A mass is suspended on a spring, pulled downward from its equilibrium position, and released. Assume that t = 0 when the spring is released, and the frequency of oscillation is w. Assume a vertical coordinate system in which the coordinate y points upward (see diagram at left).
Match the following physical quantities with their functional form.
Vertical Acceleration d^2y/dt^2 Vertical Velocity dy/dt Vertical position y Total Energy |
|
A. |
cos wt |
B. |
-sin wt |
C. |
Constant |
D. |
sin wt |
E. |
-cos (wt) |
When released the body has maximum acceleration and accelerates
upwards hence the function of acceleration
is cos(wt)
Vertical Acceleration d^2y/dt^2 ----> a) cos(wt)
Vertical velocity is minimum and increases sinosoidally as the
body moves upward so the function is
sin(wt)
Vertical Velocity dy/dt -----> d)sin(wt)
Vertical position is at a minimum (negative extreme if mean
position is taken as zero)
and increases sinosoidally hence the function describing the motion
is
-cos(wt)
Vertical position y -----> e)-cos(wt)
Total energy is a constant.
It is the sum of kinetic and potential energy; though energy
changes form from kinetic to potential and vice-versa
their sum is a constant.
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