The Velocity Addition Formula
Velocity Addition Formula
Updated: May 10, 2026
On the Electrodynamics of Moving Bodies
Einstein-EDoMB-1905-Section §5
https://www.fourmilab.ch/etexts/einstein/specrel/www/
Einstein: Relativity, The Special and the General Theory, 1920, Chapter VI page 19, Chapter XIII page 45
https://www.google.com/books/edition/Relativity/n8QKAAAAIAAJ?hl=en&gbpv=1
Both sources show the velocity-addition-formula as it is today.
Shown: V = ( v + w ) / ( 1 + vw/c² )
#### Abbreviations and notation
SRT = spezielle Relativitätstheorie, Special Relativity
rf = reduction factor ( denominator ) in the v-a-f.
Let’s change a notation without changing anything on the ground. Bring in an asterisk* for relativistic output velocity-V* of addition or subtraction.
Classical addition or subtraction: V ← ( v ± w )
SRT addition or subtraction: V* ← ( v ± w ) / ( 1 ± vw/c² )
As in most of SRT, we use left ← to ← right equation logic ( an assignment operator so-called ) rather than high school left = to = right, an identity.
5 ← 2 + 3
2 + 3 = 5
In subtraction and addition set-ups that follow, speed-w is the special case of speed-c, the speed-of-light. That simplifies the denominator reduction factor to:
rf = ( 1 ± v/c )
The sun out there in free-space fires off a photon:
Alter! When the Hills do —
Falter! When the Sun
Question if His Glory
Be the Perfect One —
#### Lorentz Transforms
Lorentz Transforms: minus-sign, shown in EDoMB-1905 Section §3 and used in Section §4 ( length contraction and time dilation. ) Shown in Halliday & Resnick as equations 37-2I:
x′ = gamma • ( x – vt )
t′ = gamma • ( t – vx / c² )
Lorentz Transforms: plus-sign, shown in H&R as equations 37-22.
x = gamma • ( x′ + vt′ )
t = gamma • ( t′ + vx′ / c² )
This plus-sign pair is shown neither in Section §5 ( v-a-f ) nor in 1920-Chapter XIII ( v-a-f ):
#### Derive the v-a-f Section §5
Section §5 has a statement which invokes the minus-sign pair of Section §3. Quote: “With the help of Section §3 equations we solve for x and t.” The statement does not lead to a display of the plus-sign pair. A single additive-spatial is shown. It is not an LT. Gamma is missing:
x = ( w′ + v ) • t / rf
It is this equations which leads to the v-a-f:
Shown: V* = ( v + w ) / ( 1 + vw/c² )
#### Derive the v-a-f H&R Chapter 37
H&R Chapter 37-3 has a similar statement: Quote: “Simply solve equations 37-21 for x.” The plus-sign pair is then shown but the algebra of “solve for” is not shown. Chapter 37-4 then has derivation of the v-a-f from the plus-sign pair shown as Equation 37-29.
The general idea is simple. Speed is distance divided by time. The plus-sign LT pair with speed-w:
x = gamma • ( wt′ + vt′ )
t = gamma • ( t′ + vwt′ / c² )
V* = x / t
Gamma divides out. Time-t′ divides out.
V* = ( v + w ) / ( 1 + vw/c² )
Special case: w = c
V* = ( v + c ) / ( 1 + vc/c² )
V* = ( v + c ) / ( 1 + v/c )
V* = c
#### Solve for gold
x′ = x – vt
paper money ← gold standard minus gold standard
x = vt + x′
gold standard ← gold standard plus paper money
Is it really the gold standard or have we been defrauded?
Footnote: Comment-1 on the blog has a version of “solve for x” taken off a web page. The algebra seems to have a blatant falsehood.
False: vt′ = vt
#### Subtract
Let’s do a velocity formula based on the minus-sign spatial of Section §3:
x′ = gamma • ( x – vt )
Point-x is a point of speed-v like point-vt, although not shown as such. Let it have speed-w. Rewrite: x = wt.
x′ = gamma • ( wt – vt )
We still have a distance equation, not a speed equation. Get rid of gamma and we move over to a distance of classical mechanics.
x′ = wt – vt
What’s up? The right-hand-side is subtraction of changing distances on essential axis-X, unprimed, subtraction of changing locations. Both distances are with respect to axis-zero. Output-x′ on the left-hand-side is not a location, is not a distance with respect to axis-zero. It is a segment on axis-X, changing in both location and size. Use of primed notation is statement of that fact. Here in Galilean mode, we don’t really have a new primed axis, “two systems of co-ordinates” as they say.
The two distances ( locations ) wt and vt are what you might call parallel distances, not a “composition” of distances wherein distance-wt is with respect to location-vt.
x′ = ( w – v ) • t
Divide by t:
x′ / t = w – v
We now have explicitly a speed equation. Let’s say speed-w is faster than speed-v. The point-wt is out in front of point-vt, but that’s because it is going faster, not because it is a serial speed, aka serial resister-w attached to resister-v. Output speed x′ / t is speed of separation, not ordinary axis speed with respect to the starting line.
Let speed-w be speed-c, the speed-of-light:
x′ = ct – vt
x′ = ( c – v ) • t
x′ / t = c – v
Speed of separation of points ct and vt is speed x′ / t. It is a good algebraic value. Point-ct gets out in front of point-vt at speed-( c – v ). But point-vt cannot view point-ct as moving ahead at speed-( c – v ). Too slow. Point-ct is a photon and a photon has speed-c regardless of who is looking at it. Point-vt must view point-ct as moving ahead at speed-c.
Point-vt views point-ct as point-x′. From that stance, the speed of point-x′ is speed judged by a clock moving at speed-v. The clock is adjusted by the factor: ( c – v ) / c < 1, less than 1. Less time for a projectile doing length-x′ is higher speed. The adjustment factor allows point-vt to have for itself a photon on distance-x′ at speed-c. Counter-intuitive because the clock announcing speed-v of point-vt is stationary on the pavement. It is not adjusted.
x′ = ( c – v ) • t
t′ = [ ( c – v ) / c ] • t
Divide distance by time to obtain speed:
V* = x′ / t′
V* = ( c – v ) • t / [ ( c – v ) / c ] • t
The velocity subtraction formula, v-s-f:
V* = ( c – v ) / ( 1 – v/c )
V* = c
#### Three distance additions
The plus-sign spatial of H&R 37-22, without gamma:
++ add: x = x′ + vt′
Introductory spatial of Section §5, without reduction factor:
++ add: x = ( w′ + v ) • t
Solve for x:
++ add: x = x′ + vt
Three equations. Which is it ? Heaven only knows !
https://groups.google.com/g/alt.arts.poetry.comments/c/R5Aif2cXSdE
#### Critical
Actually those three distance sums have something in common: all three are the sum of two serial distances not two parallel distances. Evidently the “composition of velocities” must begin with composition of distances.
1920 Chapter VI, which lays out a “carriage and embankment,” makes roughly the same statement.
Let’s not observe subtraction or addition of distances. Let’s observe subtraction and addition of speeds.
Subtraction: A photon viewed by point-vt does distance-x′ and goes too slowly. A clock associated with point-vt ( stationary with respect to point-vt but moving at speed-v on the pavement ) is adjusted, thereby restoring the photon to speed-c on distance-x′. Adjustment of this moving clock has no effect on two stationary clocks: the clock at pavement point-x doing speed-c in x = ct, and the pavement clock momentarily associated with point-vt, doing speed-v.
Addition: A photon is going to fast because it is doing the sum of two distances: distance-ct when w = c, and distance-vt. If you speed up pavement clock ( on axis-X ) at location x = ct + vt, you slow down something which has gone that distance in time-t. More time slower speed.
Critical: Doctoring up the clock at pavement location x = ( c + v ) • t can slow down the speed of point-x from c + v to c. But changing that pavement clock requires changing all pavement clocks, including the clock doing point-vt, in which case value-vt is no good.
Subtraction requires transformation of only one clock: clock c – v. Addition requires transformation of two clocks: clock c + v and clock v. A monumental crisis of institutions.
Blog comment #### Solve for x
ReplyDeletehttps://www.eftaylor.com/spacetimephysics/04a_special_topic.pdf
Equations L-10 and L-11
H&R Chapter 37-3 says you can switch over from the subtractive LT’s ( Eqs 37-21 ) to the additives ( Eqs 37-22 ) with some algebra. Quote: “Simply solve Eqs 37-21 for x and t.”
1905-Section §5 has similar verbiage, quote: “With the help of Section §3 equations [ subtractive ] we solve for x and t.”
The subtractive Lorentz Transforms, Eqs 37-21:
Spatial: x′ = gamma • ( x – vt )
Temporal: t′ = gamma • ( t – vx / c² )
Solve for x. Not shown in H&R. See EF Taylor:
Quote: “Multiply both sides of the temporal by v:”
vt′ = gamma • ( vt – v²x / c² )
Add temporal to the spatial:
x′ + vt′ = gamma • ( x – vt + vt – v²x / c² )
Term vt “cancels” out.
x′ + vt′ = gamma • ( x – v²x / c² )
x′ + vt′ = gamma • x • ( 1 – v²/c² )
x′ + vt′ = gamma • x / gamma²
x′ + vt′ = x / gamma
x = gamma • ( x′ + vt′ )
Classical Galilean:
Spatial: x′ = x – vt
Solve the spatial for x:
x = x′ + vt
Use the previous equation vt′ = vt:
x = x′ + vt′
In Galilean mode you can write vt′ = vt because t′ = t. In SRT mode t′ ≠ t.
False: vt′ = vt
False: x = x′ + vt′
SPAM RISK.