Comparing events between inertial frames
Key idea: Transform the same two events in the same order. Clock ticks share a position in their rest frame; a moving rod's endpoints must be recorded simultaneously in the measuring frame.
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Guided lessons · coming soon
Guided lesson
Guided steps
- Predict whether the flashes stay simultaneous in a moving frame.
- Read the difference form and keep one event order.
- Find the differences before and after relabelling.
- Read which difference each measurement sets to zero.
- Find Δt′ for events simultaneous in S.
- Choose the sign of Δt′, then calculate it.
- Follow how both measurement results come from the difference form.
- Use Δx′ = 0 to find Δt in S.
- Find the rod’s length using simultaneous endpoint measurements.
- Derive both results and compare the two measurement conditions.
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ContinueWhen a question compares two events, transform their differences, keeping the same event order in both frames. The main decision is usually which measurement condition is zero: simultaneous times, or co-located positions.
Check your understanding 1 Predict first
Two lamps 300 m apart flash at the same time in frame S. Are the flashes simultaneous in a frame S' moving along the line between them?
Show answer
Not simultaneous. With Δ t = 0 and Δ x ≠ 0, Δ t' = -γ vΔ x/c², which is not zero. Example B below finds its value.
Label the same two events
Call them event 1 and event 2, and define every difference as “2 minus 1”:
Use that order again for Δ x' and Δ t'. Subtracting the single-event Lorentz equations gives
The inverse equations are
Here S' moves at + v relative to S, with parallel axes and coincident origins at time zero. Reversing event order reverses all differences; changing frames does not change which events we compare.
Check your understanding 2 Why the “difference form” is so useful
In one inertial frame, two events have (x₁,t₁) = (40 m,2.0 s) and (x₂,t₂) = (100 m,5.0 s). The observer relabels the same records using x tilde = x-30 m and t tilde = t + 7.0 s. Find the event differences before and after relabelling. Would their Lorentz-transformed differences change at the same relative frame velocity?
Show answer
Originally Δ x = 100-40 = 60 m and Δ t = 5.0-2.0 = 3.0 s. The relabelled records are (10 m,9.0 s) and (70 m,12.0 s), so the differences remain 60 m and 3.0 s. Constant origin and clock offsets cancel. With the same relative velocity, the transformed differences are unchanged because the Lorentz difference equations use only these intervals.
Translate the measurement condition before substituting
| Situation | Zero condition | Consequence |
|---|---|---|
| Two events simultaneous in S | Δ t = 0 | Δ t' = -γ vΔ x/c², generally non-zero |
| Two ticks of one clock at rest in S' | Δ x' = 0 | Δ t = γΔ t'; Δ t' is proper time |
| Endpoints of a moving rod recorded together in S | Δ t = 0 | Δ x' = γΔ x; for a rod at rest in S', Δ x' = L₀ |
“Same position” and “same time” are different conditions. Identify the frame named by the question before setting either quantity to zero. Do not apply a time-dilation shortcut to an arbitrary spatially separated event pair.
Guided practice 1
Relativity of simultaneity via the difference form
Problem
Try this before viewing the solution
Show the steps Optional working
Hints
Hint 1
only the mixing term survives
Which term remains in the time transformation when the events are simultaneous in S?Show full solution
Calculate the factor
Method
Find γ for 0.80c.Reason
The transformation is relativistic.Working
Answer
γ = 1/(square root of (1-0.80²)) = 5/3Transform the interval
Method
Apply the simultaneous-in-S condition.Reason
Δ t = 0 removes the first term but not the spatial term.Working
Answer
Δ t' = -(5/3)(0.80c)(300)/c² ≈ -1.3 × 10⁻⁶ sInterpret
Method
The events are not simultaneous in S'.Reason
The negative sign means event 2 has the earlier S' time coordinate under the stated ordering.Working
Answer
t'₂ < t'₁
Quick check
Spot the mistake 2
Events simultaneous in S, not in S'
Learner claim
Try this before viewing the solution
Show the steps Optional working
Show solution step by step
Select the equation
Method
Use the Lorentz time-difference transformation.Reason
The question compares two spatially separated events across frames.Working
Answer
Δ t' = γ(Δ t-(vΔ x)/c²)Apply the condition
Method
Set Δ t = 0 and calculate γ = 1.25.Reason
Simultaneity is given only in S; the spatial term remains.Working
Answer
Δ t' = -γ(vΔ x)/c²Calculate and interpret
Method
The events are not simultaneous in S'; event 2 occurs earlier there.Reason
The transformed interval is negative under the stated ordering.Working
Answer
Δ t' = -1.25(0.60c)(240)/c² = -6.0 × 10⁻⁷ s
Common mistake
Derive the two measurement results
For the clock ticks, write Δ t' = Δτ. Their co-location in the clock rest frame gives
For the rod endpoint records, simultaneity belongs to the measuring frame S. The forward spatial difference gives L₀ = γ L, so
The two endpoint records generally have different S' times. The rod’s endpoints are stationary in S', so their coordinate separation is still L₀. Setting Δ t' = 0 instead would compare a different event pair and would not measure the rod’s moving length in S.
Exam-style question 1
Time dilation from the difference form
Examination question
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Show the steps Optional working
Show solution step by step
Identify the condition
1 markMethod
The events are co-located in S'.Reason
This is the proper-time frame condition.Working
Answer
Δ x' = 0Select and simplify
1 markMethod
Use the inverse time-difference transformation.Reason
The known interval is primed.Working
Answer
Δ t = γ(Δ t' + (vΔ x')/c²) = γΔ t'Calculate gamma
1 markMethod
Evaluate the Lorentz factor.Reason
v/c = 0.80.Working
Answer
γ = 1/(square root of (1-0.80²)) = 5/3Calculate the interval
1 markMethod
Multiply the proper time by γ.Reason
The interval in S is longer.Working
Answer
Δ t = (5/3)(4.0) ≈ 6.7 s
Self-mark with the mark scheme
Tick each mark point that your answer includes.
Mark your full written answer against these points.
Try it yourself 3
Length contraction from the difference form
Problem
Try this before viewing the solution
Show the steps Optional working
Hints
Hint 1
start from the spatial difference
Orient with Δ x' = γ(Δ x-vΔ t) and apply simultaneity in the measuring frame.Show solution step by step
Apply the measurement condition
Method
Set Δ t = 0 because the endpoints are recorded simultaneously in S.Reason
A moving length requires same-frame simultaneous endpoint positions.Working
Answer
Δ x' = γΔ xMap the lengths
Method
Identify Δ x' = L₀ and Δ x = L.Reason
The rod is at rest in S', so its primed length is proper.Working
Answer
L = L₀/γCalculate
Method
Use γ = 1.25 at 0.60c.Reason
The moving length must be smaller than the proper length.Working
Answer
L = 2.0/1.25 = 1.6 m
Quick check
Check your understanding 3
On paper, derive both results above from the Lorentz difference equations: the clock interval in S and the moving rod’s length. Show which difference is zero in each case.
Show answer
The clock ticks occur at one position in S', so Δ x' = 0. The inverse time equation gives Δ t = γ(Δ t' + vΔ x'/c²) = γΔ t'. At 0.80c, γ = 5/3 and Δ t = 6.7 s.
The moving rod’s endpoints are recorded simultaneously in S, so Δ t = 0. The forward spatial equation gives L₀ = Δ x' = γΔ x = γ L. At 0.60c, γ = 1.25 and L = 2.0/1.25 = 1.6 m.
Check the frame of each zero condition, the choice of forward or inverse equation, and the final units. The clock result multiplies by γ; the rod result divides by it.
Common mistakes
- Defining Δ x as “2 minus 1” but Δ t as “1 minus 2”, or changing the event order between frames.
- Assuming events simultaneous in one frame are simultaneous in another when they are separated in space.
- Setting Δ t' = 0 for a length measurement in S; the endpoints must be simultaneous in the measuring frame.
- Using the time-dilation shortcut for two events that are not at one place in either frame.
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Syllabus and review details
- GCE A-Level H3 Physics 2027 · 2027
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