Question 12 Solution
Step 1: Define the Relationship
Let the initial Voltmeter reading be V1 and Ammeter reading be A1.
In the second case (with parallel resistance), the readings change by a factor of η:
A2 = ηA1
V2 =
V2 =
V1
η
Using Ohm’s Law (V = IR) for the voltmeter section, we find the new equivalent resistance R’v:
R’v =
V2
A2
=
V1η
ηA1
=
V1
η2A1
=
Rv
η2
Step 2: Circuit Equations
Let Rx be the total series resistance (internal resistance + ammeter resistance).
The total current ratio is inversely proportional to the total circuit resistance:
A2
A1
= η =
Rx + Rv
Rx + R’v
Substitute R’v = Rv / η2:
Rx + Rv = η
(
Rx +
Rv
η2
)
Step 3: Solve for Rx
Expand and rearrange the equation:
Rx + Rv = ηRx +
Rv
η
Rv –
Rv
η
= ηRx – Rx
Rv ( 1 –
1
η
)
= Rx (η – 1)
Rv (
η – 1
η
)
= Rx (η – 1)
Canceling (η – 1) from both sides gives us a crucial relationship:
Rx =
Rv
η
Step 4: Calculate Initial Reading
The initial reading V1 is the potential drop across Rv in the original series circuit.
V1 = Ε
(
Rv
Rx + Rv
)
Substitute Rx = Rv / η:
V1 = Ε
(
Rv
)
Rv
η
+ Rv
Divide numerator and denominator by Rv:
V1 = Ε
(
1
)
1
η
+ 1
Multiply numerator and denominator by η:
V1 =
ηΕ
1 + η
Answer: (b)
ηΕ
η + 1
