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  • 1

    6

  • 2 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    Recapitulate We applied the postulates of

    special theory of relativity and arrived at Lorentz transformation.

    We took an old example and showed that speed of light indeed remains constant in two frames under Lorentz Transformation.

  • 3 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    Lorentz Transformation

    2

    = x x - vt

    y y

    z z

    vxt t

    c

    2

    1

    1

    v

    c

  • 4 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    Length Contraction

    Proper length of a rod is length measured in a frame in which it is at rest.

    Proper frame is a frame in which the rod is at rest.

  • 5 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    Let us first assume that the rod is placed along x-axis.

    Its proper length is largest.

    Its length is shorter in other frames.

  • 6 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    Length Measurement

    Measure the co-ordinates of the two ends of the rod.

    Is time of measurement important? Yes only if rod is moving.

  • 7 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    X1 X2

    Moving Rod

    If the co-ordinates are measured at two different time, their difference does not give the correct length.

  • 8 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    There may be other methods of measuring the length of a moving rod, some would be discussed later. But the co-ordinate difference of a moving rod would give length only if the two ends are measured at the same time.

    Moving Rod

  • 9 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    Let S be the frame in which the rod is at rest.

    O O

    z

    x

    y y

    z

    S S

    A B

  • 10 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    Events

    E 1: Observer in S measures the co-ordinate of A end of the rod. (x1, t1) E 2: Observer in S measures the co-ordinate of B end of the rod. (x2, t2)

  • 11 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    2 1 x x L in S only if 2 1 (say)t t t

    22 2 2 2

    11 1 1 2

    ,

    ,

    vxx x vt t t

    c

    vxx x vt t t

    c

  • 12 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    We note that . Still This is because the rod is at rest in S. Measurement time has to be adjusted to be same in S not in S.

    2 1t t

    2 1x x L

  • 13 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    2 1 2 1( )x x x x

    LL

  • 14 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    A 1 m rod AB is kept stationary in S, with end A at origin, in x-y plane making an angle of 60o with x-axis. What would be its length in S, if the relative speed between S and S is 0.6 c? Also find the angle that rod makes with x-axis in S.

    Example 1

  • 15 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    O O

    z

    x

    y y

    z

    S S

    x A

    B

  • 16 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    Like before, we have to define events relating to measurement of ends of the rod. And these events have to occur at same time in S. Let the co-ordinates be: E1: (x1,y1,t) E2: (x2,y2,t)

  • 17 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    2 2

    2 2

    0.5 m

    3 m

    2

    x x vt

    y y

    We have to carry out Lorentz Transformation like before. However, the co-ordinates of the rod are known in S.

  • 18 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    1 1

    1 1

    0

    0

    x x vt

    y y

    Similarly

  • 19 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    Like before time for the two events would be different in S, but we have not specifically written it here, as this is not of much interest in the problem.

  • 20 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    We eventually get

    2 1

    2 1

    0.5

    3

    2

    x x

    y y

    With 21

    1.251 0.6

  • 21 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    The length of the rod in S is thus given as

    2 2

    2 1 2 1

    220.5 3

    1.25 2

    0.91 0.95 m

    x x y y

  • 22 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    The angle that the rod makes with x-axis in S is given by

    2 1

    2 1

    3 1.25tan 2.165

    2 0.5

    y y

    x x

    This gives o65.2

  • 23 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    We note that only the x-component of the rods length is contracted in S and not the y-component.

  • 24 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    According to an observer in S a lightening strikes at a distance of 20 km from origin at t=0. At what distance from origin, did this event occur in S, which moves with v=0.6 c in frame S?

    Example 2

  • 25 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    At t=0 and t=0 the origins of S and S were coincident. Imagine a stationary rod of 20 km extending from origin to place of lightening in S. The length of this rod would be contracted in S.

    Wrong Approach

  • 26 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    Now So the co-ordinate of lightening in S would be given by the contracted length 20/1.25=16 km.

    Wrong Answer

    1.25

  • 27 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    The co-ordinate of the event in S (x=20km, t=0).Hence using Lorentz transformation the x-coordinate in S is the following

    Correct Answer

    1.25 20 0

    25 km

    x

  • 28 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    Let us calculate the time of the event as seen in S.

    Why this discrepancy?

    3

    2

    5 8

    0.6 20 101.25 0

    5 10 s taking 3 10 m/s

    ct

    c

    c

  • 29 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    So According to S lightening had struck 5x10-5 s before the origins of the two frames coincided.

  • 30 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    In S frame the events of two origins coinciding, and lightening striking are not simultaneous, though in S they are.

  • 31 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    According to S, the origin of S is approaching him with a speed of 0.6c and only 5x10-5 s after the lightening striking, will the origin of S, reach his origin.

  • 32 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    Note when the observer in S gets the information of lightening is not important. What is important is the time when the lightening took place as per his calculation.

  • 33 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    Distance of origin of S from S in S frame, at the instant lightening strikes is

    55 10 0.6 9 kmc

  • 34 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    Assume that lightening struck at point P and a stationary rod OP of 20 km length is at rest in S. This length is proper. This length would appear to be contracted in S and would indeed be given by 16 km.

  • 35 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    But according to S, the lightening occurred before his origin coincided with S. Hence the co-ordinate of the event does not measure the length of the rod in his frame.

  • 36 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    P O,O

    20 km

    P O O

    16 km 9 km

    According to S at t=0

    When lightening strikes

    According to S at t= -5 10-5 s

  • 37 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    Time Dilation

    Proper Time interval between two events is time interval measured in a frame in which the two events occur at the same place.

  • 38 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    In another frame the time interval between these two events would appear to be larger than the proper time interval.

  • 39 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    Let the time interval be proper in S. Hence the two events should have the same x co-ordinates in S, say x. Let t1 and t2 be the time of the two events measured in S.

  • 40 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    2 2 2

    1 1 2

    vxt t

    c

    vxt t

    c

    The time of the two events in S is then given as follows.

  • 41 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    The time difference between these two events in S is therefore, given as follows.

    2 1 2 1 t t t t

    Proper time interval between two events normally is written as .

  • 42 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    We note that to apply time dilation, only the x co-ordinates of the two events have to be same. Though for general definition of proper time interval all the co-ordinates should be same. We shall discuss this aspect in detail later.

  • 43 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    Lorentz Transformation of x co-ordinate gives.

    2 2

    1 1

    x x vt

    x x vt

    Hence the x values are different in S. But that is not so shocking. A difference is expected classically also in similar situation.

  • 44 Prof. Shiva Prasad, Department of Physics, IIT Bombay

    We discussed two important consequences of Lorentz Transformation: Length Contraction and Time Dilation.

    We gave some examples of length contraction and warned where one can make an error in direct use of the formula.

    Summary