T is the oscillation period of a mass M hung from a light spring. The period of oscillation will now be if another mass M is suspended alongside it.
F ∝ X
Here, F = Force and X = Displacement
The period T of an oscillating mass M suspended from a light spring. Now, if another mass M is hanging beside it, the period of oscillation will be.
T = 2πM/K
The oscillating mass M's period T, which is hung from a light spring. Now, the period of oscillation will be if another mass M is hanging next to it.
T = 2πM/K
Now when two M masses are there then, M+M = 2M and now the time period is T1
So, T1 = 2π2M/K
T1 = 2 x T = 2T
An oscillatory motion is simple harmonic motion (SHM). According to SHM, a particle's acceleration is shown to be inversely related to its displacement from the initial position at any given point. A specific type of oscillatory motion is known as SHM.
As a result, all simple harmonic movements are capable of having an oscillatory and periodic character. The opposite, however, is untrue. Not every oscillatory motion is an SHM.
Parameters in SHM that are affected by time include displacement, velocity, acceleration, and force. Sinusoids are sometimes referred to as sine, and the cosine functions serve to illustrate this. Simple Harmonic Motion explains the unique properties of alternating currents, sound waves, and light waves.
We know T= 2𝜋\(\sqrt{\frac{M}{K}}\)
When another mass is suspended
Total mass = M+M = 2M
Then Period, T’ = 2𝜋\(\sqrt{\frac{2M}{K}}\) = √2 2𝜋\(\sqrt{\frac{M}{K}}\) = √2 T
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):
AB is a part of an electrical circuit (see figure). The potential difference \(V_A - V_B\), at the instant when current \(i = 2\) A and is increasing at a rate of 1 amp/second is:
Oscillation is a process of repeating variations of any quantity or measure from its equilibrium value in time . Another definition of oscillation is a periodic variation of a matter between two values or about its central value.
The term vibration is used to describe the mechanical oscillations of an object. However, oscillations also occur in dynamic systems or more accurately in every field of science. Even our heartbeats also creates oscillations. Meanwhile, objects that move to and fro from its equilibrium position are known as oscillators.
Read More: Simple Harmonic Motion
The tides in the sea and the movement of a simple pendulum of the clock are some of the most common examples of oscillations. Some of examples of oscillations are vibrations caused by the guitar strings or the other instruments having strings are also and etc. The movements caused by oscillations are known as oscillating movements. For example, oscillating movements in a sine wave or a spring when it moves up and down.
The maximum distance covered while taking oscillations is known as the amplitude. The time taken to complete one cycle is known as the time period of the oscillation. The number of oscillating cycles completed in one second is referred to as the frequency which is the reciprocal of the time period.