First, we need to understand the working method of a potentiometer. Let's follow the given figure. This figure is a simple setup of a potentiometer when it is used for measuring the internal resistance of a cell.
A potentiometer has a long wire with a known resistance (R), and its total length is L (AB). It is attached to a cell and a potential difference is generated across the wire.
J is a moveable point for finding the balancing length. When 0 current in the galvanometer, the circuit is balanced.
When the circuit is balanced, the voltage (V) through the resistance (R) is directly proportional to the balancing length (l) i.e.
V∝l
Therefore, V = kl, where k is a constant.
When the circuit is balanced,
V=E−ir and V=iR, where i is the current in the circuit PQRS and r is the internal resistance of the cell (E).
It means that E - ir = iR.
⇒E=i(r+R) ⇒ i=E(r+R)
Therefore,
⇒V=E−ir=E−\((\frac{E}{(r+R)})\)r
⇒V=E(1−\(\frac{r}{(r+R)}\))
⇒V=\(\frac{ER}{(r+R)}\)
⇒V=\(\frac{\frac{ER}{R}}{\frac{r+R}{R}}\)
= \(\frac{E}{\frac{r}{R}+1}\)
When a resistance of infinity, let the voltage across the resistance be
V1 and the balancing length be l1
Therefore, V1=kl1 …. (i).
And
V1=\(\frac{E}{\frac{r}{R}+1}\)
But, if
R→∞ then
r/R→0
⇒V1=\(\frac{E}{0+1}\)=E…. (ii).
Let the voltage across the shunted resistance of 9.5Ω be V2 and the balancing length be l2
Therefore, V2=kl2…..(iii).
And
V2=\(\frac{9.5E}{r+9.5}\) ….. (iv).
Divide equations (i) and (iii).
⇒
\(\frac{V_1}{V_2}\) =\(\frac{I_1}{I_2}\)
Here, l1= 3 cm and l2 = 2.85cm.
This gives us that
\(\frac{V_1}{V_2}\)=\(\frac{3}{2.85}\)
Now, divide equations (ii) and (iv).
\(\frac{V_1}{V_2}\)=\(\frac{E}{\frac{9.5E}{r+9.5}}\) =\(\frac{r+9.5}{9.5}\)
But \(\frac{V_1}{V_2}\) =\(\frac{3}{2.85}\)
Therefore,
\(\frac{r+9.5}{9.5}\) = \(\frac{3}{2.85}\)
⇒2.85(r+9.5)=3(9.5)
⇒2.85r+27.075=28.5
⇒r=\(\frac{(28.5-27.075)}{2.85}\) = \(\frac{1.425}{2.85}\) = 0.5Ω
Therefore, the internal resistance of that cell is 0.5Ω
Option (C) is correct.
Here,
The formula for the Internal resistance, r = (\(\frac{E-V}{V}\))R = (\(\frac{I_1 - I_2}{I_2}\))R
=(\(\frac{3-2.85}{2.85}\))(9.5)Ω = 0.5Ω
So, Option (c) is the correct answer.
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A full wave rectifier circuit with diodes (\(D_1\)) and (\(D_2\)) is shown in the figure. If input supply voltage \(V_{in} = 220 \sin(100 \pi t)\) volt, then at \(t = 15\) msec:
Current electricity is defined as the flow of electrons from one section of the circuit to another.
There are two types of current electricity as follows:
The current electricity whose direction remains the same is known as direct current. Direct current is defined by the constant flow of electrons from a region of high electron density to a region of low electron density. DC is used in many household appliances and applications that involve a battery.
The current electricity that is bidirectional and keeps changing the direction of the charge flow is known as alternating current. The bi-directionality is caused by a sinusoidally varying current and voltage that reverses directions, creating a periodic back-and-forth motion for the current. The electrical outlets at our homes and industries are supplied with alternating current.