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Oscillations
MUHAMMAD IMTIAZ
CS, YEAR 2
NAMAL COLLEGE, MIANWALI
Oscillatory / Vibratory motion
 The motion of an object in which object moves to and fro about its mean position,
is called oscillatory motion.
 If this motion repeats itself after equal intervals of time, Called Periodic motion.
 Examples:
 Simple pendulum motion
 Motion of steel ruler
 Steel ball rolling in a curved plate
 Mobile in vibration
Simple harmonic motion
 Oscillatory motion due to restoring force, Called simple harmonic motion.
 This restoring force is equal and opposite to the applied force.
 𝑭 𝒓 = -kx
 -ve sign shows that this force is directed towards mean position.
 Hook’s law:
 The restoring force is directly proportional to the displacement and always directed
towards the mean position.
 Acc. Produced due to restoring force can be determined by 2nd law of motion
 a 𝜶 – x
 Acc. Is directly proportional to displacement and directed towards mean position.
Terminologies related SHM
 Restoring force:
 The force which is equal and opposite to applied force, Restoring force.
 Instantaneous displacement:
 The displacement at any instant from the mean position, Instantaneous displacement.
 Amplitude:
 The maximum displacement of the body from the mean position, Amplitude.
 It is denoted by 𝑋0.
Continued…
 Vibration / cycle:
 A complete round trip of body performing SHM, Vibration / cycle.
 Time period:
 Time to complete one vibration, Time period.
 T = 2 / ω
 Frequency:
 Number of vibrations in unit time, Frequency.
 f = 1 / T
 Unit is vibrations per seconds, cycles per seconds or hertz(HZ, SI unit)
Displacement
 The distance of a body from its mean position is called displacement.
 Formula:
 x = 𝑥0sin𝛳 here 𝛳 = ωt
 x = 𝑥0sinωt
 Here 𝜭 gives the state of system in its vibrational motion. i.e. if
 𝛳 = 0, ‘p’ is at mean position
 𝛳 = 90 or / 2, ‘p’ competes one fourth of its cycle
 𝛳 = 180 or , ‘p’ competes half of its cycle
 𝛳 = 270 or 3 / 2, ‘p’ competes third fourth of its cycle
 𝛳 = 360 or 2 , ‘p’ competes one cycle
Velocity
 The velocity of an object executing SHM is directed along the motion of body.
 v = 𝑥0ω cos ωt 𝛳 = ωt
 The direction of velocity depends upon the value of ′𝜭’
 Here 𝛳 = 𝑥0
2 − 𝑥2 / 𝑥0
 v = ω 𝑥0
2 − 𝑥2
 From the above equation if x = 0,
 V = maximum if x = 0
 V = minimum if 𝑥0 = 0
Acceleration
 Acceleration of body executing SHM is directly proportional to displacement and
is directed towards the mean position.
 Formula:
 a = - ω 𝟐
x
Phase / phase angle
 The angle 𝛳 = ωt is the angle which specifies the displacement as well as the
direction of motion of the point executing SHM.
 i.e. if
 𝛳 = 0, ‘p’ is at mean position
 𝛳 = 90 or / 2, ‘p’ competes one fourth of its cycle
 𝛳 = 180 or , ‘p’ competes half of its cycle
 𝛳 = 270 or 3 / 2, ‘p’ competes third fourth of its cycle
 𝛳 = 360 or 2 , ‘p’ competes one cycle
Displacement, Velocity and acceleration
 As we know a = - kx / m and a = - ω 𝟐
x
 So ω = 𝑘/𝑚 thus
 Displacement:
 x = 𝑥0sin 𝑘/𝑚 t
 Velocity:
 v = 𝑘/𝑚 𝑥0
2 − 𝑥2
 Acceleration:
 a = -
𝑘x
𝑚
 Time period:
 T = 2 𝑚/𝑘
Energy conservation in SHM
 Statement:
 In SHM energy is energy of the vibrating system remains constant. i.e. energy is
converted into P.E and K.E but the total energy remains conserve.
 Formula:
 Total energy = ½ k𝒙 𝟎
𝟐
Free and forced oscillations
 Free oscillations:
 A body is said to be oscillate freely when there is no continuous force applied on a body
to oscillate. Only initial push is required.
 The frequency of the body is called its natural frequency. E.g. simple pendulum
 Forced oscillations:
 When there is continuous force required to oscillate the body, its oscillations are called
forced oscillations.
 The physical system under going forced vibrations is known as driven harmonic
oscillator.
GKK / HKK
 Resonance
 Damped oscillations
 Sharpness of resonance
Waves
 It is the disturbance in the medium through which energy is transported without
transporting the matter.
 Examples:
 sound waves,
 waves in spring,
 waves in rope,
 water waves,
 air waves etc.
Types of waves
 Mechanical waves:
 Waves which propagate by the oscillations of material particle, called mechanical
waves.
 E.g.
 Sound waves, air waves, spring waves, water waves
 Electromagnetic waves:
 Waves which propagate by the oscillations of electric and magnetic fields, called
Electromagnetic waves.
Progressive waves
 Waves which propagates energy by moving away from the source of disturbance,
travelling or progressive waves.
 These are of two types.
 Transverse waves:
 Waves in which particles of the medium have displacement perpendicular to the
direction propagation of waves.
 Longitudinal or compressional waves:
 Waves in which particles of the medium have displacement parellel to the direction
propagation of waves.
Superposition of waves
 The composition of two (or more) waves travelling through the same medium at
the same time, principle of superposition.
 Principle of superposition leads us to three different cases:
 Interference
 Beats
 Stationary waves
Interference
 Superposition of two waves having same frequency and travelling in the same
direction, interference.
 Constructive interference:
 Whenever path difference is an integral multiple of wavelength, interference of two
waves is called constructive interference.
 Δs = nλ
 Destructive interference:
 Whenever path difference is an odd integral multiple of half of wavelength, interference
of two waves is called destructive interference.
 Δs = (2n+1)λ/2
GKK / HKK
 Beats
 Reflection of waves
 Stationary waves
 Stationary waves in stretched string
 Stationary waves in air column
 Doppler effect
Thank you

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Oscillation Fundamentals

  • 1. Oscillations MUHAMMAD IMTIAZ CS, YEAR 2 NAMAL COLLEGE, MIANWALI
  • 2. Oscillatory / Vibratory motion  The motion of an object in which object moves to and fro about its mean position, is called oscillatory motion.  If this motion repeats itself after equal intervals of time, Called Periodic motion.  Examples:  Simple pendulum motion  Motion of steel ruler  Steel ball rolling in a curved plate  Mobile in vibration
  • 3. Simple harmonic motion  Oscillatory motion due to restoring force, Called simple harmonic motion.  This restoring force is equal and opposite to the applied force.  𝑭 𝒓 = -kx  -ve sign shows that this force is directed towards mean position.  Hook’s law:  The restoring force is directly proportional to the displacement and always directed towards the mean position.  Acc. Produced due to restoring force can be determined by 2nd law of motion  a 𝜶 – x  Acc. Is directly proportional to displacement and directed towards mean position.
  • 4. Terminologies related SHM  Restoring force:  The force which is equal and opposite to applied force, Restoring force.  Instantaneous displacement:  The displacement at any instant from the mean position, Instantaneous displacement.  Amplitude:  The maximum displacement of the body from the mean position, Amplitude.  It is denoted by 𝑋0.
  • 5. Continued…  Vibration / cycle:  A complete round trip of body performing SHM, Vibration / cycle.  Time period:  Time to complete one vibration, Time period.  T = 2 / ω  Frequency:  Number of vibrations in unit time, Frequency.  f = 1 / T  Unit is vibrations per seconds, cycles per seconds or hertz(HZ, SI unit)
  • 6. Displacement  The distance of a body from its mean position is called displacement.  Formula:  x = 𝑥0sin𝛳 here 𝛳 = ωt  x = 𝑥0sinωt  Here 𝜭 gives the state of system in its vibrational motion. i.e. if  𝛳 = 0, ‘p’ is at mean position  𝛳 = 90 or / 2, ‘p’ competes one fourth of its cycle  𝛳 = 180 or , ‘p’ competes half of its cycle  𝛳 = 270 or 3 / 2, ‘p’ competes third fourth of its cycle  𝛳 = 360 or 2 , ‘p’ competes one cycle
  • 7. Velocity  The velocity of an object executing SHM is directed along the motion of body.  v = 𝑥0ω cos ωt 𝛳 = ωt  The direction of velocity depends upon the value of ′𝜭’  Here 𝛳 = 𝑥0 2 − 𝑥2 / 𝑥0  v = ω 𝑥0 2 − 𝑥2  From the above equation if x = 0,  V = maximum if x = 0  V = minimum if 𝑥0 = 0
  • 8. Acceleration  Acceleration of body executing SHM is directly proportional to displacement and is directed towards the mean position.  Formula:  a = - ω 𝟐 x
  • 9. Phase / phase angle  The angle 𝛳 = ωt is the angle which specifies the displacement as well as the direction of motion of the point executing SHM.  i.e. if  𝛳 = 0, ‘p’ is at mean position  𝛳 = 90 or / 2, ‘p’ competes one fourth of its cycle  𝛳 = 180 or , ‘p’ competes half of its cycle  𝛳 = 270 or 3 / 2, ‘p’ competes third fourth of its cycle  𝛳 = 360 or 2 , ‘p’ competes one cycle
  • 10. Displacement, Velocity and acceleration  As we know a = - kx / m and a = - ω 𝟐 x  So ω = 𝑘/𝑚 thus  Displacement:  x = 𝑥0sin 𝑘/𝑚 t  Velocity:  v = 𝑘/𝑚 𝑥0 2 − 𝑥2  Acceleration:  a = - 𝑘x 𝑚  Time period:  T = 2 𝑚/𝑘
  • 11. Energy conservation in SHM  Statement:  In SHM energy is energy of the vibrating system remains constant. i.e. energy is converted into P.E and K.E but the total energy remains conserve.  Formula:  Total energy = ½ k𝒙 𝟎 𝟐
  • 12. Free and forced oscillations  Free oscillations:  A body is said to be oscillate freely when there is no continuous force applied on a body to oscillate. Only initial push is required.  The frequency of the body is called its natural frequency. E.g. simple pendulum  Forced oscillations:  When there is continuous force required to oscillate the body, its oscillations are called forced oscillations.  The physical system under going forced vibrations is known as driven harmonic oscillator.
  • 13. GKK / HKK  Resonance  Damped oscillations  Sharpness of resonance
  • 14. Waves  It is the disturbance in the medium through which energy is transported without transporting the matter.  Examples:  sound waves,  waves in spring,  waves in rope,  water waves,  air waves etc.
  • 15. Types of waves  Mechanical waves:  Waves which propagate by the oscillations of material particle, called mechanical waves.  E.g.  Sound waves, air waves, spring waves, water waves  Electromagnetic waves:  Waves which propagate by the oscillations of electric and magnetic fields, called Electromagnetic waves.
  • 16. Progressive waves  Waves which propagates energy by moving away from the source of disturbance, travelling or progressive waves.  These are of two types.  Transverse waves:  Waves in which particles of the medium have displacement perpendicular to the direction propagation of waves.  Longitudinal or compressional waves:  Waves in which particles of the medium have displacement parellel to the direction propagation of waves.
  • 17. Superposition of waves  The composition of two (or more) waves travelling through the same medium at the same time, principle of superposition.  Principle of superposition leads us to three different cases:  Interference  Beats  Stationary waves
  • 18. Interference  Superposition of two waves having same frequency and travelling in the same direction, interference.  Constructive interference:  Whenever path difference is an integral multiple of wavelength, interference of two waves is called constructive interference.  Δs = nλ  Destructive interference:  Whenever path difference is an odd integral multiple of half of wavelength, interference of two waves is called destructive interference.  Δs = (2n+1)λ/2
  • 19. GKK / HKK  Beats  Reflection of waves  Stationary waves  Stationary waves in stretched string  Stationary waves in air column  Doppler effect