The maximum speed of a particle in S.H.M. is V. The average speed is
\(\frac {3V}{π}\)
\(\frac {4V}{π}\)
\(\frac {V}{π}\)
\(\frac {2V}{π}\)
In SHM, the displacement of the particle
x(t) = A sin(ωt)
The velocity of the particle at any given time t:
v(t) = \(\frac {dx}{dt}\) = Aω cos(ωt)
The maximum speed (Vmax) occurs when the cosine function is at its maximum value of 1, which happens at ωt = 0.
vmax = Aω
Vavg =\(\frac { total \ distance\ traveled}{time\ taken}\)
The total distance traveled in one complete cycle is 2A, and the time taken for one complete cycle is T.
Vavg = \(\frac {2A}{T}\)
The time period (T) can be calculated as the inverse of the frequency (f):
T = \(\frac {1}{f}\)
Substituting the expression for T, we get:
Vavg =\(\frac {2A}{1/f}\) = 2Af = 2πfA
Since the angular frequency (ω) is related to the frequency (f) by ω = 2πf, we can rewrite the expression for V_avg as:
Vavg = \(\frac {2πfA}{2π}\) = fA
Given that Vmax = Aω,
we can rewrite Vavg as:
Vavg = \(\frac {(V_{max} / ω)ω}{2π}\) = \(\frac {V_{max}}{ω} \times \frac {ω}{2π}\)= \(\frac {2V_{max}}{π}\)
Therefore, the correct option is (D) \(\frac {2V}{π.}\)
A particle is executing simple harmonic motion with a time period of 3 s. At a position where the displacement of the particle is 60% of its amplitude, the ratio of the kinetic and potential energies of the particle is: