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An ideal coil of 10H is connected in ser...

An ideal coil of 10H is connected in series with a resistance of `5(Omega)` and a battery of 5V. 2second after the connections is made, the current flowing in ampere in the circuit is

A

`(1-e^(-1))`

B

`(1-e)`

C

`e`

D

`e^(-1)`

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The correct Answer is:
To solve the problem, we need to find the current flowing in the circuit 2 seconds after the connection is made. We will use the formula for the current in an LR circuit, which is given by: \[ I(t) = I_0 \left(1 - e^{-\frac{R}{L}t}\right) \] Where: - \( I(t) \) is the current at time \( t \), - \( I_0 \) is the maximum current, - \( R \) is the resistance, - \( L \) is the inductance, - \( e \) is the base of the natural logarithm, - \( t \) is the time. ### Step 1: Determine the maximum current \( I_0 \) The maximum current \( I_0 \) in the circuit can be calculated using Ohm's law: \[ I_0 = \frac{E}{R} \] Where: - \( E = 5V \) (the voltage of the battery), - \( R = 5 \Omega \) (the resistance). Substituting the values: \[ I_0 = \frac{5V}{5 \Omega} = 1A \] ### Step 2: Substitute values into the current formula Now we substitute \( I_0 \), \( R \), \( L \), and \( t \) into the current formula: \[ I(t) = 1 \left(1 - e^{-\frac{5}{10} \cdot 2}\right) \] ### Step 3: Simplify the exponent Calculate the exponent: \[ -\frac{R}{L} \cdot t = -\frac{5}{10} \cdot 2 = -1 \] ### Step 4: Calculate the current Now substitute the exponent back into the equation: \[ I(t) = 1 \left(1 - e^{-1}\right) \] ### Step 5: Evaluate \( e^{-1} \) Using the approximate value of \( e \approx 2.718 \): \[ e^{-1} \approx \frac{1}{2.718} \approx 0.3679 \] Thus: \[ I(t) = 1 \left(1 - 0.3679\right) \] \[ I(t) \approx 1 \times 0.6321 \] \[ I(t) \approx 0.6321A \] ### Final Answer The current flowing in the circuit after 2 seconds is approximately **0.6321 A**. ---

To solve the problem, we need to find the current flowing in the circuit 2 seconds after the connection is made. We will use the formula for the current in an LR circuit, which is given by: \[ I(t) = I_0 \left(1 - e^{-\frac{R}{L}t}\right) \] Where: - \( I(t) \) is the current at time \( t \), - \( I_0 \) is the maximum current, - \( R \) is the resistance, ...
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