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Question: Figure shows the internal wiring of a three-range voltmeter whose binding posts are marked +, 2V, 10...

Figure shows the internal wiring of a three-range voltmeter whose binding posts are marked +, 2V, 10V and 100V. When the meter is connected to the circuit being measured, one connection is made to the post marked + and the other to the post marked with the desired voltage range. The resistance of the moving coil RGR_G is 40Ω40\Omega and a current of 1 mA in the coil causes it to deflect full-scale. Then match the following:

A

Value of resistance R1R_1 in kΩk\Omega

B

Value of resistance R3R_3 in kΩk\Omega

C

Overall resistance of the meter in 100 V range in kΩk\Omega

D

Overall resistance of the meter in 2 V range in kΩk\Omega

Answer

a-r, b-s, c-p, d-q

Explanation

Solution

The problem describes a three-range voltmeter and asks to match the calculated values of resistances and overall meter resistances with given options.

Given:

  • Resistance of the moving coil, RG=40ΩR_G = 40 \, \Omega
  • Full-scale deflection current, IG=1mA=1×103AI_G = 1 \, \text{mA} = 1 \times 10^{-3} \, \text{A}

A voltmeter is formed by connecting a high resistance (multiplier) in series with a galvanometer. The voltage range VV is given by the formula: V=IG(RG+Rseries)V = I_G (R_G + R_{series}) where RseriesR_{series} is the total series resistance connected with the galvanometer coil.

Let's calculate the required values step-by-step:

a. Value of resistance R1R_1 in kΩ\Omega When the meter is used in the 2V range, the total resistance in the circuit is RG+R1R_G + R_1. The full-scale voltage for this range is V1=2VV_1 = 2 \, \text{V}. V1=IG(RG+R1)V_1 = I_G (R_G + R_1) 2V=(1×103A)(40Ω+R1)2 \, \text{V} = (1 \times 10^{-3} \, \text{A}) (40 \, \Omega + R_1) 2/(1×103)=40+R12 / (1 \times 10^{-3}) = 40 + R_1 2000=40+R12000 = 40 + R_1 R1=200040=1960ΩR_1 = 2000 - 40 = 1960 \, \Omega Converting to kΩ\Omega: R1=1.96kΩR_1 = 1.96 \, \text{k}\Omega. So, (a) matches with (r).

b. Value of resistance R3R_3 in kΩ\Omega To find R3R_3, we first need to find R2R_2. For the 10V range, the total resistance in the circuit is RG+R1+R2R_G + R_1 + R_2. The full-scale voltage for this range is V2=10VV_2 = 10 \, \text{V}. V2=IG(RG+R1+R2)V_2 = I_G (R_G + R_1 + R_2) 10V=(1×103A)(40Ω+1960Ω+R2)10 \, \text{V} = (1 \times 10^{-3} \, \text{A}) (40 \, \Omega + 1960 \, \Omega + R_2) 10/(1×103)=2000+R210 / (1 \times 10^{-3}) = 2000 + R_2 10000=2000+R210000 = 2000 + R_2 R2=100002000=8000Ω=8kΩR_2 = 10000 - 2000 = 8000 \, \Omega = 8 \, \text{k}\Omega.

Now, for the 100V range, the total resistance in the circuit is RG+R1+R2+R3R_G + R_1 + R_2 + R_3. The full-scale voltage for this range is V3=100VV_3 = 100 \, \text{V}. V3=IG(RG+R1+R2+R3)V_3 = I_G (R_G + R_1 + R_2 + R_3) 100V=(1×103A)(40Ω+1960Ω+8000Ω+R3)100 \, \text{V} = (1 \times 10^{-3} \, \text{A}) (40 \, \Omega + 1960 \, \Omega + 8000 \, \Omega + R_3) 100/(1×103)=10000+R3100 / (1 \times 10^{-3}) = 10000 + R_3 100000=10000+R3100000 = 10000 + R_3 R3=10000010000=90000ΩR_3 = 100000 - 10000 = 90000 \, \Omega Converting to kΩ\Omega: R3=90kΩR_3 = 90 \, \text{k}\Omega. So, (b) matches with (s).

c. Overall resistance of the meter in 100 V range in kΩ\Omega The overall resistance of the meter in the 100V range is the total resistance in series with the galvanometer for this range. Rtotal,100V=RG+R1+R2+R3R_{total, 100V} = R_G + R_1 + R_2 + R_3 Rtotal,100V=40Ω+1960Ω+8000Ω+90000ΩR_{total, 100V} = 40 \, \Omega + 1960 \, \Omega + 8000 \, \Omega + 90000 \, \Omega Rtotal,100V=100000ΩR_{total, 100V} = 100000 \, \Omega Converting to kΩ\Omega: Rtotal,100V=100kΩR_{total, 100V} = 100 \, \text{k}\Omega. So, (c) matches with (p).

d. Overall resistance of the meter in 2 V range in kΩ\Omega The overall resistance of the meter in the 2V range is the total resistance in series with the galvanometer for this range. Rtotal,2V=RG+R1R_{total, 2V} = R_G + R_1 Rtotal,2V=40Ω+1960ΩR_{total, 2V} = 40 \, \Omega + 1960 \, \Omega Rtotal,2V=2000ΩR_{total, 2V} = 2000 \, \Omega Converting to kΩ\Omega: Rtotal,2V=2kΩR_{total, 2V} = 2 \, \text{k}\Omega. So, (d) matches with (q).

Summary of Matches:

  • a. Value of resistance R1R_1 in kΩ\Omega \rightarrow r. 1.96
  • b. Value of resistance R3R_3 in kΩ\Omega \rightarrow s. 90
  • c. Overall resistance of the meter in 100 V range in kΩ\Omega \rightarrow p. 100
  • d. Overall resistance of the meter in 2 V range in kΩ\Omega \rightarrow q. 2

Explanation of the solution:

  1. Voltmeter Principle: A voltmeter measures potential difference by connecting a high resistance in series with a galvanometer. The full-scale deflection voltage (VV) is related to the full-scale deflection current (IGI_G), galvanometer resistance (RGR_G), and series resistance (RseriesR_{series}) by V=IG(RG+Rseries)V = I_G (R_G + R_{series}).
  2. 2V Range: For the 2V range, the series resistance is R1R_1. Using V1=IG(RG+R1)V_1 = I_G (R_G + R_1), calculate R1R_1. The overall resistance for this range is RG+R1R_G + R_1.
  3. 10V Range: For the 10V range, the series resistance is R1+R2R_1 + R_2. Using V2=IG(RG+R1+R2)V_2 = I_G (R_G + R_1 + R_2), calculate R2R_2.
  4. 100V Range: For the 100V range, the series resistance is R1+R2+R3R_1 + R_2 + R_3. Using V3=IG(RG+R1+R2+R3)V_3 = I_G (R_G + R_1 + R_2 + R_3), calculate R3R_3. The overall resistance for this range is RG+R1+R2+R3R_G + R_1 + R_2 + R_3.
  5. Conversion: Convert all resistance values from Ohms to kilo-Ohms as required.