Concept:
The problem asks for the Laplace transform of a shifted function multiplied by a unit step function \( u(t-a) \) (also written as \( H(t-a) \)). To solve this, we use the Second Shifting Theorem of Laplace transforms:
\[
\mathcal{L}\{ f(t-a) u(t-a) \} = e^{-as} \mathcal{L}\{ f(t) \} = e^{-as} F(s)
\]
Additionally, we use the standard Laplace transform for a sine wave function:
\[
\mathcal{L}\{ \sin(\omega t) \} = \frac{\omega}{s^2 + \omega^2}
\]
Step 1: Identifying the parameters from the given function.
The given expression to transform is:
\[
\mathcal{L}\{ \sin(t-3)u(t-3) \}
\]
By comparing this directly with the standard formula \( f(t-a)u(t-a) \), we can identify our parameters:
• The shift constant is \( a = 3 \).
• The shifted function is \( f(t-3) = \sin(t-3) \).
Replacing \( (t-3) \) with an unshifted variable \( t \) gives the base function:
\[
f(t) = \sin(t)
\]
Step 2: Finding the Laplace transform of the unshifted base function \( f(t) \).
Now, let us calculate the Laplace transform \( F(s) \) of our base function \( f(t) = \sin(t) \). Here, the frequency coefficient is \( \omega = 1 \):
\[
F(s) = \mathcal{L}\{ \sin(t) \} = \frac{1}{s^2 + 1^2} = \frac{1}{s^2 + 1}
\]
Step 3: Applying the Second Shifting Theorem formula.
Now we combine our results using the Second Shifting Theorem:
\[
\mathcal{L}\{ \sin(t-3)u(t-3) \} = e^{-3s} F(s)
\]
Substituting our calculated value for \( F(s) \):
\[
\mathcal{L}\{ \sin(t-3)u(t-3) \} = e^{-3s} \cdot \left( \frac{1}{s^2 + 1} \right) = \frac{e^{-3s}}{s^2 + 1}
\]
This final form matches Option (C).