
To determine the new amplitude of oscillation when another mass \( m \) is gently placed on the mass \( M \) attached to the spring, we can use the principles of conservation of mechanical energy and properties of simple harmonic motion (SHM).
Initially, the energy in the system when only mass \( M \) is oscillating is given by:
E_i = \frac{1}{2} k A^2
After placing the additional mass \( m \) onto \( M \) at equilibrium, the system's total mass becomes \( M + m \). The new mechanical energy ( \( E_f \) ) will be distributed in the oscillation of the combined mass.
Since there is no external work done and assuming no energy loss:
E_i = E_f
The energy in the system with the new combined mass and the new amplitude \( A' \) is:
E_f = \frac{1}{2} k A'^2
Setting the initial and final energy equal gives us:
\frac{1}{2} k A^2 = \frac{1}{2} k A'^2
Since the energy before and after must remain the same:
\frac{1}{2} k A^2 = \frac{1}{2} k A'^2
However, with the new mass, we must consider the change in system properties. Using conservation of momentum principles, the kinetic energy at the equilibrium translates proportionally:
A' = A \sqrt{\frac{M}{M + m}}
Thus, the correct option is:
$A \sqrt{\frac{ M }{ M + m }}$
This solution illustrates the effect of adding an additional mass on the oscillating system's amplitude, accounting for unchanged energy and altered system mass.
Using a variable frequency ac voltage source the maximum current measured in the given LCR circuit is 50 mA for V = 5 sin (100t) The values of L and R are shown in the figure. The capacitance of the capacitor (C) used is_______ µF.
