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Planet Earth Einstein’s Theory of Special Relativity.

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Presentation on theme: "Planet Earth Einstein’s Theory of Special Relativity."— Presentation transcript:

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2 Planet Earth Einstein’s Theory of Special Relativity

3 Classical Physics Review Length and Time –Define a standard for each and compare the unknowns to them. Kinematics –derive from length and time velocity and acceleration –v =  x/  t –a =  v/  t If a is constant –v = at and x = 1/2 a t 2 –as t goes to infinity v goes to infinity

4 Dynamics Newton’s Laws (existence and strength of all forces –Law of inertia –F = ma –Law of mutual interaction Conservation laws –Momentum –Energy Electricity and Magnetism –Maxwell’s equations for the dynamics of charged particles

5 Implicit Assumption All the laws of nature have the same form in all frames of reference moving at constant velocity with respect to each other. Transformation Laws between frames. S S’ vt x X’X’ X ’ = x - vt and V’ = V - v

6 Trouble All observers can use the same laws, and communicate! Michelson-Morley Experiment –to study the nature of light - particle or wave –if it is a wave - what is the nature of the medium? –search for the ether –the experiment was null

7 Einstein’s Postulates All the laws of nature have the same form in all frames of reference moving at constant velocity with respect to each other. The speed of light is a constant for all observers moving at constant velocity with respect to each other.

8 New Transformation Equations  t =  t 0 / (1 - v 2 /c 2 ) 1/2  x =  x 0  (1 - v 2 /c 2 ) 1/2 m = m 0 / (1 - v 2 /c 2 ) 1/2 V’ x = (V x - v) / (1 - V x  v/c 2 )

9 Time dilation  t =  t 0 / (1 - v 2 /c 2 ) 1/2 A space ship goes by at v =.8c. Someone on the ship drops a ball 16 ft. and measures a time of flight of 1 sec (  t 0 ). What does a stationary observer measure (  t )?  t =  t 0 / (1 - v 2 /c 2 ) 1/2 = 1/(1 -.64) 1/2 = 1.67 sec. 16 ft.

10 Length Contraction  x =  x 0  (1 - v 2 /c 2 ) 1/2 If the ball on the spaceship has a diameter of 5 cm (  x 0 ) as measured by someone on the ship. What is its diameter as measured by a stationary observer (  x )?  x =  x 0  (1 - v 2 /c 2 ) 1/2 = 5  (1 -.64) 1/2 = 5 .6 = 3cm 16 ft.

11 Mass Increase m = m 0 /(1 - v 2 /c 2 ) 1/2 Same ball has a mass of 10 gm as measured by someone on the ship( m 0 ). What is the mass as measured by the stationary observer (m)? m = m 0 /(1 - v 2 /c 2 ) 1/2 = 10/(1 -.64) 1/2 = 10/.6 = 16.7 gm 16 ft.

12 Addition of velocity V’ x = (V x - v) / (1 - V x  v/c 2 ) A space ship goes by at.8c (v) and watches someone on earth turn on a flashlight. What is the speed of the light as measured by the observer on the ship? Note the result is independent of v! V’ x = (V x - v) / (1 - V x  v/c 2 ) = ( c -.8c)/(1 - c .8c/c 2 ) = c SS’ V =.8c

13 Compare fictitious space ship speed with actual escape speed Fictitious speed of.8 c gives the results on the previous slides. Actual escape speed is about 7 mi/sec. The speed of light is 186,000 mi/sec. The escape speed can be written as.00004c try to redo the previous slides with this speed instead of.8c! For everyday experience v/c is very small and Einstein’s equations reduce to the ones on slide 4

14 Implications of variable mass The faster an object moves the harder it is to move it any faster. Kinetic energy is not the total energy of a moving object –E = KE + m 0  c 2 = m  c 2 –Rest energy exist. A particle has energy by virtue of its existence. We have already discussed many applications of this fact!

15 Suppose the ultimate speed was 100 miles/hour What would the three equations predict for a speed of 80 miles/hour or.8c? The same as already predicted but you would see it!

16 Trends Graph of ratios of masses times and lengths


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