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The data in [link] can still be modeled with a periodic function, like a cosine function, but the function is shifted to the right. This shift is known as a phase shift and is usually represented by the Greek letter phi . The equation of the position as a function of time for a block on a spring becomes
This is the generalized equation for SHM where t is the time measured in seconds, is the angular frequency with units of inverse seconds, A is the amplitude measured in meters or centimeters, and is the phase shift measured in radians ( [link] ). It should be noted that because sine and cosine functions differ only by a phase shift, this motion could be modeled using either the cosine or sine function.
The velocity of the mass on a spring, oscillating in SHM, can be found by taking the derivative of the position equation:
Because the sine function oscillates between –1 and +1, the maximum velocity is the amplitude times the angular frequency, . The maximum velocity occurs at the equilibrium position when the mass is moving toward . The maximum velocity in the negative direction is attained at the equilibrium position when the mass is moving toward and is equal to .
The acceleration of the mass on the spring can be found by taking the time derivative of the velocity:
The maximum acceleration is . The maximum acceleration occurs at the position , and the acceleration at the position and is equal to .
In summary, the oscillatory motion of a block on a spring can be modeled with the following equations of motion:
Here, A is the amplitude of the motion, T is the period, is the phase shift, and is the angular frequency of the motion of the block.
Work is done on the block, pulling it out to The block is released from rest and oscillates between and The period of the motion is 1.57 s. Determine the equations of motion.
All that is left is to fill in the equations of motion:
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