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Lorentz Transformations

The Lorentz transformations replace the Galilean transformations of Newtonian mechanics. They mix space and time coordinates between inertial frames and reduce to the Galilean transform in the limit $v\ll c$. Any physical law that is Lorentz-covariant automatically satisfies the postulates of special relativity.

Key Concepts

Lorentz Boost
For frame Sβ€²S' moving at velocity vv in the xx-direction relative to SS: tβ€²=Ξ³(tβˆ’vx/c2)t'=\gamma(t-vx/c^2), xβ€²=Ξ³(xβˆ’vt)x'=\gamma(x-vt), yβ€²=yy'=y, zβ€²=zz'=z. The inverse replaces vβ†’βˆ’vv\to-v.
Lorentz Factor
Ξ³=1/1βˆ’Ξ²2\gamma=1/\sqrt{1-\beta^2} where Ξ²=v/c\beta=v/c. At low speeds Ξ³β†’1\gamma\to1. At v=0.866cv=0.866c, Ξ³=2\gamma=2. As vβ†’cv\to c, Ξ³β†’βˆž\gamma\to\infty.
Simultaneity Shift
The time difference between two spatially separated events in Sβ€²S' is Ξ”tβ€²=Ξ³(Ξ”tβˆ’vΞ”x/c2)\Delta t'=\gamma(\Delta t-v\Delta x/c^2). Even if Ξ”t=0\Delta t=0 (simultaneous in SS), Ξ”tβ€²β‰ 0\Delta t'\ne0 unless Ξ”x=0\Delta x=0.
Group Structure
Successive Lorentz boosts compose as: Ξ²total=(Ξ²1+Ξ²2)/(1+Ξ²1Ξ²2)\beta_{\rm total}=(\beta_1+\beta_2)/(1+\beta_1\beta_2). The Lorentz group O(3,1)O(3,1) is the symmetry group of Minkowski spacetime.

Key Equations

Lorentz boost (x-direction)
tβ€²=Ξ³(tβˆ’vxc2),xβ€²=Ξ³(xβˆ’vt)t' = \gamma\left(t - \frac{vx}{c^2}\right), \quad x' = \gamma(x - vt)
S' moves at v relative to S along x. Inverse: replace v β†’ -v.
Lorentz factor
Ξ³=11βˆ’v2/c2=11βˆ’Ξ²2\gamma = \frac{1}{\sqrt{1-v^2/c^2}} = \frac{1}{\sqrt{1-\beta^2}}
Always β‰₯ 1; diverges as v β†’ c.
Velocity addition
uβ€²=uβˆ’v1βˆ’uv/c2u' = \frac{u - v}{1 - uv/c^2}
Speed of object moving at u in S, as measured in S' (moving at v relative to S).
Worked Example

Transforming Coordinates Between Frames

Problem

Frame Sβ€²S' moves at v=0.60cv=0.60c relative to SS. An event occurs at t=5.0t=5.0 ns, x=3.0x=3.0 m in SS. Find tβ€²t' and xβ€²x'. (c=3Γ—108c=3\times10^8 m/s.)

Solution

Ξ³=1/1βˆ’0.36=1.25\gamma=1/\sqrt{1-0.36}=1.25. Note: vt=0.60Γ—3Γ—108Γ—5Γ—10βˆ’9=0.90vt=0.60\times3\times10^8\times5\times10^{-9}=0.90 m.

xβ€²=Ξ³(xβˆ’vt)=1.25(3.0βˆ’0.90)=1.25Γ—2.10=2.625Β mx' = \gamma(x-vt) = 1.25(3.0 - 0.90) = 1.25\times2.10 = 2.625\text{ m}

vx/c2=0.60Γ—3Γ—108Γ—3.0/(9Γ—1016)=0.60Γ—10βˆ’7/108Γ—3=6Γ—10βˆ’9vx/c^2 = 0.60\times3\times10^8\times3.0/(9\times10^{16})=0.60\times10^{-7}/10^8\times3=6\times10^{-9} s =6.0=6.0 ns.

tβ€²=Ξ³(tβˆ’vx/c2)=1.25(5.0βˆ’6.0)Β ns=1.25Γ—(βˆ’1.0)=βˆ’1.25Β nst' = \gamma(t - vx/c^2) = 1.25(5.0 - 6.0)\text{ ns} = 1.25\times(-1.0) = -1.25\text{ ns}
Answer xβ€²=2.63x'=2.63 m, tβ€²=βˆ’1.25t'=-1.25 ns.
Practice

Exercises

7 problems
1 of 7

Find the Lorentz factor Ξ³\gamma for Ξ²=v/c=0.80\beta=v/c=0.80.

(dimensionless)
2 of 7

Find Ξ³\gamma for v=0.990cv=0.990c.

(dimensionless)
3 of 7

Frame Sβ€²S' moves at v=0.60cv=0.60c (Ξ³=1.25\gamma=1.25). An event at x=600x=600 m, t=0t=0 in SS. Find xβ€²x' (in m).

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4 of 7

Same frame (v=0.60cv=0.60c, Ξ³=1.25\gamma=1.25). Event at x=600x=600 m, t=0t=0. Find tβ€²t' (in ns, use c=3Γ—108c=3\times10^8 m/s).

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5 of 7

Two spaceships travel in opposite directions relative to Earth. Ship A moves at Ξ²A=0.60\beta_A=0.60 and ship B at Ξ²B=0.60\beta_B=0.60 (in the opposite direction, so Ξ²B=βˆ’0.60\beta_B=-0.60 relative to Earth). Find ship B's speed as seen from ship A using velocity addition: uβ€²=(uβˆ’v)/(1βˆ’uv/c2)u'=(u-v)/(1-uv/c^2) with u=βˆ’0.60cu=-0.60c and v=0.60cv=0.60c. Express as ∣uβ€²βˆ£/c|u'|/c.

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6 of 7

A rocket travels at Ξ²=0.995\beta=0.995 relative to Earth (Ξ³β‰ˆ10\gamma\approx10). A photon is fired forward. Find its speed in the rocket frame (in units of c).

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7 of 7

A rocket (Ξ²=0.80\beta=0.80, Ξ³=1.667\gamma=1.667) emits a signal at xβ€²=0x'=0, tβ€²=0t'=0 in its frame. Find the xx coordinate in the lab frame using the inverse transform x=Ξ³(xβ€²+vtβ€²)x=\gamma(x'+vt') (in m if tβ€²=0t'=0).

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Key Takeaways

  • Lorentz boosts mix tt and xx: tβ€²=Ξ³(tβˆ’vx/c2)t'=\gamma(t-vx/c^2), xβ€²=Ξ³(xβˆ’vt)x'=\gamma(x-vt).
  • Ξ³=1/1βˆ’Ξ²2\gamma=1/\sqrt{1-\beta^2} is always β‰₯1\ge1 and grows without bound as Ξ²β†’1\beta\to1.
  • Velocity addition uβ€²=(uβˆ’v)/(1βˆ’uv/c2)u'=(u-v)/(1-uv/c^2) always gives ∣uβ€²βˆ£β‰€c|u'|\le c β€” the speed limit is self-consistently maintained.
  • The Lorentz group is a 6-parameter group (3 boosts + 3 rotations) acting on Minkowski spacetime.