3.4.5 · D1Rocket Flight Mechanics

Foundations — 6DOF equations — translational (Newton), rotational (Euler's equations)

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Before you can read the parent note, you need to own every symbol it throws at you. This page builds each one from nothing — plain words, a picture, and the reason the topic can't live without it. Read top to bottom; each block leans on the one above it.


0. What is a "rigid body"?

Why the topic needs it: the clean split into "point moves" + "body twists" is a theorem that only holds for rigid bodies. A noodle would need infinitely many numbers.


1. Vectors and the arrow picture

Figure — 6DOF equations — translational (Newton), rotational (Euler's equations)

A vector in 3D is really three numbers stacked — one for each axis. Look at the figure: the arrow casts a shadow onto each axis, and those three shadow-lengths are its components. Writing just means "walk along , then along , then along , and you land at the arrow tip."

Why the topic needs it: every quantity in 6DOF (force, velocity, spin) is a vector, and the transport theorem is derived by asking how the basis vectors themselves move when the rocket turns.


2. Rate of change: the dot and

Why the topic needs it: Newton's law and Euler's law are both statements about a rate of change — momentum's rate equals the push. Without the dot there is no law.


3. Velocity and angular velocity

Figure — 6DOF equations — translational (Newton), rotational (Euler's equations)

Why the topic needs it: is the star of Newton's equation, the star of Euler's. Both equations carry a "" term, so you must first know what is.


4. The cross product

Figure — 6DOF equations — translational (Newton), rotational (Euler's equations)

Look at the figure: a point at position on a body spinning at swings along the green arrow — tangent to its circle, at right angles to both the axis and the radius.

Why the topic needs it: the whole reason the body-frame equations differ from the ground-frame ones is this term. It is the transport theorem's punchline.


5. Two frames: inertial and body

Why the topic needs it: this is the central tension the parent note resolves. Measure in , but the law lives in — the transport theorem is the bridge. See Reference frames and rotation matrices and Transport theorem (rotating frames) to go deeper.


6. Mass , momentum , and force

Why the topic needs it: these three are the entire cast of the translational equation.


7. Inertia tensor and angular momentum

Why the topic needs it: is Euler's equation. Every symbol in it — , , , , the cross product, the two frames — you now own.


8. How it all feeds the topic

Rigid body

Vectors and components

Rate of change d/dt

Angular velocity omega

Cross product omega cross A

Two frames I and B

Transport theorem

Momentum p equals m v

Inertia tensor and H

Translational Newton eqn

Rotational Euler eqn

6DOF equations

Everything funnels into the transport theorem, which then produces both the Newton and Euler equations of the parent note the 6DOF topic.


Equipment checklist

Draw a 3D vector and label its three components.
An arrow whose shadows on the axes are , so .
What does the dot in mean, and what two things can make it nonzero?
One time-derivative; nonzero if the vector's length changes OR its direction swings (basis rotates).
Name and .
Body-frame velocity components (forward, side, up) and angular-velocity components (roll , pitch , yaw ).
What does physically give, and when is it zero?
The sideways velocity a point at gets from spinning; zero when is parallel to the axis .
Why do we need both an inertial frame and a body frame ?
Newton/Euler laws are only valid in , but measurements are easiest in ; the transport theorem bridges the two.
Why is inertia a tensor instead of a single number like mass?
A body resists twisting differently about different axes, so one number can't capture it — you need a table.
Write the rotational analog of .
with — torque equals rate of change of angular momentum.