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Mechanical Properties Of Fluids

Question
CBSEENPH11020203

In Exercise 14.9, let us take the position of mass when the spring is unstretched as x = 0, and the direction from left to right as the positive direction of x-axis.

Give as a function of time t for the oscillating mass if at the moment we start the stopwatch (= 0), the mass is, 

(a) at the mean position, 

(b) at the maximum stretched position, and

(c) at the maximum compressed position. 

In what way do these functions for SHM differ from each other, in frequency, in amplitude or the initial phase?

Solution
Distance travelled by the mass sideways, a = 2.0 cm 
Angular frequency of oscillation, 
straight omega space equals space square root of straight k over straight m end root space

space space space space equals space square root of 1200 over 3 end root space

space space space space equals square root of 400 space

space space space space space equals space 20 space rad divided by sec 
 
(a)
As time is noted from the mean position, hence using 
           x = a sin ω t, we have x = 2 sin 20 t
 
(b)
At maximum stretched position, the body is at the extreme right position, with an intial phase of π/2 rad.
Then, 
straight x space equals space straight a space sin space open parentheses ωt space plus straight pi over 2 close parentheses space
space space space space equals space straight a space cos space ωt
space
space space space space equals space 2 space cos space 20 space straight t 

(c) At maximum compressed position, the body is at left position, with an initial phase of 3 π/2 rad.
Then, 
straight x space equals space straight a space sin space open parentheses ωt space plus space fraction numerator 3 straight pi over denominator 2 end fraction close parentheses space

space space space equals space minus space straight a space cos space ωt space

space space space equals space minus space 2 space cos space 20 space straight t
 
The functions neither differ in amplitude nor in frequency.
 They differ in initial phase.