The acceleration of particle in shm at 5 cm from its mean position is 20 cm per second square the value of angular frequency is
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Well this is a more simple problem than it may first appear to be.
Let's use the known relationship between acceleration, a, and displacement, x, of a simple harmonic mass.
a(x)=−ω2xa(x)=−ω2x
Where ωω is the angular frequency of the oscillation and the negative sign shows that the mass is always accelerated towards the centre of oscillation (for a pendulum, this is caused by gravity).
Now we just substitute in your values and see if we can find the angular frequency.
I'm assuming, since you omitted a minus sign in your acceleration or displacement that the mass is at a positive displacement of x=4cmx=4cm with a negative acceleration of a=−64cms−2.a=−64cms−2.
Therefore:
a(4)=−ω2×4=−64a(4)=−ω2×4=−64
This implies:
ω=4rads/sω=4rads/s
Now,
ω=2πTω=2πT
Where TT is the time period we're looking for.
Therefore, the time period is:
T=2πω=π2sT=2πω=π2s
This is approximately a period of 1.57 seconds.
As a side note, the time period of oscillation is independent of starting displacement. It is related to the restoring force of the oscillation and/or the mass oscillating.
For instance, for a simple pendulum, the time period is given by:
T=2πlg−−√T=2πlg
Where ll is the length of the pendulum and gg is the gravitational field strength (10 N/kg or 10 ms−2ms−2 on Earth's surface).
Let's use the known relationship between acceleration, a, and displacement, x, of a simple harmonic mass.
a(x)=−ω2xa(x)=−ω2x
Where ωω is the angular frequency of the oscillation and the negative sign shows that the mass is always accelerated towards the centre of oscillation (for a pendulum, this is caused by gravity).
Now we just substitute in your values and see if we can find the angular frequency.
I'm assuming, since you omitted a minus sign in your acceleration or displacement that the mass is at a positive displacement of x=4cmx=4cm with a negative acceleration of a=−64cms−2.a=−64cms−2.
Therefore:
a(4)=−ω2×4=−64a(4)=−ω2×4=−64
This implies:
ω=4rads/sω=4rads/s
Now,
ω=2πTω=2πT
Where TT is the time period we're looking for.
Therefore, the time period is:
T=2πω=π2sT=2πω=π2s
This is approximately a period of 1.57 seconds.
As a side note, the time period of oscillation is independent of starting displacement. It is related to the restoring force of the oscillation and/or the mass oscillating.
For instance, for a simple pendulum, the time period is given by:
T=2πlg−−√T=2πlg
Where ll is the length of the pendulum and gg is the gravitational field strength (10 N/kg or 10 ms−2ms−2 on Earth's surface).
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Hi there..
I hope it's the right answer..
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