University Physics III: Waves, Optics & Modern · Problem type

Relativistic velocity addition

Use this for “A ship moving at 0.7c fires a probe forward at 0.5c relative to the ship. How fast does the probe move as seen from the planet?”

Diagram

light: x = ctS′: v = 0.6object: u′ = 0.6 in S′, u = 0.882353 in Sadding them: v + u′ = 1.2 cxctct′x′
u
=
v + u′
1 + vu′
=
0.6 + 0.6
1 + 0.6 × 0.6
=
1.2
1.36
u = 0.8824c
Adding the speeds, v + u′ = 1.2c, would beat light (dashed); the true world line stays inside the light line.
This is an example. Type your own values to start a new problem.
u
c
=
c
+
c
1
+
×
uG
Sum without relativity, in c
worked out (not typed)

Formulas

u
=
v
+
u
′
1 +
v
×
u
′
0.882353
=
0.6 + 0.6
1 + 0.6 × 0.6
uG
=
v
+
u
′
1.2 = 0.6 + 0.6

Assumptions

•
Frame S′ moves at v along +x past frame S; the object moves along the same line at u′ in S′ and at u in S.
•
Every speed is in units of c, so u = (v + u′) ÷ (1 + vu′ ÷ c²) reads u = (v + u′) ÷ (1 + vu′); a minus sign means toward −x.
•
When v and u′ are small the bottom is near 1 and u ≈ v + u′, the Galilean sum; below c plus below c always stays below c.

Step-by-step

WE KNOW
v = 0.6, u′ = 0.6
FIND
object’s speed in S, in c (u), sum without relativity, in c (uG)
Step 1 · Find object’s speed in S, in c (u)
Use u = (v + u′) ÷ (1 + v × u′)
Add
the
speeds,
then
divide
by
1
+
vu′:
the
bottom
grows
with
both
speeds
and
keeps
u
below
c.
u
=
0.6 + 0.6
1 + 0.6 × 0.6
u
=
1.2
1 + 0.36
u
=
1.2
1.36
u
=
0.882353
Step 2 · Find sum without relativity, in c (uG)
Use uG = v + u′
What everyday speeds would give: the plain sum, which can pass c.
uG = 0.6 + 0.6
uG = 1.2
Check
Put the numbers back in. Both sides should match.
0.882353
=
0.6 + 0.6
1 + 0.6 × 0.6
✓
1.2 = 0.6 + 0.6 ✓
Topic check
See what you know: 5 questions on this topic
New questions each time. Pass to mark it complete.

Related lessons

© 2026 SME. All rights reserved.