We analyze the equation for a stationary wave on a string:
\[
y = 5 \sin \left( \frac{\pi x}{3} \right) \cos (40 \pi t)
\]
The standard form for a stationary wave is:
\[
y = A \sin(kx) \cos(\omega t)
\]
where:
- \( A \) is the amplitude,
- \( k \) is the wave number,
- \( \omega \) is the angular frequency,
- \( x \) is position,
- \( t \) is time.
Comparing the given equation:
\[
y = 5 \sin \left( \frac{\pi x}{3} \right) \cos (40 \pi t)
\]
We find:
- \( A = 5 \),
- \( k = \frac{\pi}{3} \),
- \( \omega = 40 \pi \).
Nodes in a stationary wave are points of zero displacement. Nodes occur when the sine term is zero:
\[
\sin(kx) = 0
\]
This gives:
\[
kx = n\pi, \quad n = 0, 1, 2, 3, \dots
\]
Solving for \( x \):
\[
x = \frac{n\pi}{k} = \frac{n\pi}{\frac{\pi}{3}} = 3n \, \text{cm}
\]
The nodes are at \( x = 0, 3, 6, 9, \dots \).
The distance between adjacent nodes (e.g., between \( x = 0 \) and \( x = 3 \)):
\[
\text{Separation between nodes} = 3 \, \text{cm}
\]
Therefore, the answer is 3 cm.