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Question: Sliding contact of a potentiometer is in the middle of the potentiometer wire having resistance $R_p...

Sliding contact of a potentiometer is in the middle of the potentiometer wire having resistance RpR_p = 1Ω\Omega as shown in the figure. An external resistance of ReR_e = 2Ω\Omega is connected via the sliding contact.

A

0.3 A

B

1.35 A

C

1.0 A

D

0.9 A

Answer

1.0 A

Explanation

Solution

Explanation of the Solution:

  1. Divide the potentiometer: The potentiometer of Rp=1ΩR_p = 1\,\Omega is tapped at the midpoint so that each half has a resistance of 0.5Ω0.5\,\Omega.

  2. Assign Node Voltages: Let the battery voltage be V=0.9VV = 0.9\,V with terminal A at 0.9V0.9\,V and terminal B at 0V0\,V. Let node C be the tap point.

  3. Currents Through Resistors:

    • Current through the top half: I1=0.9VC0.5I_1 = \frac{0.9 - V_C}{0.5}
    • Currents from node C: I2=VC0.5(through the lower half)I_2 = \frac{V_C}{0.5} \quad \text{(through the lower half)} I3=VC2(through external resistor Re=2Ω)I_3 = \frac{V_C}{2} \quad \text{(through external resistor $ R_e = 2\,\Omega $)}
  4. Apply Kirchhoff’s Current Law (KCL) at Node C:

    I1=I2+I3I_1 = I_2 + I_3

    Substituting the expressions:

    0.9VC0.5=VC0.5+VC2\frac{0.9 - V_C}{0.5} = \frac{V_C}{0.5} + \frac{V_C}{2}
  5. Solve for VCV_C: Multiply the whole equation by 2 (LCM of 0.5 and 2):

    2×0.9VC0.5=2×VC0.5+2×VC22\times\frac{0.9 - V_C}{0.5} = 2\times\frac{V_C}{0.5} + 2\times\frac{V_C}{2}

    Since 2/0.5=42/0.5 = 4 and 2/2=12/2 = 1, we get:

    4(0.9VC)=4VC+VC4(0.9 - V_C) = 4V_C + V_C 3.64VC=5VC3.6=9VCVC=0.4V3.6 - 4V_C = 5V_C \quad \Longrightarrow \quad 3.6 = 9V_C \quad \Longrightarrow \quad V_C = 0.4\,V
  6. Determine I1I_1 (Total current from the battery):

    I1=0.90.40.5=0.50.5=1.0AI_1 = \frac{0.9 - 0.4}{0.5} = \frac{0.5}{0.5} = 1.0\,A