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The coil of a moving coil voltmeter is 50 mm long and 40 mm wide and has 120 turns on it. The control spring exerts a torque 200 × 10-6 n – m when the deflection is 100 divisions on full scale. If the flux density of the magnetic field in the air gap is 1.2 wb/m2. The resistance that must be put in series with the coil to give one volt per division.
  • a)
    72 kΩ
  • b)
    36 kΩ 
  • c)
    144 kΩ
  • d)
    108 kΩ 
Correct answer is option 'C'. Can you explain this answer?
Verified Answer
The coil of a moving coil voltmeter is 50 mm long and 40 mm wide and h...
Tc = 200 × 10-6 N – m
Td = B I N A
= 1.2 × I × 120 × 50 × 40 × 10-6
= 288 × 10-3 I n – m
At equilibrium,
Tc = Td
⇒ 200 × 10-6 = 288 × 10-3 I
⇒ I = 0.694 mA.
Let the resistance of the voltmeter circuit be R voltage across the instrument = 0.694 × 10-3 R
This produces a deflection of 100 divisions.
Volts per division 
This value should be equal to 1 in order to get 1 volt per division.
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Most Upvoted Answer
The coil of a moving coil voltmeter is 50 mm long and 40 mm wide and h...
N/m on the coil when it is deflected through an angle of 50°. Determine the voltage that will cause the coil to be deflected through this angle.

We can use the equation for torque on a coil in a magnetic field:

T = NABIBsinθ

where T is the torque, N is the number of turns on the coil, A is the area of the coil, B is the magnetic field strength, I is the current flowing through the coil, and θ is the angle between the magnetic field and the plane of the coil.

We can rearrange this equation to solve for the current:

I = T/(NABBsinθ)

The voltage V across the coil is related to the current I by Ohm's law:

V = IR

where R is the resistance of the coil. We can assume that the resistance of the coil is constant.

Substituting the values given in the problem, we have:

N = 120 turns
A = 0.05 m x 0.04 m = 0.002 m^2
T = 200 N/m
θ = 50° = 0.87 radians
B = unknown
R = unknown

Solving for B, we have:

B = T/(NABIsinθ) = 200/(120 x 0.002 x I x sin(0.87)) = 2.24 x 10^-3 I^-1 T

We can measure the current I that flows through the coil when it is deflected through the angle θ = 50°. The voltage across the coil is then:

V = IR = I(R) = I(unknown)

Substituting for B and solving for I, we have:

I = T/(NABsinθ) = 200/(120 x 0.002 x 2.24 x 10^-3 x sin(0.87)) = 0.834 A

Finally, we can calculate the voltage:

V = IR = 0.834 x R

The value of R is not given in the problem, so we cannot give a numerical answer for the voltage. However, we can see that the voltage is proportional to the current, which is in turn proportional to the torque on the coil. Therefore, increasing the torque on the coil by increasing the magnetic field strength or the number of turns on the coil will increase the deflection of the coil and the voltage measured by the voltmeter.
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The coil of a moving coil voltmeter is 50 mm long and 40 mm wide and has 120 turns on it. The control spring exerts a torque 200 × 10-6n – m when the deflection is 100 divisions on full scale. If the flux density of the magnetic field in the air gap is 1.2 wb/m2. The resistance that must be put in series with the coil to give one volt per division.a)72 kΩb)36 kΩc)144 kΩd)108 kΩCorrect answer is option 'C'. Can you explain this answer?
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