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At time $$t = 0$$ magnetic field of 1000 Gauss is passing perpendicularly through the area defined by the closed loop shown in the figure. If the magnetic field reduces linearly to 500 Gauss, in the next 5s, then induced EMF in the loop is:
Minimum Required Theory
$$\varepsilon = \frac{\Delta \Phi}{\Delta t} = A \frac{\Delta B}{\Delta t}$$
Step-by-Step Solution
Step 1: Calculate the effective area ($$A$$) of the closed loop
The geometry consists of a large main rectangle from which a smaller inner rectangular section has been subtracted (or indented).
$$\text{Net Area } A = 64\text{ cm}^2 - 8\text{ cm}^2 = 56\text{ cm}^2$$
Convert the area to SI units ($$\text{m}^2$$):
$$A = 56 \times 10^{-4}\text{ m}^2$$
Step 2: Determine the rate of change of the magnetic field ($$\frac{\Delta B}{\Delta t}$$)
The magnetic field decreases linearly from $$1000\text{ G}$$ to $$500\text{ G}$$ over a time interval $$\Delta t = 5\text{ s}$$.
$$\Delta B = 1000\text{ G} - 500\text{ G} = 500\text{ G}$$
Convert $$\Delta B$$ to Tesla (T):
$$\Delta B = 500 \times 10^{-4}\text{ T}$$
Now, calculate the rate of change:
$$\frac{\Delta B}{\Delta t} = \frac{500 \times 10^{-4}\text{ T}}{5\text{ s}} = 100 \times 10^{-4}\text{ T/s}$$
Step 3: Compute the induced EMF ($$\varepsilon$$)
Substitute the values into Faraday's formula:
$$\varepsilon = A \times \frac{\Delta B}{\Delta t}$$
$$\varepsilon = (56 \times 10^{-4}\text{ m}^2) \times (100 \times 10^{-4}\text{ T/s})$$
$$\varepsilon = 5600 \times 10^{-8}\text{ V}$$
$$\varepsilon = 56 \times 10^{-6}\text{ V}$$
Step 4: Convert to microvolts ($$\mu\text{V}$$)
Since $$10^{-6}\text{ V} = 1\text{ }\mu\text{V}$$:
$$\varepsilon = 56\text{ }\mu\text{V}$$
Final Answer
The induced EMF in the loop is $$56\text{ }\mu\text{V}$$.
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