Step 1: Apply the wave equation to the solution.
The wave equation requires that \( u_{tt} = 9 u_{xx} \), so we need to differentiate the given solution twice with respect to \( t \) and \( x \), respectively.
First, differentiate \( u(x, t) \) with respect to \( t \):
\[
u_t(x, t) = \frac{1}{2} \left[ g'(x + ct) \cdot c - g'(x - ct) \cdot (-c) \right]
= \frac{c}{2} \left[ g'(x + ct) + g'(x - ct) \right].
\]
Now, differentiate \( u_t(x, t) \) with respect to \( t \) again to find \( u_{tt} \):
\[
u_{tt}(x, t) = \frac{c^2}{2} \left[ g''(x + ct) + g''(x - ct) \right].
\]
Step 2: Differentiate \( u(x, t) \) with respect to \( x \).
Now, differentiate \( u(x, t) \) with respect to \( x \):
\[
u_x(x, t) = \frac{1}{2} \left[ g'(x + ct) - g'(x - ct) \right].
\]
Now, differentiate \( u_x(x, t) \) with respect to \( x \) again to find \( u_{xx} \):
\[
u_{xx}(x, t) = \frac{1}{2} \left[ g''(x + ct) + g''(x - ct) \right].
\]
Step 3: Substitute into the wave equation.
We substitute the expressions for \( u_{tt} \) and \( u_{xx} \) into the wave equation \( u_{tt} = 9 u_{xx} \):
\[
\frac{c^2}{2} \left[ g''(x + ct) + g''(x - ct) \right] = 9 \cdot \frac{1}{2} \left[ g''(x + ct) + g''(x - ct) \right].
\]
Canceling the common factor of \( \frac{1}{2} \) and solving for \( c^2 \), we get:
\[
c^2 = 9.
\]
Thus, the value of \( c^2 \) is \( 9 \).
If \( u(x,t) = A e^{-t} \sin x \) solves the following initial boundary value problem:
\[ \frac{\partial u}{\partial t} = \frac{\partial^2 u}{\partial x^2}, 0 < x < \pi, t > 0, \] \[ u(0,t) = u(\pi,t) = 0, t > 0, \] \[ u(x,0) = \begin{cases} 60, & 0 < x \leq \frac{\pi}{2}, \\ 40, & \frac{\pi}{2} < x < \pi, \end{cases} \] then \( \pi A = \underline{\hspace{1cm}} \).