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Question: A battery of V voltage is connected across the potentiometer wire AC of total resistance \({R_o}\) a...

A battery of V voltage is connected across the potentiometer wire AC of total resistance Ro{R_o} as shown. Calculate the potential across the resistance R if the sliding contact point B is exactly at the middle of the potentiometer wire.

A.2VR4Ro+R\dfrac{{2VR}}{{4{R_o} + R}}.
B.4VRo2Ro+R\dfrac{{4V{R_o}}}{{2{R_o} + R}}.
C.2VRRo+4R\dfrac{{2VR}}{{{R_o} + 4R}}.
D.4VRoRo+2R\dfrac{{4V{R_o}}}{{{R_o} + 2R}}

Explanation

Solution

A potentiometer is a device that is used to calculate the voltage difference. The resistance of the potentiometer is proportional to the length between the point A and B. The total resistance of the potentiometer is in parallel combination.

Complete answer:
The resistance between the points A and B is proportional to the length between the two points. As the length of resistance is exactly middle of the resistance between the points A and B therefore the resistance isRo2\dfrac{{{R_o}}}{2}.
The resistance R and the resistance between the points A and B is Ro2\dfrac{{{R_o}}}{2} and they are arranged in the parallel combination.
Let us calculate the equivalent resistance of the parallel combination,
1R1=1R+1(Ro2)\Rightarrow \dfrac{1}{{{R_1}}} = \dfrac{1}{R} + \dfrac{1}{{\left( {\dfrac{{{R_o}}}{2}} \right)}}
Solving we get the value of R1{R_1},
R1=RRoRo+2R\Rightarrow {R_1} = \dfrac{{R \cdot {R_o}}}{{{R_o} + 2R}}………eq. (1)
The total resistance between the point A and point C will be in series combination and is equal to,
R1+Ro2\Rightarrow {R_1} + \dfrac{{{R_o}}}{2}.
According to ohm's law the current flowing through the circuit is equal to,
V=IR\Rightarrow V = I \cdot R
I=VR1+(Ro2)\Rightarrow I = \dfrac{V}{{{R_1} + \left( {\dfrac{{{R_o}}}{2}} \right)}}
I=2V2R1+Ro\Rightarrow I = \dfrac{{2V}}{{2{R_1} + {R_o}}}.........eq. (2)
The voltage of the potentiometer according to the ohms law is given by,
V1=IR1\Rightarrow {{\text{V}}_1} = I \cdot {R_1}where R1{R_1} is the resistance between the points A and B.
Replace the value of R1{R_1} in the above relation from the equation (1) and equation (2).
V1=IR1\Rightarrow {{\text{V}}_1} = I \cdot {R_1}
V1=[2V2(RRoRo+2R)+Ro](RRoRo+2R)\Rightarrow {{\text{V}}_1} = \left[ {\dfrac{{2V}}{{2\left( {\dfrac{{R \cdot {R_o}}}{{{R_o} + 2R}}} \right) + {R_o}}}} \right] \cdot \left( {\dfrac{{R \cdot {R_o}}}{{{R_o} + 2R}}} \right)
After solving the above relation we get,
V1=2VR4Ro+R\Rightarrow {{\text{V}}_1} = \dfrac{{2{\text{V}}R}}{{4{R_o} + R}}

So the correct option for this problem is A.

Note:
The combination of the resistance between point A and B is in parallel connection and the total resistance of the potentiometer is in series combination. The ohm's law is advisable to remember as it is used in most of the conditions.