1.2.10 · D1Newton's Laws & Dynamics

Foundations — Atwood machine — derivation

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Before you can read the derivation, you need to own every symbol it uses. This page builds each one from a picture, in the order they depend on each other. Nothing here assumes you have seen the parent derivation yet.


0. The scene we are describing

Let's first fix the physical picture so every later symbol has a home. In the figure below, notice the labels: the wheel is the pulley, the cord is the string, and there are two blocks hanging from the two ends. The small arrows show the directions of motion when the left block is the heavier one. (We give the blocks their symbols and in Section 1, right after we define what "mass" means.)

Figure — Atwood machine — derivation

Everything below is just a careful naming of the things in that one picture.


1. Mass — the symbol


2. Gravity's pull — and the weight

Why do the blocks move at all? Because the Earth pulls them down. We need a number for "how strongly."

Figure — Atwood machine — derivation

3. Speed, velocity, and acceleration — the symbol

Before we can talk about "positive directions," we need the quantity that has a direction and that we ultimately solve for. It is built from one earlier word: velocity.


4. Force and the arrow picture

Because forces have direction, we must decide which direction counts as positive before adding them. That single choice is where most beginners slip — so let's make it a picture too.

Figure — Atwood machine — derivation

5. Tension — the symbol

The string pulls. That pull has its own name.


6. The two magic string-properties

Two idealised words in the definition do enormous work. Let's earn them.

Figure — Atwood machine — derivation

7. Newton's Second Law and the free body diagram

Everything above pours into a single law.

To apply it we draw a free body diagram: isolate one block, draw only the arrows touching it (gravity down, tension up), then add them into . The figure below shows exactly that for both blocks.

Figure — Atwood machine — derivation
Recall Free body diagram, in one line

Question: what two forces act on each hanging block? ::: gravity downward and tension upward — nothing else. See Free Body Diagrams.


8. Both edge cases — equal masses, and the heavier block on either side


9. The harmonic-mean shape (a preview)

The tension answer will turn out to look like . You don't need to derive it here — just recognise the shape, and notice the : tension is a force (newtons), so it must carry a , exactly like a weight does.


How these foundations feed the topic

Read this map top-to-bottom: the plain-language boxes at the top are the building blocks; the arrows show which idea feeds into the next; everything funnels into the final Atwood derivation at the bottom.

Mass of each block

Weight equals mass times g

Gravity strength g

Newtons Second Law net force equals mass times acceleration

Acceleration a

Tension in the string

Sign convention plus and minus

Free body diagram

Inextensible string

Equal acceleration for both blocks

Massless frictionless pulley

Atwood derivation solve for a and T

Harmonic mean shape


Equipment checklist

Cover the right side and test yourself. If any answer surprises you, re-read that section before the derivation.

What does measure, and in what unit?
Amount of stuff (inertia), in kilograms.
What is in plain words?
How much downward speed (m/s) gravity adds each second; .
Write the weight of a block of mass .
(a force, in newtons, pointing down).
What is the difference between speed and velocity?
Speed is how fast; velocity is how fast plus the direction.
What does the symbol stand for?
Acceleration — how quickly velocity changes, in .
What does mean?
The single leftover force after adding all force arrows on a body (with signs).
What can a string (rope) do — push, pull, or both?
Only pull; tension points from the block toward the pulley.
Do "string" and "rope" mean different things here?
No — they are the same idealised inextensible, massless cord.
Why is tension the same throughout the rope?
The string is massless, so net force on any piece must be zero.
What does "inextensible" force about the two blocks?
They have equal displacement, speed, and acceleration magnitude.
Why is a sign convention needed before adding forces?
Forces have direction; you must fix which way is "+" to add them correctly.
State Newton's Second Law.
.
What does a free body diagram show for one hanging block?
Only gravity down and tension up.
If , what is the acceleration and why?
— the two weights balance, so there is no net driving force.
If , which block goes down?
(the heavier side descends); the same formulas still apply.
Why is the tension formula symmetric in and ?
Swapping the two blocks cannot change the rope's pull.

Connections