1.2.10Newton's Laws & Dynamics

Atwood machine — derivation

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WHAT is an Atwood machine?

The idealisations matter — let's say why:

  • Massless string → tension is the same everywhere along it. (A massive string would need net force to accelerate itself, so TT would differ between ends.)
  • Inextensible string → both masses have the same acceleration magnitude. If m1m_1 drops by xx, m2m_2 rises by xx.
  • Massless, frictionless pulley → it just redirects the rope; it does not store/rob any force, so tension is unchanged across the pulley.
Figure — Atwood machine — derivation

HOW to derive it (from first principles)

We use only Newton's second law, Fnet=maF_{net} = ma, on each mass separately. This is Derivation-from-scratch.

Step 1 — Choose which way it accelerates. Assume m1>m2m_1 > m_2, so m1m_1 goes down and m2m_2 goes up. Why this step? We must commit to a sign convention. We'll define "the direction of motion" as positive for each mass — if we guessed wrong, aa just comes out negative, which self-corrects.

Step 2 — Forces on each mass. Each mass feels two forces: gravity mgmg (down) and tension TT (up, the rope always pulls toward the pulley).

For m1m_1 (accelerating down, take down as +): m1gT=m1a(1)m_1 g - T = m_1 a \qquad (1) Why this step? Down is positive here, so the downward weight is +m1g+m_1g and the upward tension is T-T. Net = mass × acceleration.

For m2m_2 (accelerating up, take up as +): Tm2g=m2a(2)T - m_2 g = m_2 a \qquad (2) Why this step? Up is positive here, so tension is +T+T, weight is m2g-m_2g. Same aa because the rope is inextensible.

Step 3 — Add the two equations to eliminate TT. (m1gT)+(Tm2g)=m1a+m2a(m_1 g - T) + (T - m_2 g) = m_1 a + m_2 a m1gm2g=(m1+m2)am_1 g - m_2 g = (m_1 + m_2)a Why this step? The unknown TT appears as T-T and +T+T; adding cancels it, leaving only aa.

Step 4 — Find tension. Substitute aa back into (2): T=m2(g+a)T = m_2(g+a). T=m2 ⁣(g+(m1m2)gm1+m2)=m2(m1+m2)g+(m1m2)gm1+m2T = m_2\!\left(g + \frac{(m_1-m_2)g}{m_1+m_2}\right) = m_2 \cdot \frac{(m_1+m_2)g + (m_1-m_2)g}{m_1+m_2}


WORKED EXAMPLES


COMMON MISTAKES


Flashcards

What does an inextensible string guarantee about the two masses?
They have equal acceleration magnitude (and equal-but-opposite displacement/velocity).
What does a massless string guarantee?
Tension is the same at every point of the rope.
Acceleration of an Atwood machine?
a=(m1m2)gm1+m2a = \dfrac{(m_1-m_2)g}{m_1+m_2}
Tension in an Atwood machine?
T=2m1m2m1+m2gT = \dfrac{2m_1m_2}{m_1+m_2}\,g
Why add the two Newton equations during the derivation?
To eliminate the unknown tension TT (it appears as +T+T and T-T).
Check: if m1=m2m_1=m_2, what are aa and TT?
a=0a=0 and T=mgT=mg.
Check: if m2=0m_2=0, what are aa and TT?
a=ga=g (free fall) and T=0T=0.
Why is tension less than the heavy mass's weight?
Because m1m_1 is accelerating downward, so net force on it is downward → T<m1gT<m_1g.
What is the driving force of the system?
The weight difference (m1m2)g(m_1-m_2)g.
What inertia resists that force?
The total mass (m1+m2)(m_1+m_2).

Recall Feynman: explain to a 12-year-old

Imagine a rope over a wheel with a bucket on each end. If both buckets weigh the same, nothing happens. If you put a rock in one bucket, that side sinks and the other rises — but they're tied together, so they move at the same speed. The rope pulls up on both buckets with the same strength (because the rope is light and the wheel is smooth). How fast it speeds up depends on how much extra weight you added compared to how much stuff you're trying to move in total. More extra weight → faster; more total stuff → slower (heavier to get going).


Connections

Concept Map

idealised as

idealised as

idealised as

gives

gives

apply Newton 2nd law

apply Newton 2nd law

add equations

add equations

solve for a

substitute back

Atwood machine: m1, m2 over pulley

Massless string

Inextensible string

Frictionless massless pulley

Tension same everywhere

Same acceleration magnitude

Eq 1: m1 g - T = m1 a

Eq 2: T - m2 g = m2 a

Eliminate T

a = m1 - m2 g / m1 + m2

T = 2 m1 m2 g / m1 + m2

Hinglish (regional understanding)

Intuition Hinglish mein samjho

Atwood machine ka idea bilkul simple hai: do masses ek halki (massless) aur na khinchne wali (inextensible) rope se judi hain, jo ek smooth pulley ke upar se guzarti hai. Kyunki rope ek hi hai, dono masses ki acceleration ka magnitude same hota hai — bas direction opposite. Aur kyunki rope ka apna koi weight nahi, rope mein tension TT har jagah equal rehta hai. Yeh do baatein puri derivation ki jaan hain.

Derivation mein hum har mass par alag se Newton ka second law Fnet=maF_{net}=ma lagate hain. Heavy mass m1m_1 neeche jaa rahi hai, toh us par: m1gT=m1am_1 g - T = m_1 a. Light mass m2m_2 upar jaa rahi hai, toh us par: Tm2g=m2aT - m_2 g = m_2 a. Dono equations ko add karte hain taaki TT cancel ho jaye, aur seedha mil jaata hai a=(m1m2)gm1+m2a = \frac{(m_1-m_2)g}{m_1+m_2}. Yeh wapas daalo toh tension T=2m1m2m1+m2gT = \frac{2m_1m_2}{m_1+m_2}g.

Intuition yeh hai: system ko aage badhane wala "driving force" sirf weight ka difference (m1m2)g(m_1-m_2)g hai, aur jo cheez resist karti hai woh hai total mass (m1+m2)(m_1+m_2). Isiliye agar dono masses barabar ho jaayein toh a=0a=0 — koi motion nahi. Yaad rakho: tension kabhi m1gm_1g ya m2gm_2g ke equal nahi hota jab tak acceleration ho — woh dono ke beech mein hoti hai.

Exam tip: pehle hamesha free body diagram banao, sign convention fix karo (motion direction ko positive lo), phir dono equations add karke TT uda do. Yeh same trick inclined plane aur multi-pulley problems mein bhi kaam aati hai.

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