Q.A steel rod long is clamped at its middle. The fundamental frequency of longitudinal vibrations of the rod are given to be . What is the speed of sound in steel?
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Start your 14-day free trial to unlock the full solution →The rod is clamped at the centre, so the centre is a node and the free ends are antinodes. This makes the rod length equal to half the wavelength. Using , the speed of sound in steel comes out to .
The key idea here is to connect the physical setup — a rod clamped at the middle — to the standing wave pattern it supports. When you clamp a rod at its centre, that point cannot move. In a longitudinal wave, a point that cannot move is a displacement node. The free ends, on the other hand, can vibrate freely, so they are displacement antinodes.
So the rod is supporting a standing wave with a node at the centre and antinodes at both ends. That means the length of the rod is exactly half a wavelength: from one antinode to the next antinode is , and the rod spans exactly that distance.
For a rod clamped at the centre, fundamental mode:
Now let’s work through the numbers.
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Identify the given data
Length of rod:
Fundamental frequency:
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Relate length to wavelength
As argued, for the fundamental mode:
So
- Apply the wave speed formula For any wave, . …
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