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Question: AB is a uniform wire of length L= 100 cm. A cell of emf $V_0$ = 12 *volt* is connected across AB. A ...

AB is a uniform wire of length L= 100 cm. A cell of emf V0V_0 = 12 volt is connected across AB. A resistance R, cell of emf V and a milliammeter (which can show deflection in both directions) is connected to the circuit as shown. Contact C can be slid on the wire AB. Distance AC = x. The current (I) through the milliammeter is taken positive when the cell of emf V is discharging. A graph of I vs x has been shown. Neglect internal resistance of the cells

Answer

V = 2.4 V, R = 80 Ω

Explanation

Solution

To solve this problem, we need to analyze the potentiometer circuit and the given graph of current (I) versus distance (x).

1. Calculate the potential gradient of the potentiometer wire: The length of the uniform wire AB is L=100 cmL = 100 \text{ cm}. The cell connected across AB has an EMF V0=12 VV_0 = 12 \text{ V}. The potential gradient (ϕ\phi) along the wire is given by: ϕ=V0L=12 V100 cm=0.12 V/cm\phi = \frac{V_0}{L} = \frac{12 \text{ V}}{100 \text{ cm}} = 0.12 \text{ V/cm}

2. Formulate the equation for current (I) in the secondary circuit: The secondary circuit consists of a resistance R, a cell of EMF V, and a milliammeter connected between point A and contact C. The distance AC is x. The potential difference across the segment AC of the potentiometer wire is VAC=ϕxV_{AC} = \phi \cdot x. Let's apply Kirchhoff's Voltage Law (KVL) to the loop formed by the resistance R, cell V, milliammeter, and the wire segment AC. The problem states that current I is taken positive when the cell of EMF V is discharging. This means current flows out of the positive terminal of cell V. From the circuit diagram, the positive terminal of cell V is connected towards the milliammeter and then to point C. The current then flows from C to A through the potentiometer wire, and from A, it flows through resistance R to the negative terminal of cell V. Let's assume the potential at point A is 0 V (VA=0V_A = 0). Then the potential at point C is VC=VAC=ϕxV_C = V_{AC} = \phi x. Applying KVL by moving from A through R, cell V, milliammeter, to C and back to A: Starting from A, moving in the direction of current I (A to R, then to V-, then to V+, then to mA, then to C, then to A): VAIR+VVC=0V_A - I \cdot R + V - V_C = 0 (Here, IR-IR is the potential drop across R, +V+V is the potential rise across the cell V, and VC-V_C is the potential drop from C to A, as we are moving from C to A along the wire to complete the loop from point A) Substituting VA=0V_A = 0 and VC=ϕxV_C = \phi x: 0IR+Vϕx=00 - I \cdot R + V - \phi x = 0 Vϕx=IRV - \phi x = I \cdot R I=VϕxRI = \frac{V - \phi x}{R}

3. Use the given graph to find V and R: The graph shows I (in mA) versus x (in cm). It is a straight line, which is consistent with our linear equation for I. The equation I=VRϕRxI = \frac{V}{R} - \frac{\phi}{R} x is in the form y=c+mxy = c + mx, where c=VRc = \frac{V}{R} (y-intercept) and m=ϕRm = -\frac{\phi}{R} (slope).

From the graph:

  • At x = 0 cm, I = 30 mA. Substituting these values into the current equation: 30×103 A=Vϕ(0)R30 \times 10^{-3} \text{ A} = \frac{V - \phi (0)}{R} 30×103=VR30 \times 10^{-3} = \frac{V}{R} (Equation 1)

  • At I = 0 mA, x = 20 cm (this is the null point). Substituting these values into the current equation: 0=Vϕ(20 cm)R0 = \frac{V - \phi (20 \text{ cm})}{R} Since R cannot be zero, the numerator must be zero: Vϕ(20)=0V - \phi (20) = 0 V=20ϕV = 20 \phi (Equation 2)

4. Calculate the values of V and R: Substitute the value of ϕ\phi into Equation 2: V=20 cm×0.12 V/cm=2.4 VV = 20 \text{ cm} \times 0.12 \text{ V/cm} = 2.4 \text{ V}

Now, substitute the value of V into Equation 1: 30×103=2.4 VR30 \times 10^{-3} = \frac{2.4 \text{ V}}{R} R=2.4 V30×103 A=2.40.03 Ω=2403 Ω=80 ΩR = \frac{2.4 \text{ V}}{30 \times 10^{-3} \text{ A}} = \frac{2.4}{0.03} \ \Omega = \frac{240}{3} \ \Omega = 80 \ \Omega

5. Verification (optional): The slope of the graph is m=ΔIΔx=030×103 A20 cm0 cm=30×10320 A/cm=1.5×103 A/cmm = \frac{\Delta I}{\Delta x} = \frac{0 - 30 \times 10^{-3} \text{ A}}{20 \text{ cm} - 0 \text{ cm}} = \frac{-30 \times 10^{-3}}{20} \text{ A/cm} = -1.5 \times 10^{-3} \text{ A/cm}. From our equation, the theoretical slope is m=ϕR=0.12 V/cm80 Ω=0.1280 A/cm=0.0015 A/cm=1.5×103 A/cmm = -\frac{\phi}{R} = -\frac{0.12 \text{ V/cm}}{80 \ \Omega} = -\frac{0.12}{80} \text{ A/cm} = -0.0015 \text{ A/cm} = -1.5 \times 10^{-3} \text{ A/cm}. The calculated values are consistent with the graph.

The values of V and R are 2.4 V and 80 Ω\Omega respectively.