Show that the oscillations due to a spring are simple harmonic oscillations and obtain the expression of periodic time.
According to figure a block of mass $m$ fixed to a spring, which in turn is fixed to a rigid wall.
The block is placed on a friction less horizontal surface.
If the block is pulled on one side and is released it then executes a to and fro motion about a mean position.
Let $x=0$, indicate the position of the centre of the block when the spring is in equilibrium. The positions - A and + A indicate the maximum displacements to the left and the right of the mean position.
For spring Robert Hooke law, "Spring when deformed, is subject to a restoring force, the magnitude of which is proportional to the deformation or the displacement and acts is opposite direction."
Let any time $t$, if the displacement of the block from its mean position is $x$, the restoring force $\mathrm{F}$ acting on the block it
$\mathrm{F}(x)=-k x \quad \ldots$ $(1)$
Where $k$ is constant of proportionality and is called the spring constant or spring force constant.
Equation $(1)$ is same as the force law for $SHM$ and therefore the system executes a simple harmonic motion.
A $15 \,g$ ball is shot from a spring gun whose spring has a force constant of $600 \,N/m$. The spring is compressed by $5 \,cm$. The greatest possible horizontal range of the ball for this compression is .... $m$ ($g = 10 \,m/s^2$)
A uniform stick of mass $M$ and length $L$ is pivoted at its centre. Its ends are tied to two springs each of force constant $K$ . In the position shown in figure, the strings are in their natural length. When the stick is displaced through a small angle $\theta $ and released. The stick
Five identical springs are used in the following three configurations. The time periods of vertical oscillations in configurations (i), (ii) and (iii) are in the ratio
A uniform rod of length $L$ and mass $M$ is pivoted at the centre. Its two ends are attached to two springs of equal spring constants $k$. The springs are fixed to rigid supports as shown in the figure, and the rod is free to oscillate in the horizontal plane. The rod is gently pushed through a small angle $\theta$ in one direction and released. The frequency of oscillation is
A spring having a spring constant $‘K’$ is loaded with a mass $‘m’$. The spring is cut into two equal parts and one of these is loaded again with the same mass. The new spring constant is