What Forces Affect the Motion in an Inclined Pulley System?

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SUMMARY

The discussion focuses on the forces affecting the motion in an inclined pulley system involving a 1.0 kg physics book and a 600 g coffee cup. The book is pushed up the slope with an initial speed of 3.0 m/s, and the coefficients of static and kinetic friction are 0.50 and 0.20, respectively. The calculations reveal that the book slides back down the incline after traveling 0.65 meters, and a force of 4.63 N is required to keep the book stationary on the slope.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Knowledge of friction coefficients (static and kinetic)
  • Ability to apply kinematic equations
  • Familiarity with free body diagrams in physics
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  • Study the effects of varying friction coefficients on inclined planes
  • Learn about tension in pulley systems and its calculations
  • Explore advanced kinematic equations and their applications
  • Investigate the dynamics of multi-body systems in physics
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Students studying physics, particularly those focusing on mechanics and inclined planes, as well as educators looking for practical examples of force analysis in pulley systems.

azn_oohwee
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I am having a problem finding the last part of this problem, and I'm not really sure if I did the first part right.

The 1.0 kg physics book in Figure P8.38 is connected by a string to a 600 g coffee cup. The book is given a push up the slope and released with a speed of 3.0 m/s. The coefficients of friction are Us = 0.50 and uk = 0.20.

http://www.webassign.net/knight/p8-38.gif

(a) How far does the book slide?

(b) At the highest point, does the book stick to the slope, or does it slide back down?

If the book sticks, what magnitude of force along the incline is required to make it slide down? If the book slides, what magnitude of force along the incline is required to make the book stick?

So this is what I did.

For the cup
∑(Fc)y = T - mg = ma

For the book.
∑(Fb)y = N - mgcos(@) = 0
∑(Fb)x = -T - fk - mgsin(@) = ma
∑(Fb)x = -T - uk(m(b)*a + (m(b)*g) - m(b)sin(@) = m(b)a

I add the cup to the book.

-m(a)g - uk(m(b)*a + (m(b)*g) - m(b)sin(@) = m(b)a + m(c)a = a(m(b) + m(a))

-{ g(m(a) + uk(m(b)*a + (m(b)*g) - m(b)sin(@) } / { m(b) + m(a) = a

after solving for acceleration I use a to find delta x

Vf = 0, Vi = 3 so

0 = (3)^2 + 2a(deltaX)

deltaX = -9/2a

so that gives me (a)

For (b) I reason the book slides back down.

And for C I'm having trouble visualizing how to set up the problem

I'm setting it up like this

Components to the left:

Tension
Ma
Mgsin@

Components to the right:

static friction
and the force?


I just need a little help on this one. Anything will be greatly appreciated. Thanks.
 
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azn_oohwee said:
The 1.0 kg physics book in Figure P8.38 is connected by a string to a 600 g coffee cup. The book is given a push up the slope and released with a speed of 3.0 m/s. The coefficients of friction are Us = 0.50 and uk = 0.20.

...

So this is what I did.

For the cup
∑(Fc)y = T - mg = ma

For the book.
∑(Fb)y = N - mgcos(@) = 0
∑(Fb)x = -T - fk - mgsin(@) = ma
∑(Fb)x = -T - uk(m(b)*a + (m(b)*g) - m(b)sin(@) = m(b)a


I do not understand your last equation. Why did you replace friction by uk(ma +mg)? Friction is N*uk.

ehild
 
oops sorry..

I meant to write..

∑(Fb)x = -T - fk - mgsin(@) = ma

∑(Fb)x = -T - ukN - mgsin(@) = ma

N = mgcos@ so

∑(Fb)x = -T - ukmgcos@ = ma

-m(a)g - uk(m(b)gcos@ - m(b)gsin@ = m(b)a + m(c)a

a = - { g(m(c) - uk(m(b)cos@) - m(b)sin@ } / {m(b) + m(c) }

That should be more correct.

I have the answers to the problems now. The last question was a bit vague on the wording, i'll have to ask my professor about that one.

(a) 0.65m
(b) slide back down
(C) 4.63N
 

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