3.3.1 · D1Rocket Propulsion

Foundations — Tsiolkovsky rocket equation — full first-principles derivation from momentum

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This is the D1 Foundations page for the parent topic. Read it before the derivation. We assume you have seen nothing — not even the arrow on top of a vector. Every symbol used in the main note is built here, in an order where each one leans only on the ones before it.


0. What a symbol even is here

A symbol is a short name for a number that describes something physical. When we write , we mean "the amount of stuff in the rocket right now" — a single number, in kilograms. Nothing more mysterious than a label on a box. Our job below is to make sure every label is attached to a real picture before it appears in an equation.


1. Mass, — "how much stuff"

Picture a bathroom scale. The number it shows is (proportional to) . For a rocket, is the rocket's shell plus whatever fuel is still on board at this instant.


2. Velocity, — "how fast, and which way"

Figure — Tsiolkovsky rocket equation — full first-principles derivation from momentum

Look at the figure: the rocket moves right along one straight line. The amber arrow is . A longer arrow means faster; if the arrow flipped to point left, would be negative. Because everything happens along a single line, we can drop the arrow-on-top notation and treat as a plain signed number.


3. Change and the symbol (delta)

Picture two snapshots: before and after. If the rocket started at and ended at m/s, then m/s. Delta answers "how much did it move the needle?"


4. Momentum, — "throwing power"

Figure — Tsiolkovsky rocket equation — full first-principles derivation from momentum

In the figure, momentum is drawn as an arrow whose length is . Notice the two ways to get a long arrow: lots of mass (big block) or high speed (long velocity arrow). Momentum bundles both into one number.


5. Conservation of momentum — "the total never changes"

Figure — Tsiolkovsky rocket equation — full first-principles derivation from momentum

The figure shows the skateboarder-in-space idea. Before the throw, person + ball sit still: total . After the throw, the ball flies left with some negative momentum, so the person must fly right with equal positive momentum — the two arrows cancel to keep the total at . Nobody pushed on the outside; they only pushed on each other.


6. Newton's law in momentum form — "push changes momentum"


7. The relative exhaust velocity,

Figure — Tsiolkovsky rocket equation — full first-principles derivation from momentum

Two frames are drawn. Top: riding on the rocket, you always see gas leave your tail at the same speed — no matter how fast the whole rocket is going. Bottom: from the ground, the gas's speed is the rocket's speed minus , written , because the exhaust points backward.


8. The infinitesimal and the derivative

Think of a movie made of frames. is the gap between two neighbouring frames — almost zero. In that gap the mass changes by and the velocity by .


9. The natural logarithm,


10. Mass ratio,


Prerequisite map

Mass m

Momentum p = m v

Velocity v

Delta v

Conservation of momentum

Newtons law dp over dt

Exhaust velocity v_e

Rocket equation derivation

Infinitesimals and derivative

Natural log ln

Delta v = v_e ln of R

Mass ratio R

Read the map top-down: mass and velocity build momentum; momentum plus Newton's law give conservation; conservation plus the exhaust speed plus calculus produce the derivation; the derivation spits out a logarithm; the log plus the mass ratio give the final formula.


Equipment checklist

Test yourself — cover the right side and answer aloud before revealing.

What does stand for, and does it stay constant for a rocket?
The rocket's current mass in kg; it decreases as fuel burns.
What is velocity and how does its sign work here?
Speed with direction; positive = forward along the line, negative = backward.
What does mean?
The change in velocity, — the boost the engine delivers.
Write the definition of momentum .
(mass times velocity), unit kg·m/s.
State conservation of momentum in one sentence.
With no outside force, the total momentum of the system stays constant.
What does Newton's law in momentum form say, and what happens in free space?
; in free space so is constant.
Is measured from the ground or the rocket?
From the rocket — it is constant regardless of the rocket's ground speed.
What is the ground-frame velocity of the ejected gas?
.
What is the sign of and why?
Negative, because the rocket loses mass.
Why do we drop the term ?
It is a product of two infinitesimals — second order, negligibly small.
What question does answer?
" to what power equals ?"
Define the mass ratio .
, initial mass over final mass, always greater than 1.