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The emf of a cell is epsilon and its int...

The emf of a cell is `epsilon` and its internal resistance is r. its termnals are cannected to a resistance R. The potential difference between the terminals is `1.6V for R = 4 Omega, and 1.8 V for R = 9 Omega. Then,

A

`epsilon =1 V, r = 1 Omega`

B

`epsilon =2V, r = 1 Omega`

C

`epsilon =2 V, r =2Omega`

D

`epsilon =2.5 V, r = 0.5 Omega`

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To solve the problem, we will use the concepts of electromotive force (emf), internal resistance, and Ohm's law. Let's break down the solution step by step. ### Step 1: Write the equations for the two cases We know that the potential difference (V) across the external resistor (R) can be expressed as: \[ V = \epsilon - I \cdot r \] Where: - \( \epsilon \) is the emf of the cell, - \( I \) is the current flowing through the circuit, - \( r \) is the internal resistance of the cell. The current \( I \) can be calculated using Ohm's law: \[ I = \frac{V}{R} \] ### Step 2: Set up the equations for the two given scenarios For the first case where \( R = 4 \, \Omega \) and \( V = 1.6 \, V \): \[ 1.6 = \epsilon - I \cdot r \] Substituting \( I \): \[ 1.6 = \epsilon - \left(\frac{1.6}{4}\right) r \] This simplifies to: \[ 1.6 = \epsilon - 0.4r \] Rearranging gives us: \[ \epsilon = 1.6 + 0.4r \quad \text{(Equation 1)} \] For the second case where \( R = 9 \, \Omega \) and \( V = 1.8 \, V \): \[ 1.8 = \epsilon - I \cdot r \] Substituting \( I \): \[ 1.8 = \epsilon - \left(\frac{1.8}{9}\right) r \] This simplifies to: \[ 1.8 = \epsilon - 0.2r \] Rearranging gives us: \[ \epsilon = 1.8 + 0.2r \quad \text{(Equation 2)} \] ### Step 3: Equate the two equations Since both expressions equal \( \epsilon \), we can set them equal to each other: \[ 1.6 + 0.4r = 1.8 + 0.2r \] ### Step 4: Solve for \( r \) Rearranging the equation: \[ 0.4r - 0.2r = 1.8 - 1.6 \] This simplifies to: \[ 0.2r = 0.2 \] Dividing both sides by 0.2 gives: \[ r = 1 \, \Omega \] ### Step 5: Substitute \( r \) back to find \( \epsilon \) Now we can substitute \( r = 1 \, \Omega \) back into either Equation 1 or Equation 2 to find \( \epsilon \). Using Equation 1: \[ \epsilon = 1.6 + 0.4(1) \] This simplifies to: \[ \epsilon = 1.6 + 0.4 = 2.0 \, V \] ### Conclusion Thus, the values we have found are: - The emf of the cell \( \epsilon = 2.0 \, V \) - The internal resistance \( r = 1 \, \Omega \)

To solve the problem, we will use the concepts of electromotive force (emf), internal resistance, and Ohm's law. Let's break down the solution step by step. ### Step 1: Write the equations for the two cases We know that the potential difference (V) across the external resistor (R) can be expressed as: \[ V = \epsilon - I \cdot r \] Where: - \( \epsilon \) is the emf of the cell, - \( I \) is the current flowing through the circuit, ...
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