Base area of the cork = \(A\)
Height of the cork = \(h\)
Density of the liquid =\(\rho_l\)
Density of the cork = \(\rho\)
In equilibrium:
Weight of the cork = Weight of the liquid displaced by the floating cork
Let the cork be depressed slightly by x. As a result, some extra water of a certain volume is displaced. Hence, an extra up-thrust acts upward and provides the restoring force to the cork.
Up-thrust = Restoring force, \(F\) = Weight of the extra water displaced
\(F\) = –(Volume × Density × \(g\))
Volume = Area × Distance through which the cork is depressed
Volume = \(Ax\)
∴ \(F\) = \(– A x \rho_lg\) … (i)
According to the force law:
\(F\) = \(kx\)
\(k\) = \(\frac{F}{x}\)
Where, \(k\) is a constant
\(k\) = \(\frac{F}{x}\)=\(-A\rho_lg\)....(ii)
The time period of the oscillations of the cork:
\(T\) = \(2\pi\sqrt{\frac{m}{K}}\)...(iii)
Where,
\(m\) = Mass of the cork
= Volume of the cork × Density
= Base area of the cork × Height of the cork × Density of the cork
= \(Ah\rho\)
Hence, the expression for the time period becomes:
\(T\) =\( 2\pi\sqrt{\frac{Ah\rho}{A\rho_lg}}\)
=\(2\pi\sqrt{\frac{h\rho}{\rho_lg}}\)
Figures 9.20(a) and (b) refer to the steady flow of a (non-viscous) liquid. Which of the two figures is incorrect ? Why ?
Simple Harmonic Motion is one of the most simple forms of oscillatory motion that occurs frequently in nature. The quantity of force acting on a particle in SHM is exactly proportional to the displacement of the particle from the equilibrium location. It is given by F = -kx, where k is the force constant and the negative sign indicates that force resists growth in x.
This force is known as the restoring force, and it pulls the particle back to its equilibrium position as opposing displacement increases. N/m is the SI unit of Force.
When a particle moves to and fro about a fixed point (called equilibrium position) along with a straight line then its motion is called linear Simple Harmonic Motion. For Example spring-mass system
The restoring force or acceleration acting on the particle should always be proportional to the displacement of the particle and directed towards the equilibrium position.
When a system oscillates angular long with respect to a fixed axis then its motion is called angular simple harmonic motion.
The restoring torque (or) Angular acceleration acting on the particle should always be proportional to the angular displacement of the particle and directed towards the equilibrium position.
Τ ∝ θ or α ∝ θ
Where,