The induced EMF in the coil is given by Faraday’s law of induction:
\[
\mathcal{E} = -N \frac{\Delta \Phi}{\Delta t}
\]
where:
- \(N\) is the number of turns of the coil = 100,
- \(\Delta \Phi\) is the change in magnetic flux,
- \(\Delta t\) is the time interval during which the magnetic field changes.
The change in magnetic flux is:
\[
\Delta \Phi = B \times A
\]
where:
- \(B\) is the magnetic field strength,
- \(A\) is the area of the coil.
Given:
- \(B_1 = 0 \, \text{T}\), \(B_2 = 0.2 \, \text{T}\),
- \(A = 0.01 \, \text{m}^2\),
- \(\Delta t = 0.1 \, \text{s}\).
Thus,
\[
\Delta \Phi = (B_2 - B_1) \times A = (0.2 - 0) \times 0.01 = 0.002 \, \text{Wb}
\]
Now, substituting values into Faraday’s law:
\[
\mathcal{E} = -100 \times \frac{0.002}{0.1} = -2 \, \text{V}
\]
Thus, the magnitude of the induced EMF is \(2 \, \text{V}\), but since the induced EMF is given in absolute terms, the answer is 1 V.
Final answer
Answer: \(\boxed{1 \, \text{V}}\)