Physic Labs

Theory of relativity

The twin paradox

Compare the two worldlines of a round trip and measure the elapsed times: Earth records Δt=2D/v\Delta t=2D/v while the traveler ages only Δτ=(2D/v)1−v2/c2\Delta\tau=(2D/v)\sqrt{1-v^2/c^2}, showing that the “paradox” is resolved by the change of inertial frame at turnaround.

Undergraduate

Equipment

  • 3D spacetime diagram with the twins' two worldlines
  • Slider “Tốc độ β = v/c” (speed)
  • Slider “Tham số mô hình” (model parameter, trip distance scale)
  • Quantitative γ(β) graph with marker; “Đặt lại góc nhìn” and “Tạm dừng” buttons

Procedure

  1. Read the two worldlines

    Inspect the spacetime diagram: the stay-at-home twin follows a straight worldline, while the traveler's worldline bends at the turnaround point. Elapsed aging is the proper time along each worldline, Δτ=∫1−v2/c2 dt\Delta\tau=\int\sqrt{1-v^2/c^2}\,dt, which is shorter for the bent path.

  2. Vary the speed β

    Drag the β slider from 0 toward 0.9 and read the elapsed times for both twins. The lower graph tracks γ=1/1−β2\gamma=1/\sqrt{1-\beta^2}; as β rises, the gap Δt−Δτ\Delta t-\Delta\tau grows, and it diverges as β→1\beta\to1.

  3. Check the round-trip numbers

    Pick β and read off the trip distance scale from the model slider. Compute Δt=2D/v\Delta t=2D/v and Δτ=Δt/γ\Delta\tau=\Delta t/\gamma by hand and compare with the readouts; then predict the age gap for a faster trip before moving the slider to confirm.

Simulation

Experiment history

Einstein's 1905 paper on special relativity already noted that clocks in relative motion cannot stay synchronized: a clock transported around a closed path returns behind one that stayed put. Paul Langevin popularized the striking traveler version in 1911, framing it as a genuine puzzle rather than a mathematical footnote. Hermann Minkowski's 1908 spacetime picture gave the clean resolution: each twin ages by the proper time along his worldline, and the traveler's bent worldline simply has less proper time. The effect is not hypothetical — atomic clocks flown around the world in the Hafele–Keating experiment (1971) and daily corrections in GPS satellites confirm the predicted gains and losses of time.

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