Step 1: Find the angular acceleration.
The wheel starts from rest, so
\[
\omega_0=0.
\]
At
\[
t=2\ \text{s},
\]
the angular velocity is
\[
\omega=3.14\ \text{rad s}^{-1}.
\]
Using
\[
\omega=\omega_0+\alpha t,
\]
we get
\[
3.14=0+\alpha(2).
\]
Therefore,
\[
\alpha=\frac{3.14}{2}.
\]
\[
\alpha=1.57\ \text{rad s}^{-2}.
\]
Step 2: Find angular displacement from \(t=0\) to \(t=20\ \text{s}\).
Acceleration continues up to
\[
t=20\ \text{s}.
\]
Angular displacement during uniformly accelerated motion is
\[
\theta_1=\omega_0t+\frac{1}{2}\alpha t^2.
\]
Since
\[
\omega_0=0,
\]
we get
\[
\theta_1=\frac{1}{2}(1.57)(20)^2.
\]
\[
\theta_1=\frac{1}{2}\times 1.57 \times 400.
\]
\[
\theta_1=314\ \text{rad}.
\]
Step 3: Find angular velocity at \(t=20\ \text{s}\).
\[
\omega_{20}=\omega_0+\alpha t.
\]
\[
\omega_{20}=0+1.57(20).
\]
\[
\omega_{20}=31.4\ \text{rad s}^{-1}.
\]
Step 4: Find angular displacement from \(t=20\ \text{s}\) to \(t=40\ \text{s}\).
At \(t=20\ \text{s}\), acceleration is ceased.
So, from \(t=20\ \text{s}\) to \(t=40\ \text{s}\), the wheel moves with constant angular velocity
\[
\omega=31.4\ \text{rad s}^{-1}.
\]
Time interval is
\[
20\ \text{s}.
\]
Thus,
\[
\theta_2=\omega t.
\]
\[
\theta_2=31.4\times 20.
\]
\[
\theta_2=628\ \text{rad}.
\]
Step 5: Find total angular displacement.
\[
\theta=\theta_1+\theta_2.
\]
\[
\theta=314+628.
\]
\[
\theta=942\ \text{rad}.
\]
Step 6: Convert radians into revolutions.
One revolution is
\[
2\pi\ \text{rad}.
\]
Using
\[
\pi=3.14,
\]
we get
\[
2\pi=6.28\ \text{rad}.
\]
Number of revolutions is
\[
n=\frac{\theta}{2\pi}.
\]
\[
n=\frac{942}{6.28}.
\]
\[
n=150.
\]
Step 7: Final conclusion.
Therefore, the number of revolutions made by the wheel is
\[
\boxed{150}
\]
Hence, the correct option is
\[
\boxed{(4)}
\]