Wave Motion | Wave & Optics | Part 1 | Class 12 | New Curriculam 2078 | Notes | Nepal |

Waves



The disturbance which propagates from one point to another point without net transport of matter is called wave. It is due to repeated simple harmonic motion of particle carrying energy but not due to actual linear movement of particle carrying energy.

Examples: sound wave, light wave, water ripples etc.


Characteristics of Wave Motions:

  • Wave motion is a disturbance propagating in a medium. 
  • It transfers energy as well as momentum from one point to another.
  • When it propagates in a medium particles of the medium execute vibrating
  • motion about their mean position.
  • It has finite and fixed speed which depends on the nature of the medium and
  • is given by v = ๐‘“ × ๐œ†.
  • 5. Speed of wave and particle velocity are different. The particle velocity is ๐‘ฃ =๐‘Ž๐œ”๐‘๐‘œ๐‘ ๐œ”๐‘ก.  

Types of wave motion

1. Electromagnetic waves

2.Mechanical waves

3.Matter waves


Electromagnetic waves

1. Doesn't need a medium for its propagation. light wave, heat waves, radio waves etc.

2. Speed is equal to speed of light.

3. Moving charges back and forth will produce oscillating electric and magnetic fields. The electric field and magnetic field are perpendicular to each other.


Mechanical waves:

• Requires material medium for their propagation.

• For the propagation of mechanical waves, medium must possess elasticity, inertia and low resistance for motion (i.e. damping must be very small)

• Examples: water waves, sound waves, waves in pipes and strings etc.


Types of mechanical waves

Transverse waves:

If the particle of a medium vibrate perpendicularly to the propagation of the wave, then the wave is called transverse wave. For eg: wave on strings, water ripples, etc.


• Vibration is perpendicular to the propagation of waves.

• For the propagation of transverse wave medium should havemodulus or rigidity. So, these waves are present in solids.

• Polarization is possible.

• Travels in the form of crest and troughs.



Longitudinal waves:

If the particles of a medium vibrate along the direction of propagation of the wave, the wave is called longitudinal wave. For eg: waves on spring along length, sound waves on air, etc.
Longitudinal Wave Fig


• Vibration is parallel to the propagation of waves.

• For the propagation of longitudinal waves medium must have Bulk modulus of elasticity. So, these waves are present in all three media solid liquid and gases.

• Polarization is not possible.

• Travels in the form of compression and rarefactions.


Matter Wave

The waves associated with the microscopic particles such as electrons, protons, neutrons, atoms and molecules when they are in motion are called matter waves. The concept of matter wave was first introduced by de-Broglie, so it is called de-Broglie wave


Waves on the water:

Water waves are an example of waves that involve a combination of both longitudinal and transverse motions. As a wave travels through the water, the particles travel in clockwise circles. The radius of the circles decreases as the depth into the water increases.

Notes: Waves on the earth surface during earthquake is the combination of longitudinal and transverse waves.

 

Some terms related to wave:

 Displacement:

The distance of an oscillating particle of the wave from its equilibrium position at any particular time.

The displacement equation is,

๐’š = ๐š๐ฌ๐ข๐ง ๐’˜๐’•๐œฑ

Where, y= displacement of the particle at any instant of time ‘t’

            a= amplitude=maximum displacement from its mean position.

            w= angular frequency=2๐œ‹๐‘“

             ๐‘ค๐‘ก๐›ท=phase of the wave


Particle speed:

During wave propagation medium of the particles undergo simple harmonic motion

around their mean position. The speed of these particles is called particle speed.

We know,

                  ๐’š = ๐š๐ฌ๐ข๐ง(๐’˜๐’• − ๐œฑ)

Differentiating with respect to time we get,

 ๐‘Ž๐‘ค๐‘๐‘œ๐‘ (๐’˜๐’• − ๐œฑ)

∴ ๐’— = ๐’‚๐’˜๐’„๐’๐’” ๐’˜๐’• − ๐œฑ

For maximum speed, ๐‘๐‘œ๐‘ (๐’˜๐’• − ๐œฑ) =1 so  = ๐‘Ž๐‘ค (๐‘š๐‘’๐‘Ž๐‘› ๐‘๐‘œ๐‘ ๐‘–๐‘ก๐‘–๐‘œ๐‘›)

For minimum speed. ๐‘๐‘œ๐‘  (๐’˜๐’• − ๐œฑ) =0, so = 0 (๐‘’๐‘ฅ๐‘ก๐‘Ÿ๐‘’๐‘š๐‘’ ๐‘๐‘œ๐‘ ๐‘–๐‘ก๐‘–๐‘œ๐‘›)


Frequency:

Number of complete oscillation made by oscillating particles in one second is called

 frequency. It is denoted by ‘f’. Its SI unit is Hertz(per second).


Wavelength

The distance between successive identical parts of the wave. It's unit is meters. Also,

The linear distance travelled by wave in one complete oscillation is called wavelength.


Time period

The time taken for one complete oscillation is called time period.

It is denoted by T

Or,

It is also defined as the reciprocal of frequency.

i.e. 

Its SI unit is seconds(s)



Wave Velocity

Linear distance travelled by wave per unit time is called wave velocity.

i.e. ๐‘ค๐‘Ž๐‘ฃ๐‘’ ๐‘ฃ๐‘’๐‘™๐‘œ๐‘๐‘–๐‘ก๐‘ฆ = ๐‘ค๐‘Ž๐‘ฃ๐‘’ ๐‘™๐‘’๐‘›๐‘”๐‘กโ„Ž ๐‘ก๐‘–๐‘š๐‘’ ๐‘๐‘’๐‘Ÿ๐‘–๐‘œ๐‘‘

∴ ๐‘ฃ = ๐œ† × ๐‘“

Its SI unit is  


Phase of the wave:

The argument of the sine/cosine in a given wave equation is called phase angle or simply phase of the wave. It gives the state of the vibrating particle as regards its position and direction of motion.

The equation of progressive wave is,

Here, phase of the wave(๐œ‘) = 

Its SI unit is radian.


Progressive Waves

The waves which moves in forward direction with constant amplitude is called progressive waves.


Characteristics of Progressive Waves:

  • A progressive waves transfer energy from one part of space at other
  • In progressive waves, no particle is permanently at rest.
  • In progressive waves all the particles vibrates with same amplitude and with same frequency.
  • It may be either transverse or longitudinal.

Equation of progressive waves and equation of stationery wave equation: 

From Book


Principle of superposition of waves.

The principle of superposition of waves state, "if two or more that two waves superimposed, then the displacement equation of the resultant waves is equal to the algebraic sum of the displacement of the individual waves that superimposed.

Let  be the displacement equation of the individual waves that superimposed then the displacement of the resultant wave is :


*Thank You*

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