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happyphysics.com Physics Lecture Physics Lecture Resources Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

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Page 1: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

happyphysics.com

Physics Lecture Physics Lecture ResourcesResources

Prof. Mineesh GulatiHead-Physics Wing

Happy Model Hr. Sec. School, Udhampur, J&K

Website: happyphysics.com

Page 2: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

Ch 37 Relativity

© 2005 Pearson Education

Page 3: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

37.1 Invariance of Physical Laws37.1 Invariance of Physical Laws

© 2005 Pearson Education

Same emf induced

Page 4: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

Einstein’s PostulateEinstein’s Postulate

First PostulateFirst Postulate: The laws of physics are : The laws of physics are the same in every inertial frame of the same in every inertial frame of reference.reference.

Second PostulateSecond Postulate: The speed of light in : The speed of light in vacuum is the same in all inertial vacuum is the same in all inertial frames of reference and is independent frames of reference and is independent of the motion of the source.of the motion of the source.

© 2005 Pearson Education

Page 5: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

© 2005 Pearson Education

Page 6: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

© 2005 Pearson Education

Galilean coordinate transformation

Page 7: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

Galilean coordinate Galilean coordinate transformationtransformation

' ' 'x x ut y y z z

Galilean velocity Galilean velocity transformationtransformation

'x xv v u

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Page 8: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

37.2 relativity of Simultaneity37.2 relativity of Simultaneity

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Page 9: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

© 2005 Pearson Education

Whether or not two events at different x-axis locations are simultaneous depends on the state of motion of the observer

Page 10: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

37.3 Relativity of Time Intervals

© 2005 Pearson Education

At rest: ∆t0=2d/c

Page 11: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

During time ∆tDuring time ∆t

2 2

22

2 2

0

0

2

2

( )2

2 2

2

2

2 2

1

u tl d

l u tt d

c c

c t u ttc

tt

uc

© 2005 Pearson Education

Page 12: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

time dilation

22

0

1 cu

tt

221

1

cu

0tt

© 2005 Pearson Education

Page 13: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

© 2005 Pearson Education

Page 14: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

Example 37.1High-energy subatomic particles coming from spHigh-energy subatomic particles coming from space interact with atoms in the earth’s upper atmace interact with atoms in the earth’s upper atmosphere, producing unstable particles called muoosphere, producing unstable particles called muons. A muon decays with a mean lifetime of 2.2*10ns. A muon decays with a mean lifetime of 2.2*10--

66s as measured in a frame of reference in which it s as measured in a frame of reference in which it is at rest. If a muon is moving at 0.99c relative to tis at rest. If a muon is moving at 0.99c relative to the earth, what will you measure its mea lifetime the earth, what will you measure its mea lifetime to be?o be?

ANS:ANS:

© 2005 Pearson Education

60

2 2 2

6

2.2 10

1 / 1 (0.99)

15.6 10

t st

u c

s

Page 15: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

37.4 Relativity of Length

0

2

2

0 1l

c

ull

length contraction

© 2005 Pearson Education

Page 16: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

Example 37.4

A spaceship flies past earth at a speed A spaceship flies past earth at a speed of 0.99c. A crew member on board the of 0.99c. A crew member on board the spaceship measures its length, obtaining spaceship measures its length, obtaining the value 400m. What length do the value 400m. What length do observers measure on earth?observers measure on earth?

ANS:ANS: 2

0 2

2

1

(400 ) 1 (0.99)

56.4

ul l

c

m

m

© 2005 Pearson Education

Page 17: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

37.5 The Lorentz Transformations

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Page 18: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

)(1

2

22

2

cuxtcu

cuxtt

zz

yy

utxcu

utxx

)(1 22

Lorentz coordinate transformation

21 cuv

uvv

x

xx

Lorentz velocity transformation

21 cvu

uvv

x

xx

© 2005 Pearson Education

Page 19: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

37.6 the Doppler Effect for Electromagnetic Waves

Doppler effect, electromagnetic waves

© 2005 Pearson Education

0fuc

ucf

Page 20: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

relativistic momentum

221 cv

m

vp

vp

37.7 Relativistic Momentum

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Page 21: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

37.8 Relativistic Work and Energy

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Page 22: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

relativistic kinetic energy

22

22

2

)1(1

mcmccv

mcK

total energy, rest energy, and momentum

2

22

22

1mc

cv

mcmcKE

2222 )()( pcmcE

© 2005 Pearson Education

Page 23: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

37.9 Newtonian Mechanics and Relativity

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Page 24: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

© 2005 Pearson Education

All of the fundamental laws of physics have the same form in all inertial frames of reference. The speed of light in vacuum is

the same in all inertial frames and is independent of the motion of the source. Simultaneity is not an absolute concept; events that are simultaneous in one frame are not necessarily simultaneous in a second frame moving relative to the first.

Page 25: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

If two events occur at the same space point in a particular frame of reference, the time interval ∆t0 between the events as measured in that frame is called a proper time interval. If this frame moves with constant velocity u relative to a second frame, the time interval ∆t

between the events as observed in the second frame is longer than ∆t0 . This effect is called time dilation. (Examples 37.1 through

37.3)

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Page 26: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

If two points are at rest in a particular frame of reference, the distance l0 between the points as measured in that frame is

called a proper length. If this frame moves with constant velocity u relative to a second frame and the distances are measured parallel to the motion, the distance l between the

points as measured in the second frame is shorter than l0 . This effect is called length contraction. (See Examples 37.4 through

37.6)

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Page 27: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

The Lorentz coordinate transformation relates the coordinate and time of an event in an inertial frame S to the coordinates and time of the same event as observed in a second inertial frame S’

moving at velocity u relative to the first. For one-dimensional motion, a particle’s velocities vx in S and v’x in S’ are related by the Lorentz velocity transformation. (See Examples 37.7 and 37.8)

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Page 28: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

© 2005 Pearson Education

The Doppler effect is the frequency shift in light from a source due to the relative motion of source and observer. For a source moving toward the observer with speed u, Eq.(37.25) gives the received frequency f in terms of the emitted frequency f0.(See

Example 37.9)

Page 29: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

For a particle of rest mass m moving with velocity , the relativistic momentum is given by Eq. (37.27) or (37.31) and the relativistic kinetic energy K is given by Eq. (37.36). The total energy E is the sum of the kinetic energy and the rest energy mc2 . The total energy can also be expressed in terms of the magnitude of momentum p and rest mass m. (See Examples 37.10 through 37.12)

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v

p

Page 30: Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com

© 2005 Pearson Education

The special theory of relativity is a generalization of Newtonian mechanics.

All the principles of Newtonian mechanics are present as limiting cases when all the speeds are

small compared to c. Further generalization to

include noninertial frames of reference and their

relation to gravitational fields leads to the general

theory of relativity.

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