Recapitulate Proper length Proper frame of reference Proper

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Recapitulate • Proper length (ℓ). • Proper frame of reference. • Proper time interval

Recapitulate • Proper length (ℓ). • Proper frame of reference. • Proper time interval ( ) • Length Contraction Formula. • Time Dilation Formula.

Measuring Length of Platform Measurement of length of a platform by an observer stationary

Measuring Length of Platform Measurement of length of a platform by an observer stationary on the platform and another moving in a train with relativistic speed. Assume both frames to be inertial.

S’ v S A B

S’ v S A B

Define Events E 1: The origin of S’ coinciding with end A of platform.

Define Events E 1: The origin of S’ coinciding with end A of platform. E 2: The origin of S’ coinciding with end B of platform.

In S E 1: (x 1, t 1) E 2: (x 2, t 2)

In S E 1: (x 1, t 1) E 2: (x 2, t 2) Is x 2 -x 1= L ? Is t 2 -t 1 proper ?

In S Length is proper.

In S Length is proper.

In S’ E 1: (x’ 1, t’ 1) E 2: (x’ 2, t’ 2)

In S’ E 1: (x’ 1, t’ 1) E 2: (x’ 2, t’ 2) Is x’ 2 -x’ 1= L’? Is t’ 2 -t’ 1 proper?

In S’

In S’

Applying inverse transformation.

Applying inverse transformation.

 -Meson Shower The incoming primary cosmic rays create -meson in the upper atmosphere.

-Meson Shower The incoming primary cosmic rays create -meson in the upper atmosphere. The life time of mesons at rest is 2 s. If the mean speed of meson is 0. 998 c, what fraction of mesons created at the height of 20 km reach the sea-level?

Assume -mesons to travel with constant speed. Decay time interval 2 x 10 -6

Assume -mesons to travel with constant speed. Decay time interval 2 x 10 -6 s is proper in -meson frame. In earth frame it is dilated. c=0. 998 c gives = 15. 82 Decay time in earth frame =15. 82 x 2 x 10 -6 s = 3. 164 x 10 -5 s

Time to travel to earth in earth frame =20 x 103/0. 998 c =

Time to travel to earth in earth frame =20 x 103/0. 998 c = 6. 68 x 10 -5 s The fraction reaching earth in earth frame can be calculate using

This fraction is 0. 12. Classically it would have been 3. 12 x 10

This fraction is 0. 12. Classically it would have been 3. 12 x 10 -15. What would an observer in – meson frame conclude?

Old Problem about Light Emission S’ c S c v

Old Problem about Light Emission S’ c S c v

Events E 1: Light reaching front wall of the train. E 2: Light Reaching

Events E 1: Light reaching front wall of the train. E 2: Light Reaching the back wall of the train.

In S’ Frame

In S’ Frame

Event 1 in S Frame Assume origins were coincident when light was emitted.

Event 1 in S Frame Assume origins were coincident when light was emitted.

Event 2 in S Frame

Event 2 in S Frame

As expected, we see that The time difference is given below.

As expected, we see that The time difference is given below.

Co-ordinate Difference The difference in co-ordinates of two events. Is it related to the

Co-ordinate Difference The difference in co-ordinates of two events. Is it related to the length of compartment? In which frame the length is proper?

The x 1 -x 2 is an overestimate of length of the train because

The x 1 -x 2 is an overestimate of length of the train because t 1>t 2. Can we get correct length? Yes, if we can find out the distance the train moved in the time difference.

vΔt x 2 x 1

vΔt x 2 x 1

Length in S

Length in S

Velocity Transformation We know the components of velocity a particle in S and want

Velocity Transformation We know the components of velocity a particle in S and want to find the same in S’ for the same particle.

Notation Relative velocity between frames. Constant as a function of time. Instantaneous velocity of

Notation Relative velocity between frames. Constant as a function of time. Instantaneous velocity of particle is S. Need not be constant. Instantaneous velocity of particle is S’. Need not be constant.

Events related to Displacement Imagine that a particle is moving in x- direction in

Events related to Displacement Imagine that a particle is moving in x- direction in a frame S. E 1: Particle found at x 1 at t 1. E 2: Particle found at x 2 at t 2.

Even if the velocity of particle is not constant in the limit Δt tending

Even if the velocity of particle is not constant in the limit Δt tending to zero would give the instantaneous velocity of particle in S.

If the motion is in threedimension, in general

If the motion is in threedimension, in general

Similarly looking at the same particle in S’, we can define:

Similarly looking at the same particle in S’, we can define:

Note that like displacement, the time difference has also to be measured in one’s

Note that like displacement, the time difference has also to be measured in one’s own frame.

Lorentz Transformation in differential form.

Lorentz Transformation in differential form.

Velocity Transformation

Velocity Transformation

Inverse Velocity Transformation

Inverse Velocity Transformation

Comment One can show that • If u<c in S, u<c in S’ also

Comment One can show that • If u<c in S, u<c in S’ also irrespective of v. • If u=c in S, u=c in S’ also irrespective of v.