Given: The equation of motion of a particle executes SHM is x( t )=Acos( ωt+ϕ ). At t=0 the position of the particle is 1 cm. The initial velocity of the particle is ω cm/s and angular frequency of the particle is π s -1 .
The equation of SHM is given by,
x( t )=Acos( ωt+ϕ )(1)
Where, the displacement of particle is x( t ), the amplitude is A, the angular frequency is ω and the phase difference is ϕ.
According to given condition,
At t=0, x( 0 )=1 cm
By substituting the value of t as zero in equation (1), we get
x( 0 )=Acos( ω×0+ϕ ) 1=Acosϕ (2)
Differentiating equation (1) with respect to time, we get
By substituting the value of x( t ) in equation (3), we get
dx( t ) dt = d dt ( Acos( ωt+ϕ ) ) v( t )=−Aωsin( ωt+ϕ ) (3)
According to given condition,
At t=0, v( 0 )=ω cm/s
By substituting the given values in equation (3), we get
ω=−Aωsin( ω×0+ϕ ) −1=Asinϕ (4)
Square and add the equation (2) and equation (4).
A 2 ( cos 2 ϕ+ sin 2 ϕ )=1+1 A 2 =2 A= 2 cm
Divide equation (4) by equation (2).
tanϕ=−1 tanϕ=tan( 3π 4 ),tan( 7π 4 ),…
By comparing the terms on both the sides, we get
ϕ= 3π 4 , 7π 4 ,…
Thus, the amplitude and initial phase angle are 2 cm and 3π 4 , 7π 4 ,… respectively.
The general equation of Simple Harmonic Motion (SHM) is given by,
y=Bsin( ωt+α )(5)
Substitute y=1 at x=0 in equation (5).
1=Bsin( ω×0+α ) 1=Bsinα (6)
Differentiate the equation (5) with respect to time.
v= d dt ( Bsin( ωt+α ) ) =Bωcos( ωt+α )
Substitute v=ω at t=0 in above equation.
ω=Bωcos( ω×0+α ) 1=Bcosα (7)
Square and add the equation (6) and equation (7).
B 2 ( cos 2 ϕ+ sin 2 ϕ )=1+1 B 2 =2 B= 2 cm
Divide equation (6) by equation (7).
Bsinα Bcosα =1 tanα=1 tanα=tan( π 4 , 5π 4 ,… ) α= π 4 , 5π 4 ,…
Thus, the amplitude and initial phase angle are 2 cm and π 4 , 5π 4 ,… respectively.