
The induced electromotive force (EMF) in the rod is given by the formula: \[ \text{EMF} = B \times v \times l \] Where:
\( B \) is the magnetic field strength (0.04 T),
\( v \) is the velocity of the rod (5 ms\(^{-1}\)),
\( l \) is the length of the rod (2 m).
Substituting the values: \[ \text{EMF} = 0.04 \times 5 \times 2 = 0.4 \, \text{V} \] Now, using Ohm’s Law, the current through the rod is: \[ I = \frac{\text{EMF}}{R} = \frac{0.4}{3} = 0.1333 \, \text{A} = 133 \, \text{mA} \] Thus, the current through the rod is 133 mA.
The induced EMF \( \mathcal{E} \) in the moving rod can be calculated using the formula for motional EMF: \[ \mathcal{E} = B \cdot L \cdot v \] where:
\( B \) is the magnetic field strength (\( 0.04 \, \text{T} \)),
\( L \) is the length of the rod (\( 2 \, \text{m} \)),
\( v \) is the velocity of the rod (\( 5 \, \text{ms}^{-1} \)).
Substituting the given values: \[ \mathcal{E} = 0.04 \cdot 2 \cdot 5 = 0.4 \, \text{V} \] Now, the current \( I \) through the rod can be found using Ohm's law: \[ I = \frac{\mathcal{E}}{R} \] where \( R \) is the resistance of the rod (\( 3 \, \Omega \)). Substituting the values: \[ I = \frac{0.4}{3} = 0.133 \, \text{A} = 133 \, \text{mA} \] Thus, the current through the rod is \( 133 \, \text{mA} \).
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