Step 1: Recall the definition of signal energy.
The energy of a continuous-time signal $f(t)$ is defined as:
\[
E = \int_{-\infty}^{\infty} |f(t)|^2 \, dt
\]
Step 2: Apply time scaling property.
For a time-scaled signal $f(at)$, the energy becomes:
\[
E_a = \int_{-\infty}^{\infty} |f(at)|^2 \, dt
\]
Step 3: Perform change of variable.
Let $u = at \Rightarrow dt = \frac{du}{a}$. Hence,
\[
E_a = \frac{1}{|a|} \int_{-\infty}^{\infty} |f(u)|^2 \, du
\]
Step 4: Substitute the given value.
Here, $a = 2$. Therefore,
\[
E_{f(2t)} = \frac{1}{2} E
\]
Step 5: Final conclusion.
Thus, the energy of the signal $f(2t)$ is $E/2$.