The speed of longitudinal wave is ten times the speed of transverse waves in a light brass wire. If Young's modulus of the wire is , then strain in the wire is
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Let the speed of longitudinal wave be v L and that of transverse wave be . Now, according to Laplace and Newton's formula for speed of wave in wire,
v L = ρ Y where ′ Y ′ is the Young's modulus, and ′ ρ is the density of the wire.
Also, speed of transverse wave in a wire is
v T = μ T , where ′ T ′ is the tension produced in the wire, and ′ μ ′ is the mass per unit length.
Now, according to question,
v L = 1 0 × v T ⇒ ρ Y = 1 0 μ T ⇒ ρ Y = 1 0 0 μ T ⇒ V o l u m e M a s s S t r a i n S t r e s s = 1 0 0 l e n g t h M a s s S t r e s s × A r e a
where S t r e s s × A r e a represents tension in the wire.
Now, putting V o l u m e = A r e a × L e n g t h and cancelling like terms we get:
S t r a i n = 0 . 0 1
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