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Oscilation and Optics

The document discusses simple harmonic motion and wave motion, describing key concepts such as oscillation, frequency, wavelength, amplitude, and types of waves including transverse, longitudinal, electromagnetic, and mechanical waves. It also covers topics like simple harmonic oscillators, damped and forced oscillations, the simple pendulum, and wave properties and characteristics.

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0% found this document useful (0 votes)
82 views32 pages

Oscilation and Optics

The document discusses simple harmonic motion and wave motion, describing key concepts such as oscillation, frequency, wavelength, amplitude, and types of waves including transverse, longitudinal, electromagnetic, and mechanical waves. It also covers topics like simple harmonic oscillators, damped and forced oscillations, the simple pendulum, and wave properties and characteristics.

Uploaded by

misganamarcos10
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF, TXT or read online on Scribd
You are on page 1/ 32

Oscillations, Waves and Optics

Jan, 2024, ASTU

1
ASTU Cover Page - 1/32 Jan – 2024
Simple Harmonic Motion
 Periodic or oscillatory motion is motion of an object that regularly returns to a given
position after a fixed time interval.
 If something is oscillating (vibrating) this means that it is moving backwards and
forwards, up and down, side to side, and in and out around some central position
(equilibrium point).

 Simple harmonic motion (SHM) is a special type of


m
periodic motion or oscillation where;
 motion is about an equilibrium position at which
point no net force acts on the system,
 the restoring force is directly proportional to the
displacement 𝒙 from the equilibrium position
 acts in the direction opposite to that of
displacement.

2
ASTU Simple Harmonic Motion - 2/32 Jan – 2024
Simple Harmonic Motion
 Velocity as a Function of Position

 Conservation of energy provides a simple method of deriving an expression for the velocity
of an object undergoing periodic motion as a function of position.

 This expression shows that the object’s speed is a maximum


at 𝑥 = 0 and is zero at the extreme positions 𝑥 = ±𝐴.

3
ASTU Simple Harmonic Motion - 3/32 Jan – 2024
Simple Harmonic Motion
 Period and Frequency

 The frequency of the periodic motion of a mass on a spring is

 The angular frequency (𝝎) is


4
ASTU Simple Harmonic Motion - 4/32 Jan – 2024
Simple Harmonic Motion

 First condition

The solution is

 Second condition

5
ASTU Simple Harmonic Motion - 5/32 Jan – 2024
Simple Harmonic Motion
 Example 1
‽ A 0.2kg block connected to a light spring for which the force constant is 5 N/m is free to
oscillate on a frictionless, horizontal surface. The block is displaced 5 cm from
equilibrium and released from rest. A) Find the period of its motion. B) Determine the
maximum speed and acceleration of the block. C) Express the position, velocity, and
acceleration as functions of time.

6
ASTU Simple Harmonic Motion - 6/32 Jan – 2024
Simple Harmonic Motion
 Example 2
‽ What if the block were released from the same initial position, 𝑥𝑖 = 5 𝑐𝑚, but with an initial
velocity of 𝑣𝑖 = −0.100 𝑚/𝑠?

7
ASTU Simple Harmonic Motion - 7/32 Jan – 2024
Simple Harmonic Motion
 Energy of the Simple Harmonic Oscillator

 The kinetic energy of the block is

 The elastic potential energy stored in the


spring for any elongation 𝑥 is given by

Total mechanical energy

8
ASTU Simple Harmonic Motion - 8/32 Jan – 2024
Simple Harmonic Motion
 Example 3
‽ A 0.500kg cart connected to a light spring for which the force constant is 20.0 N/m oscillates on a frictionless,
horizontal air track. A) Calculate the maximum speed of the cart if the amplitude of the motion is 3.00 cm. B)
What is the velocity of the cart when the position is 2.00 cm? C) Compute the kinetic and potential energies of
the system when the position of the cart is 2.00 cm.

9
ASTU Simple Harmonic Motion - 9/32 Jan – 2024
Simple Harmonic Motion
 The Simple Pendulum

 The forces acting on the bob are the tension and the weight.
 T is the force exerted by the string
 mg is the gravitational force
 The tangential component of the gravitational force is the
restoring force.
 Recall that the tangential acceleration is

 The equation for 𝜃 is the same form as for the spring,


with solution
 This gives another differential equation  (t )   max cos(t   )
g  2 L
  so the period is T =  2 
L   g
10
ASTU Simple Harmonic Motion - 10/32 Jan – 2024
Simple Harmonic Motion
Damped Oscillations
 In many real systems, nonconservative forces such as friction or air resistance also act and
retard the motion of the system. Consequently, the mechanical energy of the system
diminishes in time, and the motion is said to be damped.

where 𝜔0 = 𝑘/𝑚 represents the angular frequency in the absence of a retarding force (the
undamped oscillator) and is called the natural frequency of the system.
11
ASTU Simple Harmonic Motion - 11/32 Jan – 2024
Simple Harmonic Motion
 When the magnitude of the retarding force is small such that
𝑏Τ
2𝑚 < 𝜔0 , the system is said to be underdamped.

A: underdamping: there are a few small oscillations before the oscillator


comes to rest.

 When 𝑏 reaches a critical value 𝑏𝑐 such that 𝑏𝑐ൗ2𝑚 = 𝜔0 , the


system does not oscillate and is said to be critically damped.

B: critical damping: this is the fastest way to get to equilibrium.

 If the medium is so viscous that the retarding force is large


compared with the restoring force that is, if 𝑏Τ2𝑚 > 𝜔0 , the
system is overdamped.
C: overdamping: the system is slowed so much that it takes a long time to
get to equilibrium.
12
ASTU Simple Harmonic Motion - 12/32 Jan – 2024
Simple Harmonic Motion
Forced Oscillations

 Forced vibrations occur when there is a periodic driving force. This force may or may
not have the same period as the natural frequency of the system.
 If the frequency is the same as the natural frequency, the amplitude becomes quite large.
This is called resonance.

13
ASTU Simple Harmonic Motion - 13/32 Jan – 2024
Wave Motion

 A wave is a disturbance that carries energy


from place to place.

 A wave does NOT carry matter with it! It just


moves the matter as it goes through it.

14
ASTU Wave Motion - 14/32 Jan – 2024
Wave Motion
 Some waves do not need matter (called a “medium”) to be able to move (for example,
through space). These are called electromagnetic waves (or EM waves).
 Some waves MUST have a medium in order to move. These are called mechanical waves.

15
ASTU Wave Motion - 15/32 Jan – 2024
Wave Motion
 Type of wave
1. Transverse waves: Waves in which the medium moves at right angles to the direction of the
wave.

2. Compressional (or longitudinal) waves: Waves in which the medium moves back and
forth in the same direction as the wave.

16
ASTU Wave Motion - 16/32 Jan – 2024
Wave Motion
 Crest: the highest point of the wave.  Frequency (f): how many waves go past a point
in one second; unit of measurement is hertz (Hz).
 Trough: the lowest point of the  Wavelength (λ): The distance between one point
wave. on a wave and the exact same place on the next
wave.
 Compression: where the particles  Amplitude (A): how far the medium moves from
are close together rest position (where it is when not moving).
 Period (T): is the time it takes for one cycle to
 Rarefaction: where the particles are complete.
spread apart

17
ASTU Wave Motion - 17/32 Jan – 2024
Wave Motion
 Traveling wave
 The function describing the positions of the elements
of the medium through which the sinusoidal wave is
traveling can be written

18
ASTU Wave Motion - 18/32 Jan – 2024
Wave Motion
 Reflection and Transmission of Waves
 A wave reaching the end of its medium, but where the medium is still free to
move, will be reflected (b), and its reflection will be upright.
 A wave hitting an obstacle will be reflected (a), and its reflection will be inverted.

19
ASTU Wave Motion - 19/32 Jan – 2024
Wave Motion

 In this situation part of the wave is reflected, and


part of the wave is transmitted.
 Part of the wave energy is transferred to the more
dense medium, and part is reflected.
 The transmitted pulse is upright, while the reflected
pulse is inverted.

 The speed and wavelength of the reflected wave


remain the same, but the amplitude decreases.
 The speed, wavelength, and amplitude of the
transmitted pulse are all smaller than in the incident
pulse.
20
ASTU Wave Motion - 20/32 Jan – 2024
Wave Motion
 Reflection;
 Bounce off of wave.
 Occurs when a waves reaches an obstacle/barrier.
 Traveling in the opposite direction.
 Its frequency does not change.
 Obey first law of reflection of light.
 The angle of incident = the angle of reflection

21
ASTU Wave Motion - 21/32 Jan – 2024
Wave Motion

 Diffraction;
 A spreading of wave after passing the edge of an obstacle or gap/slit.
 Narrow gap has more effect.
 Wide gap has less effect.

 Large obstacle, small wavelength =


low diffraction
 Small obstacle, large wavelength =
large diffraction

22
ASTU Wave Motion - 22/32 Jan – 2024
Wave Motion
 Refraction;
 breaking of wave.
 Is a measure of the extent to which a medium reflects light.
 Change speed and direction as they move from one material to another.
 The wavelength may decrease/increase.
 It use in lenses, camera, telescope.

23
ASTU Wave Motion - 23/32 Jan – 2024
Wave Motion
 The superposition principle says that when two waves pass through the same point, the
displacement is the arithmetic sum of the individual displacements.
 In the figure below, (a) exhibits destructive interference and (b) exhibits constructive
interference.

24
ASTU Wave Motion - 24/32 Jan – 2024
Wave Motion
 Interference;
 Add up or cancel out.
 There are two types: constructive and destructive.
 Constructive;  Destructive;
 If two waves are in phase with each other  If two waves are out of phase with each
they combine to make a bigger wave. other they cancel each other, so that there is
 Constructive interference occurs when the no wave.
crests of one wave are over the crests of
another wave

25
ASTU Wave Motion - 25/32 Jan – 2024
Light and Optics
 light travels in a straight-line path in a homogeneous medium, until it encounters a boundary
between two different materials.

 The reflection of light from such a smooth surface


is called specular reflection.
 The reflection from any rough surface is known
as diffuse reflection.

 The angle of reflection equals the angle


of incidence:

26
ASTU Light and Optics - 26/32 Jan – 2024
Light and Optics

27
ASTU Light and Optics - 27/32 Jan – 2024
Light and Optics
The Law of Refraction
 The index of refraction, 𝑛, of a medium is defined as:

 As light travels from one medium to another,


its frequency doesn’t change.

Snell’s law of refraction.

28
ASTU Light and Optics - 28/32 Jan – 2024
Light and Optics
 At some particular angle of incidence 𝜃𝑐 , called the critical angle, the refracted light ray
moves parallel to the boundary so that 𝜃2 = 90𝑜 . For angles of incidence greater than 𝜃𝑐 ,
the ray is entirely reflected at the boundary.

29
ASTU Light and Optics - 29/32 Jan – 2024
Light and Optics
 Example 4
‽ A light ray of wavelength 589 nm (produced by a sodium lamp) traveling through air is
incident on a smooth, flat slab of crown glass at an angle 𝜃1 = 30𝑜 to the normal. (a) Find
the angle of refraction, 𝜃2 . (b) At what angle 𝜃3 does the ray leave the glass as it re-enters
the air?

30
ASTU Light and Optics - 30/32 Jan – 2024
Image Formation
 Images are formed at the point where rays of light actually intersect or where they appear to
originate.

 The image formed by an object placed in front


of a flat mirror is as far behind the mirror as
the object is in front of the mirror.

 The lateral magnification M is


defined as:

31
ASTU Image Formation - 31/32 Jan – 2024
End

32
ASTU End - 32/32 Jan – 2024

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