Step 1: Define the DC component.
The DC component of a periodic signal is its average value over one period. For a signal \(x(t)\) with period \(T_0\), the DC component, often denoted as \(a_0\), is calculated by the formula:
\[
a_0 = \frac{1}{T_0} \int_{T_0} x(t) \,dt
\]
where the integral is taken over any interval of length \(T_0\). We can choose the interval \( [-\frac{T_0}{2}, \frac{T_0}{2}] \).
Step 2: Set up the integral based on the signal definition.
The signal \(x(t)\) is 1 for \(|t|<T_1\) (which means \(-T_1<t<T_1\)) and 0 otherwise within the period. So, the integral is non-zero only in the range from \(-T_1\) to \(T_1\).
\[
a_0 = \frac{1}{T_0} \int_{-T_0/2}^{T_0/2} x(t) \,dt = \frac{1}{T_0} \int_{-T_1}^{T_1} (1) \,dt
\]
Step 3: Evaluate the integral.
\[
a_0 = \frac{1}{T_0} \left[ t \right]_{-T_1}^{T_1}
\]
\[
a_0 = \frac{1}{T_0} (T_1 - (-T_1)) = \frac{1}{T_0} (2T_1) = \frac{2T_1}{T_0}
\]
This matches option (C).