Special Relativity - Angle Transformations

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SUMMARY

The discussion focuses on the application of special relativity to determine the length contraction and angle transformation of a moving rod. The length of the rod as perceived by a stationary observer is calculated using the formula L = L_0√(1 - (v²/c²)cos²θ_0). Additionally, the angle transformation is derived as tanθ = γtanθ_0, where γ = 1/√(1 - (v²/c²)). The participants emphasize the importance of correctly applying trigonometric identities and algebraic manipulation to arrive at the required expressions.

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  • Understanding of special relativity concepts, particularly length contraction and Lorentz transformations.
  • Familiarity with trigonometric identities and their applications in physics.
  • Knowledge of the Lorentz factor, γ, and its derivation.
  • Basic algebra skills for manipulating equations and simplifying expressions.
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Rubber Ducky
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Homework Statement



A rod of length L_0 moves with a speed v along the horizontal direction. The rod makes an angle of θ_0 with respect to the x'-axis.

(a) Show that the length of the rod as measured by a stationary observer is given by

L=L_0\sqrt{1-\frac{v^2}{c^2}cos^2θ_0}


(b) Show that the angle that the rod makes with the x-axis is given by the expression
tanθ=γtanθ_0

(Take the lower end of the rod to be at the origin of the primed coordinate system.)

Homework Equations



γ=\frac{1}{\sqrt{1-\frac{v^2}{c^2}}}

L=\frac{L_0}{γ}

{L_0}^2=(x')^2+(y')^2 and L^2=x^2+y^2

The Attempt at a Solution



Let x and y be the rod's length and height (picture the rod forming the hypotenuse of a right triangle):

x'=L_0cosθ_0

There is no movement in the y (or y') direction, so y'=y=L_0sinθ_0

Meanwhile, the x component will contract in the non-prime reference frame, so x=\frac{x'}{γ}=\frac{L_0cosθ_0}{γ}

Thus L^2=x^2+y^2=\frac{L_0^2cos^2θ_0}{γ^2}+L_0^2sin^2θ_0

The algebra gets messy at this point, and I'm not sure what methods I should be using to yield the required form. I looked at my trig identities but none really seemed to fit the situation. And hopefully I haven't made a silly error in the physics side of things!
 
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Rubber Ducky said:
Thus L^2=x^2+y^2=\frac{L_0^2cos^2θ_0}{γ^2}+L_0^2sin^2θ_0

The algebra gets messy at this point, and I'm not sure what methods I should be using to yield the required form.

Write out the γ2 factor in terms of v/c and simplify. It's not too bad.
 

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