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) \(\frac {2V}{π.}\)
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity):