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Guess we're all fine so let's get down to business shall we?

Problem:

A box of mass m is placed on a frictionless incline at an angle to the horizontal. The box is connected by a light, inextensible rope over a frictionless pulley at the top of the incline to a hanging mass M.

  • At time t=0, the system is released from rest.
  • Assume the rope does not slip on the pulley.
  • The incline and pulley apparatus are fixed.

Question: What is the acceleration of the box just after release?

(i know the image looks weird, but it's AI generated and I hope you get the idea)

1,000 sats paid
noknees's bounties

F net M = M * a = Tension - M * g

F net m = m * a = m * g * sin(ɵ) - Tension

adding the two equations: a(M+m) = g [m * sin(ɵ)] - g * M

final answer: a = g {[m * sin(ɵ)] - M}/(M+m)

good review in 11 min here;

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excellent! Correct steps too!

Congo to @SHA256man for this weeks BNB 🥳!


Here is the detailed solution in case some don't understand:

Given:Given:

  • Mass of box on incline:
  • Incline angle:
  • Hanging mass:
  • Pulley: frictionless bearing but with moment of inertia and radius (to be included for rotational effects)
  • Rope: light and inextensible
  • The system is released from rest at
  • Incline is frictionless

Okay so,

  • Let acceleration of box along the incline be $a$ downwards (positive direction along slope down).
  • The hanging mass moves vertically downward with acceleration .
  • Let tensions on the box side of the rope and hanging mass side be and respectively.
  • Because the pulley has rotational inertia, .

(Box accelerates down the incline, gravity component downward minus tension force opposing motion.)

(Mass accelerates downwards, gravity downward minus tension upward.)

Since the rope unwinds without slipping, the angular acceleration of the pulley relates to linear acceleration by:

Torque on pulley is caused by difference in tensions:

Rearranged:

We have 3 equations:

Rewrite tensions from (1) and (2):

Substitute into (3):

Simplify:

Group terms with on right:

  • If pulley moment of inertia , this reduces to a simpler formula:

(This case may be problematic if , implying infinite acceleration—showing the importance of pulley inertia.)

  • If the pulley has significant , the denominator increases, reducing acceleration. :)
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ooph, i have to review the torque mechanics a bit, the pulleys i solved intuitively and then wrote out the solution in a structured manner; thank u for the challenge and an opportunity to review some basics!

  • have u looked at SCIENCIA from wooden books?

  • how do u format the equations into standard scientific format? what quick online or github tool do u use for that?
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looks worthy of reading, i must try it

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how do u format the equations into standard scientific format? what quick online or github tool do u use for that?

Look up MathJax and LaTeX

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10 sats \ 1 reply \ @Scroogey 2 Dec

The masses and the pulley are irrelevant when you ask about the acceleration?

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no but the pulley is a frictionless bearing but with moment of inertia I and radius R (to be included for rotational effects)

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Haha that image itself is like a MC Escher painting

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lol true

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