni [432]3 years ago
8 0

Answer:

Part(a):  The relative capacitance is \dfrac{C_{A}}{C_{B}} = 0.33

Part(b): The relative energy stored is \dfrac{U_{A}}{U_{B}} = 0.33

Part(c): The relative charge stored is \dfrac{Q_{A}}{Q_{B}} = 0.33

Explanation:

We know the capacitance (C) of a capacitor having charge (Q) and subjected to a potential difference of (V) is given by

C = \dfrac{Q}{V}

Also, the energy (U) stored by a capacitor can be written as

U = \dfrac{1}{2}C~V^{2}

Let us assume that the inner radius of the Capacitor B, as shown in the figure, be \textbf{r_{i}^{B}}\bf{r_{i}^{B}}, the outer radius be \bf{r_{o}^{B}}, the inner radius of Capacitor A be \bf{r_{i}^{A}} and the outer radius be \bf{r_{o}^{B}}.

Given in the problem,

&& r_{o}^{B} = 2~r_{B}^{i}\\&& r_{o}^{A} = 4~r_{B}^{i}\\&& and~r_{i}^{B} = 4~r_{o}^{B} = 8~r_{B}^{i}

Now, the capacitance (C) of a cylindrical capacitor is given by,

\bf{C = \dfrac{2~\pi~\epsilon_{0}~L}{ln(\dfrac{r_{o}}{r_{i}})}}

where \epsilon_{o} is the permittivity of the free space, L is the length of the cylindrical capacitor.

Part(a):

The capacitance of capacitor A,

C_{A} = \dfrac{2~\pi~\epsilon_{0}L}{ln(\dfrac{r_{o}^{A}}{r_{i}^{A}})} = \dfrac{2~\pi~\epsilon_{0}L}{ln(\dfrac{8~r_{i}^{B}}{r_{i}^{B}})} = \dfrac{2~\pi~\epsilon_{0}L}{ln(8)}

and the capacitance of capacitor B,

C_{B} = \dfrac{2~\pi~\epsilon_{0}L}{ln(\dfrac{r_{o}^{B}}{r_{i}^{B}})} = \dfrac{2~\pi~\epsilon_{0}L}{ln(\dfrac{2~r_{i}^{B}}{r_{i}^{B}})} = \dfrac{2~\pi~\epsilon_{0}L}{ln(2)}

giving the relative capacitance of each capacitor to be

\dfrac{C_{A}}{C_{B}} = \dfrac{ln(2)}{ln(8)} = \dfrac{ln(2)}{3~\ln(2)} = \dfrac{1}{3} = 0.33

Part(b):

Energy stored by capacitor A,

U_{A} = \dfrac{1}{2}~C_{A}~V^{2}

Energy stored by capacitor B,

U_{B} = \dfrac{1}{2}~C_{B}~V^{2}

giving the relative energy stored by each capacitor to be

\dfrac{U_{A}}{U_{B}} = \dfrac{C_{A}}{C_{B}} = 0.33

Part(c):

The charge stored by capacitor A,

Q_{A} = C_{A}~V

The charge stored by capacitor B,

Q_{B} = C_{B}~V

giving the relative charge stored by each capacitor to be

\dfrac{Q_{A}}{Q_{B}} =  \dfrac{C_{A}}{C_{B}} = 0.33

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(a) 638.4 J

The work done by a force is given by

W=Fd cos \theta

where

F is the magnitude of the force

d is the displacement of the object

\theta is the angle between the direction of the force and the displacement

Here we want to calculate the work done by the force F, of magnitude

F = 152 N

The displacement of the suitcase is

d = 4.20 m along the ramp

And the force is parallel to the displacement, so \theta=0^{\circ}. Therefore, the work done by this force is

W_F=(152)(4.2)(cos 0)=638.4 J

b) -328.2 J

The magnitude of the gravitational force is

W = mg

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m = 19.6 kg is the mass of the suitcase

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Substituting,

W=(19.6)(9.8)=192.1 N

Again, the displacement is

d = 4.20 m

The gravitational force acts vertically downward, so the angle between the displacement and the force is

\theta= 90^{\circ} - \alpha = 90+24=114^{\circ}

Where \alpha = 24^{\circ} is the angle between the incline and the horizontal.

Therefore, the work done by gravity is

W_g=(192.1)(4.20)(cos 114^{\circ})=-328.2 J

c) 0

The magnitude of the normal force is equal to the component of the weight perpendicular to the ramp, therefore:

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And substituting

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\alpha=24^{\circ}

We find

R=(19.6)(9.8)(cos 24)=175.5 N

Now: the angle between the direction of the normal force and the displacement of the suitcase is 90 degrees:

\theta=90^{\circ}

Therefore, the work done by the normal force is

W_R=R d cos \theta =(175.4)(4.20)(cos 90)=0

d) -194.5 J

The magnitude of the force of friction is

F_f = \mu R

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d = 4.20 m

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f) 3.3 m/s

First of all, we have to find the work done by each force on the suitcase while it has travelled a distance of

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Using the same procedure as in part a-d, we find:

W_F=(152)(3.80)(cos 0)=577.6 J

W_g=(192.1)(3.80)(cos 114^{\circ})=-296.9 J

W_R=(175.4)(3.80)(cos 90)=0

W_f =(46.3)(3.80)(cos 180)=-175.9 J

So the total work done is

W=577.6+(-296.9)+0+(-175.9)=104.8 J

Now we can use the work-energy theorem to find the final speed of the suitcase: in fact, the total work done is equal to the gain in kinetic energy of the suitcase, therefore

W=\Delta K = K_f - K_i\\W=\frac{1}{2}mv^2\\v=\sqrt{\frac{2W}{m}}=\sqrt{\frac{2(104.8)}{19.6}}=3.3 m/s

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3 years ago
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