The particle executing Simple Harmonic Motion in a straight line has velocities at three points distant one metre from each other. If is the maximum velocity of the particle then find .
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Let's call the points with 8 m / s , 7 m / s , 4 m / s as A , B , C respectively.
Let h be the displacement of point A from the mean position.
It follows that the displacements of B and C from the mean position are ( h + 1 ) and ( h + 2 ) respectively.
Using: v = ω A 2 − x 2 where v is instantaneous velocity, A is amplitude from mean position, ω is the angular frequency and x is displacement from mean position:
8 = ω A 2 − h 2 ⟹ 6 4 = A 2 ω 2 − h 2 ω 2 ( 1 ) 7 = ω A 2 − ( h + 1 ) 2 ⟹ 4 9 = A 2 ω 2 − ( h + 1 ) 2 ω 2 ( 2 ) 4 = ω A 2 − ( h + 2 ) 2 ⟹ 1 6 = A 2 ω 2 − ( h + 2 ) 2 ω 2 ( 3 )
Subtracting ( 2 ) from ( 1 ) :
1 5 = ( 2 h + 1 ) ω 2 ( 4 )
Subtracting ( 3 ) from ( 2 ) :
3 3 = ( 2 h + 3 ) ω 2 ( 5 )
Dividing ( 5 ) by ( 4 ) :
1 5 3 3 = 2 h + 1 2 h + 3 ⟹ h = 3 1
Substituting the above in ( 4 ) :
1 5 = 9 1 5 ω 2 ⟹ ω = 3
Substituing the values of h and ω in ( 1 ) gives A = 3 6 5 .
The maximum velocity V is at the mean position and is given by V = A ω .
∴ V = 6 5 ⟹ ⌊ V ⌋ = 8