We are given the equation of a stationary wave along a stretched string:
\[
y = 5 \sin \left( \frac{\pi x}{3} \right) \cos (40 \pi t)
\]
% Step 1: General Form of a Stationary Wave
The general equation of a stationary wave is of the form:
\[
y = A \sin(kx) \cos(\omega t)
\]
where:
- \( A \) is the amplitude of the wave,
- \( k \) is the wave number,
- \( \omega \) is the angular frequency,
- \( x \) is the position along the string,
- \( t \) is the time.
In this case, comparing the given equation with the general form:
\[
y = 5 \sin \left( \frac{\pi x}{3} \right) \cos (40 \pi t)
\]
We identify:
- The amplitude \( A = 5 \),
- The wave number \( k = \frac{\pi}{3} \),
- The angular frequency \( \omega = 40 \pi \).
% Step 2: Distance Between Adjacent Nodes
In a stationary wave, nodes are points where the displacement is always zero. These occur when the sine term is zero. Thus, the condition for a node is:
\[
\sin(kx) = 0
\]
The general solution to this is:
\[
kx = n\pi, \quad n = 0, 1, 2, 3, \dots
\]
Solving for \( x \), we get:
\[
x = \frac{n\pi}{k} = \frac{n\pi}{\frac{\pi}{3}} = 3n \, \text{cm}
\]
Thus, the nodes are located at \( x = 0, 3, 6, 9, \dots \).
The separation between two adjacent nodes is the distance between two consecutive values of \( x \). For example, the distance between \( x = 0 \) and \( x = 3 \) is:
\[
\text{Separation between nodes} = 3 \, \text{cm}
\]
Thus, the correct answer is 3 cm.