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Question: An accumulator of emf 2V and negligible internal resistance is connected across a uniform wire of le...

An accumulator of emf 2V and negligible internal resistance is connected across a uniform wire of length 10m10m and resistance 30Ω30\Omega . The appropriate terminals of a cell of emf 1.5V1.5V and internal resistance 1Ω1\Omega is connected to one end of the wire, and the other end of the cell is connected through a sensitive galvanometer to a slider on the wire. If the balancing changes when the cell of 1.5V1.5V is shunted with a resistance of 5Ω5\Omega is x4m\dfrac{x}{4}m. Find xx.

Explanation

Solution

Resistance is defined as the opposition offered to the flow of electrons in a current carrying conductor. Also the e.m.f. is the energy provided by a cell to the charge passing through it. When the electric potential decreases along the path following in a circuit, then there is voltage drop.

Complete step by step answer:
Step I:
Given that the cell is connected to a galvanometer, there will be a deflection when the galvanometer is made to slide on the wire.
Let the length of the wire XY is =x = x such that the current II flowing through that part of the wire is zero and the galvanometer shows a zero deflection. That is
Ig=0{I_g} = 0
Also voltage drop on the balancing length is given in accordance to Ohm’s Law,
V=IRV = IR
Here ρ\rho is the resistance
So, V=IρxV = I\rho x

Step II:
When there is no current in the wire and galvanometer shows zero deflection, then
Voltage across the circuit = Voltage across the part of wire XZ
Let ρ\rho be the resistance of the wire.
Since only two resistances are in parallel along the part of the wire XZ. The equivalent resistance in a parallel circuit is the reciprocal of the sum of individual resistances and is given by
1Req=1R1+1R2\dfrac{1}{{{R_{eq}}}} = \dfrac{1}{{{R_1}}} + \dfrac{1}{{{R_2}}}
On substituting the corresponding values,
1Req=(11+15)\Rightarrow \dfrac{1}{{{R_{eq}}}} = (\dfrac{1}{1} + \dfrac{1}{5})
1Req=65\Rightarrow \dfrac{1}{{{R_{eq}}}} = \dfrac{6}{5}
Step III:
Also the resultant e.m.f is given by
Eeq=E1r1+E2r21Req{E_{eq}} = \dfrac{{\dfrac{{{E_1}}}{{{r_1}}} + \dfrac{{{E_2}}}{{{r_2}}}}}{{\dfrac{1}{{{R_{eq}}}}}}
Substituting the values and solving,
Eeq=1.51+0565\Rightarrow {E_{eq}} = \dfrac{{\dfrac{{1.5}}{1} + \dfrac{0}{5}}}{{\dfrac{6}{5}}}
On simplifications,
Eeq=54volt\Rightarrow {E_{eq}} = \dfrac{5}{4}volt
Step IV:
Let yy is the length of the wire that is to be calculated when slider is moved and when the galvanometer shows zero deflection,
54=23×3010×y\Rightarrow \dfrac{5}{4} = \dfrac{2}{3} \times \dfrac{{30}}{{10}} \times y
On simplification,
y=254m\Rightarrow y = \dfrac{{25}}{4}m
On further simplification,
x=25m\Rightarrow x = 25m

The length of xx is 25m25m.

Note:
It is important to note that the terms e.m.f and voltage are different. When external forces work to move a charge from one point to another then the voltage produced is represented by e.m.f. But the voltage denotes the potential difference across two points.