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Periodic motion
When an object repeats its motion after fixed
interval of time, this type of motion is
called periodic motion.
For Example: motion of planets
around the sun,
motion of hands of a clock, motion of pendulum.
Oscillatory motion
Oscillatory motion is a specific type
of periodic motion in which a body
moves back and forth about a fixed
point, called mean position.
Simple Harmonic Motion (S.H.M.)
Simple Harmonic Motion is a motion in
which the acceleration of the particle is
always directed towards a fixed point on a
straight line and is proportional to the
displacement of the particle from that point.
Examples of SHM
1.The motion of a bob of a simple pendulum.
2.The motion of the mass attached to a spring.
•The motion of liquid oscillating in a U-tube.
For Example: motion of a pendulum, the
vibrations produced in strings of a guitar.
Displacement:
The distance of a particle executing SHM
from its mean position, at a given instant is
called displacement.
OM = y is the displacement of the particle at any time t.
Few important terms
completed in one second.
n =
from the mean position is called its
amplitude.
The maximum displacement = OY
A m plitude =
ymax = OY = r
Time Period(T): The time taken to complete one
vibration is known as time period.
Amplitude:
The maximum displacement of the particle
Frequency(n): The number of vibrations
1
T
Angular velocity =
Angular velocity:
=
=
2 n
Angle described in one revolution
Time taken to complete one revolution
2
T
sin
=
Equationof simple Harmonic Motion
(expression for displacement)
OM = y
Let particle P traces an angle
at o after time t.
POX =
Also MPO =
OM = OP sin
M
O
P
yOM
OP
y = r sin
or y = r sin
t
M
y = r cos
or y = r cos t
POX = = MPO
Also NPQ =
(i)v cos along the diameter
YOY'
(ii)v sin perpendicular to the diameter YOY'
Only velocity to M is given by the component v cos
Component (v sin ) has no effecton
the motion of M.
Velocity of a particle executing SHM
Special Cases:
(a) When y = 0 i.e. displacement is zero or the
body is at mean position.
= v
= v 1
=
velocity of M, V =
velocity
of M, V= v cos
1 sin2
2
r
y
r2 y2
r
=
vr r2
y2
r
r2
y2
( y = r sin
)
This value of velocity is called velocity amplitude of SHM.
(b) When y = r i.e. displacement is maximum or
the body is at extreme position.
From Eq. (1),Vmax = r (max.
velocity)
Vmin = 0 (minimum velocity)
using velocity of M, V =
r2 y2
r
This centripetal acceleration is
resolved into
components.
two rectangular
The centripetal acceleration
acting at P is along PO
(ii) v cos perpendicular to
YOY'.
(i) v sin along PN i.e. along the diameter
YOY'
Acceleration of a particle executing SHM
v2
r
2
r
2
But the actual expression for acceleration is given by
a = – 2y
It also shows that acceleration is always directed
towards point o.
= r
sin
Acceleration of
M, a =v sin
Component (ii) has no effect on the motion of M.
2
r2 2
r
a
=
2y
= 2 r
sin
(b) If y =r i.e. displacement is maximum or the
body is at extreme position.
From Eqn. (2) acceleration, amax
(maximum acceleration)
=
2
r
Special Cases:
(a) If y = 0 i.e. displacement is zero or the
body is at mean position.
From Eqn. (2) acceleration, amin = 0
acceleration)(minimum
The magnitude of the acceleration of a particle
executing SHM is
a = 2y (neglecting negative sign)
Velocity of a particle executing SHM
Expression for the time period and frequency
of a particle executing SHM
But
=
, where T is the time period
a
acceleration
y displacement
=2
T
or frequency, n =
or Time period, T =
2
acceleration
displacement
2
T=
displacement
acceleration
1 acceleration(a)
2 displacement(y)
i.e. x Fa (Applied force = Fa = Deforming force)
Deformation Deforming force.
Hook’s Law
It states that deformation is always proportional
to the deforming force.
or
or Fa = K x where K is constant of
proportionality and is called spring factor or
or theforce constant stiffness factor of
spring.
Fa x
Definition of spring factor
It is defined as the force in newtons required
to stretch the spring through 1m.
Also we know Fa = – Fr
Fr = – K x
Since Fa =K x , If x = 1 m
Then Fa = K
Vibrations of a mass attached to a spring
(i)Vertical oscillations
•Horizontal oscillations.
(i) Oscillationsof a mass attached with
a vertical spring.
Thus Fa = – Fr
From (1) and (2) Ma = – K x
If 'a' be the acceleration produced by the force Fr
in a mass M, then
x
M
a K
Now we know Time period,
displacement
accelerationT =
2
Fr = Ma .....(1)
also by Hook's law Fr = – K x .....(2)
K
If n be the frequency of vibrations, then
1 1
n = =2
T
1 K
2 M
M
T =
2
(ii) Oscillations
horizontal spring.
of mass attached with a
M
K
T =
2
n = 1
1=
2
T
1 K
2 M
Vibrations of Loaded Beam
(a) Beam supported at one end.
Cantilever: A beam fixed horizontally at
one end and free to vibrate at the other
end is called cantilever.
T
=
2
p
g
Free vibrations:
When a body is set into vibrations and is
allowed to vibrate freely under the influence of
its own elastic forces
called free vibrations.
such vibrations are
lT =2
g
n =1
g
2 l
Damped Vibrations
Vibrations in which energy continuously goes
on dissipating and finally the motion die
out, are called damped vibrations.
Vibrations in which the body vibrate with a
frequency other than its natural frequency
under the external periodic force, are
called forced vibrations.
Example: 1.Child's swing with external force.
2. Vibrating pendulum with some force.
Resonant vibration
A special type of forced vibration in which
the frequency of applied force matches
with natural frequency of the body is
called resonant vibration.
Forced Vibrations
The phenomenon of making a body to vibrate
with its natural frequency under the influence
of another vibrating body with the same
frequency, is called resonance.
Resonance
Definition of wave or wave motion
motion is being
particle to another.
handed over from one
or wave
It is a form of disturbance which travels
through the material medium due to therepeated periodic motion of the vibrating
particles about their mean position and the
(a) Elasticity
(b) Inertia
(c) Minimum friction
Types of waves or wave motion :
1. Longitudinal wave motion
2. Transverse wave motion
Properties:
LONGITUDINAL WAVE MOTION
mean position in the
propagation of the wave.
Example:
1. Sound waves.
2. Wavesproducedinairbycompressing and
releasing spring.
C = Compression R = Rarefaction
C RC
It is that type of wave motion in which
particles of the medium vibrate about their
direction of
It is that type of wave motion in which
particles of the medium vibrate about their
mean position perpendicular to the
direction of propagation of the wave.
Examples:
1.Light waves .
2.All electro-magnetic waves are
transverse in nature i.e. Radio waves, X- rays,
- rays etc.
3.Waves produced on the surface of
water when a
piece of stone is dropped into it.
WaveParticles
TRANSVERSE WAVE MOTION
distance
crest.
Trough: The point on the wave at the
maximum distance below the mean position is
called trough.
T
Crest: The point on the wave at the maximum
from the mean position is called
C
A B
Also AB =
A FEW DEFINITIONS
(i) Wavelength ( ):
It is the distance travelled by the wave in onecomplete cycle.
C
T
A BM
It is defined as the distance travelled by the
wave per unit time.
Relation between Velocity (v),Frequency (n) and Wavelength () of the
wave.
Wave velocity (v):
Wavelength () is the distance travelled by the
wave in one time period (T).Wavelength ()
distan ce
timeVelocity =
Velocity = Time period (T) T
or v = n for light wave, c = v
Distinction Between Transverse & Longitudinal Waves
Transverse Waves Longitudinal Waves
1. Particles of the medium
vibrate perpendicular
to the wave.
2. Travels in the form of
crest and trough.
3. Transverse wave can
be polarised.
4. There is no change in
the density of the
medium.
1. P a r t i c l e s o f t h emedium vibrate parallel
to the wave.
2. Travels in the form of
compression and
rarefaction.
3 Longitudinalwaves
cannot be polarised.
4. There is change in the
density of the
medium.
2. Applications of sound waves
The branch of physics which deals with
the design and construction of halls,
theatre, auditorium etc. with best sound
effect is called acoustics of buildings.
Co-efficient of absorption of sound
An open window acts as a perfect
absorber of sound energy. The absorption co-
efficient of an open window is one i.e. 100%.
a =
Acoustics of Building:
Sound energy absorbed by the surface
Total sound energy incident upon the surface
Musical sound: It produces pleasant effect
on the ear. It’s curve is regular and has a
definite amplitude. Fig. (a)
Musical Sound And Noise
Noise: It produces unpleasant effect on the ear.
The curve is irregular and has no definite
amplitude. Noise is usually of low frequency.
Noise
The persistence sound in a room or hall after
the original sound has been stopped is
called Reverberation.
Reverberation
It is defined as the time required for the
intensity of sound to fall to one millionth
(10–6th) of its original intensity after
the source stops sounding.
Sabine's formula for reverberation time (T)
Standard Reverberation time
T= .............10.16 V
as
V = the volume of the room in cubic metres (m3).
S = area of the surfaces in square metres (m2).
a = the coefficient of absorption.
a s = the total surface absorption of materials.
Factors on Which Reverberation Time Depends
1.Size of room or hall.
2.Total absorption by the various surfaces.
Q. A cinema hall has volume of 7500 m3. It
is required to have reverberation time 1.5
sec. What would be the total absorption in the
hall ?
i.e. a s = a1 s1 + a2 s2 + a3 s3 + ...... an sn
= 800 units
0.16 V
T
0.16 7500
1.5as = =
Methods to control reverberation time
1. Covering the walls and floor with
absorbing materials.
2. By providing a few open windows.
3. By using false ceiling.
4. By increasing good number of audience.
5. By using heavy curtains with folds.
6. By using upholstered seats in the hall.
Echo
Echo is repetition of sound due to reflection
from some object.
Thus sound must travel (d = v × t) = 332 × 1
=33.2 metres, for an echo to be heard.
So that minimum distance of the large
reflecting surface from the listener should be
= 16.6 m
Remedy: To avoid confusion between
original sound and its echo the surfaces
must be covered with good absorbing
material.
10
Audio frequency range is 20Hz to 20kHz.
Infrasonics
The sound waves having frequency less than
20Hz are called as Infrasonics.
Ultrasonics
The sound waves having
frequency more
than 20kHz are called as ultrasonics.
Audible range of sound waves
Production of Ultrasonic Waves
(1) Magnetostriction Oscillator
Principle : It is based upon magnetostriction
effect.
“If a ferromagnetic material in the form of
a rod (iron or nickel), is subjected
to alternating magnetic field, the rod
expands and contracts in length alternately.”
Construction
High frequency oscillator
A rod of Nickel or Invar
( 36% Ni + 64% Fe) is
clamped in the middle. L1 and L2 are two
coils surrounding the rod XY. Coils are
connected with High frequency oscillator.
l = Length of rod, = Density of material
Y = Young’s modulus of elasticity.
1. High frequency A.C. current is
passed through coil L1.
2. As a result of this alternating magnetic field is
associated with the coil which makes the bar
magnetised and demagnetised.
3. The length of the rod changes and free ends
begin to vibrate.4. Thus high frequency ultrasonics are
produced.
Working
n =1 Y
2l
Applications of ultrasonics
1. Drilling : A ferromagnetic rod is placed in a
coil through which high frequency A.C. is
passed. At the lower end of rod a tool bit is
attached. The rod vibrates with high frequency.
The bit moves up and down very fast and thus
make a hole in the material placed below.
Rod
Tool bit
A ferromagnetic rod is placed in a coil through which
high frequency A.C. is passed. At the lower end of rod
a hammer is attached. The rod vibrates with high
frequency and hammer hits the plates. The molecules
of plates start vibrating and diffuse into each other
and thus sheets get welded.
(2) Cold Welding :
(3) Ultrasonic cleaning :
Ultrasonic waves cause violent agitation when
transmitted through a liquid. Cleaning job is put in
a detergent solution and then ultrasonic waves
are passed. Strong agitations of molecules perform a
super cleaning job on small pieces of machinery.
The principle of SONAR is same as that of
RADAR.
1. It is used to measure the depth of sea water.
2. It is also used to detect ice berg or
submarine in the sea water.
3. It helps sailor to steer ship in a safer
(4) SONAR : Sound Navigation and Ranging.
direction.
4. Knowing the velocity of ultrasonic waves
and time taken by the wave, the distance
(depth) can be determined.
d =v x t
2
1st SessionalFeb.2014
Subject : Applied Physics – II
Section –ANote : Attempt all the Questions 5×1 = 5
I.Define Acoustics of Buildings.
II.Define Noise.
III.Define Simple Harmonic Motion.
IV.Define Cantilever.
V. Define Wavelength.
Section – BNote : Attempt any four Questions 4×5 = 20
2. Explain construction and working of
Magnetostriction oscillator?
3. What are the methods to control
reverberation time?
Q.4 Explain
transverse and longitudinal waves?
5. What are free and forced vibrations?
6. Calculate the displacement and velocity
for S.H.M?
1st SessionalFeb.2015
Subject : Applied Physics – II
Section – ANote : Attempt all the Questions 5×1 = 5
I.Define wave motion by giving examples.
•Give relation between wave
velocity,
frequency and wavelength.
III.Define cantilever and give the formula of
time period of cantilever.
IV.Define What is acoustics and
acoustics of buildings.
•Give full form of SONAR.
Section – BNote : Attempt any four Questions 4×5 = 20
2. What is SHM? Derive an expression for
velocity of SHM.
3. What is Reverberation? Give methods to
control Reverberation.
Q.4 Discuss
by giving example free vibration & resonant
vibration.
5. Explain principle, construction & working of
magnetostriction oscillator.
• Give difference between transverse and
longitude wave.
1. Principles of optics
(1) Reflection :
When light is incident on the surface of an
object, some of the light is bounced back into
the same medium. This phenomenon is called
as reflection of light.
M1 M2
rayray
(i)The incident ray, the reflected ray and the
normal at the point of incidence all lie in the
same plane.
(ii)The angle of incidence is equal to the angle
of reflection.
i= r
The laws of reflection are :
Real and Virtual Objects and Images
(i)An object is said to be real when light
diverges from it.
(ii)An object is said to be virtual when light
converges towards it.
(iii)An image is said to be Real when light
converges towards it. It can be obtained on
screen.
(i)An image is said to be virtual when light
diverges from it. It can not be obtained on the
screen.
(a)All the distances along the principal axis are
measured from the pole of the spherical mirror.
(b)The distances measured in the same direction
as that of the incident light are taken as
positive, while the distances measured in the
direction opposite to that of incident light are
taken as negative.
(c)The distances perpendicular to the principal
axis (i.e. size of object and size of image) are
taken as positive if measured in upward
direction but negative if measured in downward
direction.
Sign Conventions:
Sign Conventions
Height upward
(positive)
Height downwards (negative)
In the direction of
light (positive)
Against incident light
(negative)
where v = image-distance i.e. the distance
from the pole to the image.
u =object-distancei.e.thedistancefrom
the pole to the object.
f =focallengthi.e.thedistancefromthe
pole
to the focus F.
Spherical mirror formula
1
1=
1
v u f
Also f =R
2
Linear Magnification
m =sizeof image
sizeof object
I
O
v
um = =
Uses of Spherical Mirrors
Concave mirrors
1.They are used in search lights.
2.They are used in solar cookers to focus sunlight.
3.Concave mirrors are used by doctors to focus
light on certain parts of the body.
4.It is also used as shaving mirror.
Convex mirrors
1. Widelyused as rear view mirrors in
cars, scooters etc.
2. They are used as reflectors in street lights.
Refraction of Light
The phenomenon of bending of light
rays while passing from one medium to
another is called Refraction of light.
(i)The incident ray, refracted ray and the
normal at the point of interface all lie in the
same plane.
(ii)The ratio of sine of the angle of
incidence to the sine of the angle of
refraction is constant for a given pair of media.
(This law is also known as the SNELL’s law).
The Snell’s law
The laws of refraction are :
=Constant =a g
sin i
sinr
Where a g is the refractive index of glass w.r.t.
Air.
Absolute refractive index of a medium
a m =Velocityof light in air Velocityof light inMedium
c
v
Lenses
A lens is made of a homogeneous transparent
material bounded by two spherical surfaces or
one spherical and one plane surface.
Where C = 3 x 108 m/s
Lenses are of two types :
Formation of Images by a Convex Lens
Image formation with a Concave Lens
Lens Formula
=11 1
v u f
where v = image-distance
u = object-distance
f = focal length
m =
Note: If ‘m’ is positive then image will be
virtual and erect if ‘m’ is negative, then image
will be real
lenses.
and inverted for mirrors and
It is same for both type of
lenses
Linear Magnification
image height
object height
size of image
size of object=
I vm = =
O u
It is reciprocal of the focal length measured in
metre.
Power of a Lens
P =1
f metre
The unit of the power of lens is ‘Dioptre’ and
is
indicated by the symbol ‘D’.
Thus if the focal length of a lens is 0.25 m, its
power will be ?
P is positive for a convex lens and that of a
concave lens is negative.
Q. Two lenses, one of focal length 20 cm
(convex lens) and another of focal
length
–10cm (concave lens) are placed in contact.
What is the focal length and power of the
combination?
Ans. P = - 5D, F = - 0.2 m
P = P1 + P2
Power of combination of Lenses
1 1
F f1
1
f2
(i) Simple microscope ( A convex lens of small F.L.)
(ii) Compound microscope
Near point or least distance of distinct vision (D)
It is the minimum distance from the eye at
which an object can be seen clearly.
Standard near point distance D = 25 cm.
Microscope :
It is an
instrument image
of small object.
that produces enlarged
Magnifying Power (M)
It is the ratio of the angle subtended by
the image to the angle subtended by the
object at naked eye at the near point.
(i) Simple microscope
M = 1 D
f
(ii) Compound microscope
L = Distance between two lenses.
1 fe
L D
fo
M =
Telescope
(i) Astronomical telescope :
(ii) Terresterial telescope :
(iii)Galilian telescope :
Length of tube remains fixed i.e. L= (fe+fo)
M = –fo
fe
Total Internal reflection
When the angle of incidence of a ray of light
travelling in a denser medium is greater than
the critical angle for the two media, the ray is
totally reflected back into the same
medium. This phenomenon is called total
internal reflection of light.
The critical angle for a medium is the angle of
incidence in the medium for which the angle of
refraction in air is 90°.
Conditions for Total Internal Reflection.
(i)The incident light must pass from a denser
medium into a rarer medium.
•The angle of incidence in denser medium
must be greater than critical angle (ic).
Critical angle
Refractive index,
=
1 1
sine of critical angle sin ic
1st SessionalFeb.2014
Subject : Applied Physics – II
Section –ANote : Attempt all the Questions 5×1 = 5
I.Define Acoustics of Buildings.
II.Define Noise.
III.Define Simple Harmonic Motion.
IV.Define Cantilever.
V. Define Wavelength.
Section – BNote : Attempt any four Questions 4×5 = 20
2. Explain construction and working of
Magnetostriction oscillator?
3. What are the methods to control
reverberation time?
Q.4 Explain
transverse and longitudinal waves?
5. What are free and forced vibrations?
6. Calculate the displacement and velocity
for S.H.M?
THANK YOU