Length contraction

Length contraction is the shortening of the length of an object moving relative to an observer, compared to its proper length, which is the length measured by an observer at rest relative to the object. Consider a moving train with a clock, which consists of a photon bouncing horizontally between two mirrors A and B (see diagram below).

For observer X, who is at rest on a platform and seeing the passing train, the total distance travelled by the photon from A to B in t_1 (indicated by the top purple arrow) is

ct_1=L+ut_1\; \; \; \; \; \; \; \; 250

where c is the speed of light, L is length of the clock according to X, and u is the speed of the train.

When the photon returns from B to A in t_2, A would have travelled a distance of ut_2. Thus, the distance travelled by the returning photon from B to A (indicated by the bottom purple arrow) is

ct_2=L-ut_2\; \; \; \; \; \; \; \; 251

The total time taken is t=t_1+t_2. Substituting eq250, where t_1=\frac{L}{c-u}, and eq251, where t_2=\frac{L}{c+u}, in t, yields

t=\frac{2L}{c}\frac{1}{1-\frac{u^{2}}{c^2}}\; \; \; \; \; \; \; \; 252

For observer Y, who is on the train, the total time t_0 (or proper time) measured by him is t_0=\frac{2L_0}{c}, where L_0 is called the proper length, which is the length measured by an observer who is at rest with respect to the object being measured. From eq249,

t=t_0\frac{1}{\sqrt{1-\frac{v^{2}}{c^{2}}}}=\frac{2L_0}{c}\frac{1}{\sqrt{1-\frac{v^{2}}{c^{2}}}}\; \; \; \; \; \; \; \; 253

Equating eq252 with eq253 gives

L=\frac{L_0}{\gamma}\; \; \; \; \; \; \; \; 254

where \gamma=\frac{1}{\sqrt{1-\frac{v^{2}}{c^{2}}}}.

To illustrate eq254, consider a person on Earth observing a spaceship moving from Earth to the Moon. The proper length between the Earth and the Moon is the length measured by an observer at rest with respect to the two (i.e., the Earth frame), while the proper length of the spaceship is the length measured by an astronaut on the spaceship. The astronaut measures the proper length of the spaceship, which remains the same regardless of the spaceship’s motion. However, due to length contraction, the observer on Earth sees the spaceship as contracted in the direction of its motion. Meanwhile, the astronaut, traveling on the spaceship, observes the distance between the Earth and the moon as contracted, since, from his perspective, the Earth and the moon are moving.

 

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