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Two batteries (connected in series) of same emf 10 V of internal resistances `20ohm` and `5ohm` are connected to a load resistance of `30ohm`. Now an unknown resistance x is connected in parallel to the load resistance. Find value of x so that potential drop of battery having internal resistance `20ohm` becomes zero.

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To solve the problem, we need to find the value of the unknown resistance \( x \) that, when connected in parallel to a load resistance of \( 30 \, \Omega \), causes the potential drop across the battery with an internal resistance of \( 20 \, \Omega \) to become zero. ### Step-by-Step Solution: 1. **Understanding the Circuit**: We have two batteries connected in series, each with an emf of \( 10 \, V \). The internal resistances are \( R_1 = 20 \, \Omega \) and \( R_2 = 5 \, \Omega \). A load resistance \( R_L = 30 \, \Omega \) is connected, and we need to find the resistance \( x \) that is connected in parallel to \( R_L \). 2. **Condition for Zero Potential Drop**: For the potential drop across the battery with internal resistance \( R_1 \) (i.e., \( 20 \, \Omega \)) to be zero, the voltage across it must equal its emf: \[ V_1 = E_1 - I \cdot R_1 = 0 \] where \( E_1 = 10 \, V \) and \( R_1 = 20 \, \Omega \). 3. **Finding the Current \( I \)**: Rearranging the equation gives: \[ I \cdot R_1 = E_1 \implies I = \frac{E_1}{R_1} = \frac{10 \, V}{20 \, \Omega} = 0.5 \, A \] 4. **Calculating Voltage Across the Second Battery**: Now, we can find the voltage drop across the second battery with internal resistance \( R_2 = 5 \, \Omega \): \[ V_2 = E_2 - I \cdot R_2 = 10 \, V - 0.5 \, A \cdot 5 \, \Omega = 10 \, V - 2.5 \, V = 7.5 \, V \] 5. **Applying Kirchhoff's Current Law**: Let \( I_1 \) be the current through the load resistance \( R_L \) and \( I_2 \) be the current through the unknown resistance \( x \). According to Kirchhoff's current law: \[ I = I_1 + I_2 \] where \( I = 0.5 \, A \). 6. **Finding Currents Through \( R_L \) and \( x \)**: The current through the load resistance \( R_L \) is given by: \[ I_1 = \frac{V_2}{R_L} = \frac{7.5 \, V}{30 \, \Omega} = 0.25 \, A \] The current through the unknown resistance \( x \) is: \[ I_2 = I - I_1 = 0.5 \, A - 0.25 \, A = 0.25 \, A \] 7. **Finding the Value of \( x \)**: Using Ohm's law for the current through \( x \): \[ I_2 = \frac{V_2}{x} \implies 0.25 \, A = \frac{7.5 \, V}{x} \] Rearranging gives: \[ x = \frac{7.5 \, V}{0.25 \, A} = 30 \, \Omega \] ### Final Answer: The value of the unknown resistance \( x \) is \( 30 \, \Omega \).

To solve the problem, we need to find the value of the unknown resistance \( x \) that, when connected in parallel to a load resistance of \( 30 \, \Omega \), causes the potential drop across the battery with an internal resistance of \( 20 \, \Omega \) to become zero. ### Step-by-Step Solution: 1. **Understanding the Circuit**: We have two batteries connected in series, each with an emf of \( 10 \, V \). The internal resistances are \( R_1 = 20 \, \Omega \) and \( R_2 = 5 \, \Omega \). A load resistance \( R_L = 30 \, \Omega \) is connected, and we need to find the resistance \( x \) that is connected in parallel to \( R_L \). 2. **Condition for Zero Potential Drop**: ...
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