# Linear Simple Harmonic Motion

#### Oscillatory Motion:

• A to and fro periodic motion of a body along a definite path is called oscillatory motion.
• e.g. the motion of heavy bob of a pendulum, the Motion of molecules of solid due to thermal energy.

#### Oscillation:

• It is defined as a complete to and fro motion of a body performing oscillatory motion along its path.
• The body covers its path twice in one oscillation.

#### Examples of Oscillatory Motion:

• The motion of heavy bob of the pendulum.
• The motion of pivoted magnetic needle in the uniform magnetic field.
• The Motion of molecules of solid due to thermal energy.
• The motion of needle of a sewing machine.
• The motion of prongs of tuning fork.
• The motion of medium particles, when a longitudinal or transverse wave travels through it.

#### Periodic Motion:

• When the body performs the same set of movements again and again within a fixed interval of time, then the body is said to have periodic motion.
• e.g. motion of the moon around the earth, the motion of the minute hand of a clock.

#### Extreme Position:

• It is defined as the position of the body at which the body comes to rest momentarily.
• They are ends of the path and the body never moves beyond these positions.

#### Mean Position:

• It is defined as the position of the body at which the net force acting on the body is zero. Hence this position is also called an equilibrium position.
• It is the centre of the path and the body moves equally on its two sides.

#### Displacement:

• It is defined as the distance of the body from the mean position at that instant irrespective of the position from which it starts.

#### Definition:

• Linear simple harmonic motion is defined as the motion of a body in which
• the body performs an oscillatory motion along its path.
• the force (or the acceleration) acting on the body is directed towards a fixed point                  (i.e. means position) at any instant.
• the force (or the acceleration) acting on a body is directly proportional to the displacement of the body at every instant.
• e.g. the motion of heavy bob o the pendulum.

#### Examples of Linear Simple Harmonic Motion:

• The motion of heavy bob of pendulum.
• The motion of pivoted magnetic needle in uniform magnetic field.
• The Motion of molecules of solid due to thermal energy.
• The motion of needle of sewing machine.
• The motion of prongs of tuning fork.
• The motion of medium particles, when a longitudinal or transverse wave travel through it.

#### Displacement of Simple Harmonic Motion:

• The distance of the body performing S.H.M. from its mean position is called as a displacement.
• It is denoted by letter ‘x’. Its S.I. unit is metre.

#### Amplitude of Simple Harmonic Motion:

• The maximum displacement of body performing S.H.M. from mean position is called as amplitude of S.H.M.
• It is denoted by letter ‘a’. Its S.I. unit is metre.

#### Path length or range of Simple Harmonic Motion:

• The total length of the path over which the body performing linear S.H.M. moves is called the path length or range of linear S.H.M.
• Path length or range is twice the ampitude and in one oscillation body covers a total distance of ‘4a’. Thus,  path length = 2 × amplitude

#### Period of Simple Harmonic Motion:

• The time taken by body performing S.H.M. to complete one oscillation is called as a period of S.H.M.
• It is denoted by a letter ‘T’ and its S.I. unit is second.

#### Frequency of Simple Harmonic Motion:

• The number of oscillations performed by the body performing S.H.M in unit time (one second)  is called as frequency of S.H.M.
• It is denoted by letter ‘n’. Its S.I. unit is hertz (Hz).

#### Defining Equation of Linear Simple Harmonic Motion:

• Linear simple harmonic motion is defined as the motion of a body in which
• the body performs an oscillatory motion along its path.
• the force (or the acceleration) acting on the body is directed towards a fixed point                  (i.e. means position) at any instant.
• the force (or the acceleration) acting on a body is directly proportional to the displacement of the body at every instant.
• The force acting on the body, which is directed towards the mean position at every instant, it is called as a restoring force.

From definition of S.H.M.

F    ∝    – x

∴ F     =   – k x

Where,  F  =  restoring force

x  =  displacement

k is constant called force constant

This equation is known as defining equation of linear S.H.M.

Differential Equation of Linear S.H.M.:

• By definition of linear S.H.M., the force acting on a particle performing S.H.M. is given by

F = – kx     …..   (1)

Where k is force per unit displacement, which is constant.

By Newton’s second law of motion

F  = mf       …..  (2)

Where,  m = mass of body

f = acceleration of the body

F = restoring  force acting on body

By definition of linear acceleration,

From equations (2) and (5) we have

• The equations (7) (8) and  (9) (different forms) are known as differential equations of linear S.H.M. which is second order homogeneous differential equation.

#### Expression for Acceleration of a Particle Performing Linear S.H.M.:

Differential equation of S.H.M. is

Where k = Force constant, m = Mass of a body performing S.H.M.

• This is an expression of an acceleration of a body performing linear S.H.M. Negative sign indicate the direction of acceleration towards the mean position or it is opposite to the direction of displacement.

#### Special Cases:

• Case – I: When the body is at the mean position, its displacement x  =  0.

f min =  0

Thus at the mean position, acceleration is minimum and i.e. zero.

• Case – II: When the body is at the extreme position. The magnitude of its displacement x  = a

f  =  ω²a

Thus at extreme position, the magnitude of acceleration is maximum

#### Expression for Velocity of a Particle Performing Linear S.H.M.:

Differential equation of S.H.M. is

Where k = Force constant, m = Mass of a body performing S.H.M.

Integrating both sides of the equation

Where C = Constant of integration

v =  velocity of the body.

x = Displacement of the body.

At extreme position x = ± a   and v = 0

Substituting these values in equation (1) we have

This is an expression of the velocity of the particle performing S.H.M.

where a  =  amplitude of S.H.M.

x  =  displacement of body.

#### Special Cases:

• Case – I: When particle is at mean position i.e. x = 0

The velocity of the particle performing S.H.M. is maximum at the mean position.

Vmax  =  ωa

• Case – II: When particle is at extreme position i.e. x = a.

The velocity of the particle performing S.H.M. is minimum and i.e. zero at the extreme position

#### Expression for Displacement of a Particle Performing Linear S.H.M.:

Magnitude of velocity of particle performing S.H.M. is given by

where a  =  amplitude of S.H.M.

x  =  displacement of body.

ω =   Angular velocity

Integrating both sides

• Case – 1: When the particle is starting from mean position.x = 0 at t = 0.

substituting these values in equation (1)

This is an expression for displacement of particle

performing S.H.M. and starting from mean position.

• Case 2: If particle is starting from extreme position i.e. x = ± a  at t = 0.

substituting these values in equation (1)

This is is an expression for displacement of particle

performing S.H.M. and starting from an extreme position.

• Case – 3: If the particle is starting from any other position than extreme or mean position. Let x = x0  when t = 0.

Substituting these values in equation (1).

This is an expression for displacement of particle

performing S.H.M. and starting from any position.

• Value of α depends upon the initial conditions. If body starts from mean position a =  0. If body starts from extreme position a =± π/2.
• α is called an initial phase or epoch of S.H.M. and x0 =  initial displacement of the particle.

#### Expression for Velocity and Acceleration of a Particle Performing S.H.M. Using Expression of Displacement:

The general equation of displacement of a particle is

x = a sin (ωt + α)   ………….. (1)

The velocity of the particle can be obtained by differentiating both sides w.r.t. t,

This is an expression for the velocity of a particle performing linear S.H.M.

We can get the acceleration of the body by differentiating equation (2) again w.r.t. t.

This is an expression for the acceleration of a particle performing linear S.H.M.

#### Phase of S.H.M.:

• Displacement of particle performing S.H.M. is given by

x = a sin (ωt + α)

where x  =  displacement, a  =  amplitude of S.H.M., =  angular velocity

t  =  time, α =  initial phase (epoch)

• The quantity (ωt + α) is called as the phase of S.H.M.  Phase of a body performing linear S.H.M. is defined as the state of the body w.r.t. the mean position at instant ‘t’.
• When the particle is at mean position quantity (ωt + α) is zero when it is at extreme position quantity (ωt + α) is  π/2. It means if particle starts moving from mean position to extreme position (ωt + α) starts increasing from zero to π/2.
• When the body is at the mean position, then its phase is kπ where k = 0,1,2,3,….. and when body is at the extreme position then its phase is kπ.  where k  =  1,3,5,7,…..
• From the value of (ωt + α) , we can get an idea of exact position and state of motion of the particle performing S.H.M.

#### Time Period of a Particle Performing Linear S.H.M.:

Differential equation of S.H.M. is

Where k = Force constant, m = Mass of a body performing S.H.M.

This is an expression for the time period of a particle performing linear S.H.M.

#### Expression for Time Period of a Particle Performing Linear S.H.M.  in Terms of Force Constant:

By differential equation of S.H.M.,

Where T = Period of S.H.M.

This is an expression for the time period of S.H.M. in terms of force constant.

#### Uniform circular motion is a special case of linear S.H.M.:

• Consider particle ‘P’ moving along a circular path with uniform angular velocity w.  Let M be its projections on diameter AB of the circular path as shown in fig. The x components of displacement, velocity, and acceleration of particle P are same as x components of displacement, velocity, and acceleration of projection M respectively.
• Suppose the particle P starts from the initial position with initial phaseα at time t  = 0. In time t the angle between OP and x-axis is (ωt + α).

From figure,

This is an expression for displacement of particle M at time t.

The velocity of the particle  M is given by

• Thus the acceleration of particle M is directly proportional to the displacement of the particle and its direction is opposite to that of displacement. But this is the defining character of linear S.H.M. Hence uniform circular motion is a special case of linear S.H.M.