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1 meter long metallic wire is broken in...

`1` meter long metallic wire is broken into two unequal parts `P and Q. P` part of the wire in uniformly extended into another wire `R`. Length of `R` is twice the length of `P` and the resistance of `R` is equal to that of `Q`. Find the ratio of the resistance `P` and `R` and also the ratio of the length `P and Q`

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To solve the problem, let's break it down step by step. ### Step 1: Define the lengths of the wire parts Let the length of part P be \( L \) meters. Since the total length of the wire is 1 meter, the length of part Q will be: \[ L_Q = 1 - L \] ### Step 2: Define the length of wire R According to the problem, the length of wire R is twice the length of wire P: \[ L_R = 2L \] ### Step 3: Calculate the area of wire R Since wire R is made from part P, we need to consider the volume conservation. The volume of wire P is equal to the volume of wire R: \[ \text{Volume of P} = \text{Volume of R} \] \[ A_P \cdot L = A_R \cdot L_R \] Substituting \( L_R = 2L \): \[ A_P \cdot L = A_R \cdot 2L \] Cancelling \( L \) from both sides (assuming \( L \neq 0 \)): \[ A_P = 2A_R \] Thus, the area of wire R is: \[ A_R = \frac{A_P}{2} \] ### Step 4: Calculate the resistance of wires P and R The resistance \( R \) of a wire is given by the formula: \[ R = \frac{\rho L}{A} \] Where \( \rho \) is the resistivity, \( L \) is the length, and \( A \) is the cross-sectional area. #### Resistance of wire P: \[ R_P = \frac{\rho L}{A_P} \] #### Resistance of wire R: Substituting \( L_R = 2L \) and \( A_R = \frac{A_P}{2} \): \[ R_R = \frac{\rho (2L)}{A_R} = \frac{\rho (2L)}{\frac{A_P}{2}} = \frac{4\rho L}{A_P} \] ### Step 5: Find the ratio of the resistances \( R_P \) and \( R_R \) Now we can find the ratio of the resistances: \[ \frac{R_P}{R_R} = \frac{\frac{\rho L}{A_P}}{\frac{4\rho L}{A_P}} = \frac{1}{4} \] ### Step 6: Find the ratio of lengths \( P \) and \( Q \) From our earlier definition, we have: \[ L_Q = 1 - L \] Now we can express the ratio of lengths \( P \) and \( Q \): \[ \frac{L_P}{L_Q} = \frac{L}{1 - L} \] Since we know the resistance of wire R is equal to the resistance of wire Q, we can set up the equation: \[ R_R = R_Q \] Substituting the expressions for resistance: \[ \frac{4\rho L}{A_P} = \frac{\rho (1 - L)}{A_Q} \] Assuming the areas are equal (for simplicity), we can cancel \( \rho \) and rearrange: \[ 4L = 1 - L \] Solving for \( L \): \[ 5L = 1 \implies L = \frac{1}{5} \] Thus, the length of Q is: \[ L_Q = 1 - L = 1 - \frac{1}{5} = \frac{4}{5} \] Now we can find the ratio: \[ \frac{L_P}{L_Q} = \frac{\frac{1}{5}}{\frac{4}{5}} = \frac{1}{4} \] ### Final Ratios 1. The ratio of the resistances \( R_P \) and \( R_R \) is \( \frac{1}{4} \). 2. The ratio of the lengths \( P \) and \( Q \) is \( \frac{1}{4} \).
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