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ADVENT OF MODERN
PHYSICS
CHAPTER # 17
2ND YEAR PHYSICS
1
RELATIVISTIC MECHANICS
 The branch of physics which deals with the relative motion of
observer and object is called Relative Mechanics.
 In physics, relativistic mechanics refers to mechanics compatible with special
relativity and general relativity.
Syeda fatima rizvi
2
FRAME OF REFERENCE
FRAME OF
REFERENCE
Frame of reference is a co-
ordinate system in which
measurement is carried out.
In order to know the change in
position of an object a
reference point is required.
Point O in the figure is
the reference point or Origin
and together with three axes,
this system is called the
coordinate system.
INERTIAL FRAME OF
REFERENCE
The frame of reference moving
with constant velocity i.e. zero
acceleration is called inertial
frame of reference
Newton laws of mechanics are
applicable in inertial frame of
reference
NON INERTIAL FRAME
OF REFERENCE
The frame of references having
acceleratory motions are called
non-inertial frame of references
Newton laws of mechanics are
not applicable in non-inertial
frame of references.
Syeda fatima rizvi
3
THEORY OF RELATIVITY
SPECIAL THEORY OF RELATIVITY
The part of relative mechanics that deals with
the inertial frame of references is called
special theory of relativity.
GENERAL THEORY OF RELATIVITY
The part of relative mechanics that deals with
non inertial frame of references is called
general theory of relativity.
Syeda fatima rizvi
4
Syeda fatima rizvi
5
BASIC ASSUMPTIONS OF SPECIAL
THEORY OF RELATIVITY
 The motion of a body can be represented by same equation of motion for all the
inertial frame of reference whatever is their velocity.
 For all the inertial frame of reference the velocity of light remains constant. i.e. c =
3 x 108 m/s.
Syeda fatima rizvi
6
RESULTS OF SPECIAL THEORY OF
RELATIVITY
Syeda fatima rizvi
7
MASS VARIATION
According to the special theory of relativity, the mass of
an object in a frame of reference at rest is called its rest mass mo. if this mass is
measured by an observer moving with a constant speed v relative to the object,
then it will not remain constant if the speed v is comparable to c. The mass m in
the moving frame will vary according to the mass variation
Syeda fatima rizvi
8
Syeda fatima rizvi
9
LENGTH CONTRACTION
In the theory of special relativity it has been found that the measurement of
length of a rod in a stationary frame of reference is not the same when the rod
is measured by the observer in the moving frame of reference with the velocity
relative to the rod, provided that the measurement is made along the direction
of motion.
Syeda fatima rizvi
10
Syeda fatima rizvi
11
Syeda fatima rizvi
12
TIME DILATION
Time is regarded as an absolute quantity in classical mechanics whereas in the
special theory of relativity it is considered to be a relative entity based on the
measurement of time in frame of references in relative motion.
The time interval between two events taking place at the same point in space as
timed with a clock at rest with respect to that point is called the proper time
interval and is denoted by To. Time measured with a clock in motion with
respect to the events is known as relativistic time it is represented by T. Both of
the time intervals To & T refer to the time elapsed between the same pair of
events occurring in the two frames moving with a relative speed v.
Syeda fatima rizvi
13
Syeda fatima rizvi
14
MASS ENERGY RELATION
We know that the speed of light is a universal constant. We cannot reach speeds
greater than the speed of light by the relativistic addition of velocities. The question is
how to reconcile with this result of special relativity with Newton's second law, F=ma. It
would be seen that any constant force, no matter how small, applied for a considerably
very long time, should continuously accelerate any mass 'm' at a rate a=f/m until the
speed was arbitrarily very large. Einstein, concluded that energy has inertia i.e. the
more energy a body possess, the more inertia that body will display. Since, inertia is a
property of matter, which is associated with mass. Thus from Einstein's argument mass is
simply a property attributed to the total energy of the body and only the total energy is
required, to know the total mass of the body. Thus, in special theory of relativity total
energy and mass are related by the famous Einstein's equation.
E=mc2
Syeda fatima rizvi
15

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Modern Physics: Relativity Mechanics & Mass-Energy Relation

  • 1. ADVENT OF MODERN PHYSICS CHAPTER # 17 2ND YEAR PHYSICS 1
  • 2. RELATIVISTIC MECHANICS  The branch of physics which deals with the relative motion of observer and object is called Relative Mechanics.  In physics, relativistic mechanics refers to mechanics compatible with special relativity and general relativity. Syeda fatima rizvi 2
  • 3. FRAME OF REFERENCE FRAME OF REFERENCE Frame of reference is a co- ordinate system in which measurement is carried out. In order to know the change in position of an object a reference point is required. Point O in the figure is the reference point or Origin and together with three axes, this system is called the coordinate system. INERTIAL FRAME OF REFERENCE The frame of reference moving with constant velocity i.e. zero acceleration is called inertial frame of reference Newton laws of mechanics are applicable in inertial frame of reference NON INERTIAL FRAME OF REFERENCE The frame of references having acceleratory motions are called non-inertial frame of references Newton laws of mechanics are not applicable in non-inertial frame of references. Syeda fatima rizvi 3
  • 4. THEORY OF RELATIVITY SPECIAL THEORY OF RELATIVITY The part of relative mechanics that deals with the inertial frame of references is called special theory of relativity. GENERAL THEORY OF RELATIVITY The part of relative mechanics that deals with non inertial frame of references is called general theory of relativity. Syeda fatima rizvi 4
  • 6. BASIC ASSUMPTIONS OF SPECIAL THEORY OF RELATIVITY  The motion of a body can be represented by same equation of motion for all the inertial frame of reference whatever is their velocity.  For all the inertial frame of reference the velocity of light remains constant. i.e. c = 3 x 108 m/s. Syeda fatima rizvi 6
  • 7. RESULTS OF SPECIAL THEORY OF RELATIVITY Syeda fatima rizvi 7
  • 8. MASS VARIATION According to the special theory of relativity, the mass of an object in a frame of reference at rest is called its rest mass mo. if this mass is measured by an observer moving with a constant speed v relative to the object, then it will not remain constant if the speed v is comparable to c. The mass m in the moving frame will vary according to the mass variation Syeda fatima rizvi 8
  • 10. LENGTH CONTRACTION In the theory of special relativity it has been found that the measurement of length of a rod in a stationary frame of reference is not the same when the rod is measured by the observer in the moving frame of reference with the velocity relative to the rod, provided that the measurement is made along the direction of motion. Syeda fatima rizvi 10
  • 13. TIME DILATION Time is regarded as an absolute quantity in classical mechanics whereas in the special theory of relativity it is considered to be a relative entity based on the measurement of time in frame of references in relative motion. The time interval between two events taking place at the same point in space as timed with a clock at rest with respect to that point is called the proper time interval and is denoted by To. Time measured with a clock in motion with respect to the events is known as relativistic time it is represented by T. Both of the time intervals To & T refer to the time elapsed between the same pair of events occurring in the two frames moving with a relative speed v. Syeda fatima rizvi 13
  • 15. MASS ENERGY RELATION We know that the speed of light is a universal constant. We cannot reach speeds greater than the speed of light by the relativistic addition of velocities. The question is how to reconcile with this result of special relativity with Newton's second law, F=ma. It would be seen that any constant force, no matter how small, applied for a considerably very long time, should continuously accelerate any mass 'm' at a rate a=f/m until the speed was arbitrarily very large. Einstein, concluded that energy has inertia i.e. the more energy a body possess, the more inertia that body will display. Since, inertia is a property of matter, which is associated with mass. Thus from Einstein's argument mass is simply a property attributed to the total energy of the body and only the total energy is required, to know the total mass of the body. Thus, in special theory of relativity total energy and mass are related by the famous Einstein's equation. E=mc2 Syeda fatima rizvi 15