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8 - N u m e r i c a l   1

Problem

The length of a spaceship is measured to be exactly one-third of its proper length. What is the speed of the spaceship relative to the observer?


Data

  • Proper length of the spaceship (LpL_p) = reference length
  • Measured length (LL) = 13Lp\frac{1}{3} L_p
  • Speed of light (cc) = constant

To Find: Speed of the spaceship relative to the observer (vv).


Prerequisite Concepts

Relativistic length contraction is given by:

L=Lp1โˆ’v2c2,L = L_p \sqrt{1 - \frac{v^2}{c^2}},

where:

  • LL is the contracted length observed,
  • LpL_p is the proper length,
  • vv is the speed of the moving object,
  • cc is the speed of light.

Rearranging:

1โˆ’v2c2=LLp.\sqrt{1 - \frac{v^2}{c^2}} = \frac{L}{L_p}.

Solution

  1. From the given data:
L=13Lp. L = \frac{1}{3} L_p.

Substituting into the contraction equation:

1โˆ’v2c2=LLp=13. \sqrt{1 - \frac{v^2}{c^2}} = \frac{L}{L_p} = \frac{1}{3}.
  1. Squaring both sides:
1โˆ’v2c2=(13)2, 1 - \frac{v^2}{c^2} = \left(\frac{1}{3}\right)^2, 1โˆ’v2c2=19. 1 - \frac{v^2}{c^2} = \frac{1}{9}.
  1. Rearranging:
v2c2=1โˆ’19. \frac{v^2}{c^2} = 1 - \frac{1}{9}.

Simplify:

v2c2=99โˆ’19=89. \frac{v^2}{c^2} = \frac{9}{9} - \frac{1}{9} = \frac{8}{9}.
  1. Solving for vv:
v2=89c2. v^2 = \frac{8}{9} c^2. v=89c. v = \sqrt{\frac{8}{9}} c.
  1. Simplifying:
v=83c. v = \frac{\sqrt{8}}{3} c.

Approximation:

vโ‰ˆ0.9428c. v \approx 0.9428 c.

Answer

The speed of the spaceship relative to the observer is approximately v=0.9428cv = 0.9428c.