Cylinder attached to a block on an inclined plane, rotational dynamics

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A cylinder with mass M and radius R rolls down an inclined plane while pulling a block of mass Mb, with the system's motion affected by friction and gravity. The moment of inertia for the cylinder is given as I_c = 1/2 MR^2. The challenge is to derive the linear acceleration of the system, considering the forces acting on both the cylinder and the block. A proposed solution for the linear acceleration is a = 2g[(M + Mb)sinθ - μMbcosθ] / (3M + 2Mb). Participants in the discussion suggest drawing free body diagrams to clarify the forces involved and help in solving the problem accurately.
jsrev
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Homework Statement



A cylinder of mass M and radius R, with moment of inertia:
I_c = \frac{1}{2}MR^2
rolls down without slipping through an inclined plane with an angle of θ, while pulling a block of mass Mb with an attached frame (of insignificant mass) which is connected to the axis of the cylinder.
If the cylinder rolls without slipping over the surface and the coefficient of kinetic friction between the block Mb and the surface is μ, then:

a. Deduct an expression for the linear acceleration of the system.

This problem didn't come with a figure, but I made one based on what I think the system looks like.
See figure http://imgur.com/HyiUSLu


Homework Equations



Linear acceleration

The Attempt at a Solution



I've tried a few ways, like calculating the linear acceleration of each object (the cylinder and the block) but there are some things I don't get.
I have tried calculating
a_{cylinder} = \frac{gsinθ}{k}
given that k is a constant that equal 1/2 from the first equation. Then I got the linear acceleration of the block with a_{block} = gsinθ and also considered the friction, but I'm not any close to the answer.

The given solution is:

a = \frac{2g[(M+M_b)sinθ-μM_bcosθ]}{3M + 2M_b}

If anyone can guide me a little bit in this one I would really appreciate it. Thank you.
 
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jsrev said:

Homework Statement



A cylinder of mass M and radius R, with moment of inertia:
I_c = \frac{1}{2}MR^2
rolls down without slipping through an inclined plane with an angle of θ, while pulling a block of mass Mb with an attached frame (of insignificant mass) which is connected to the axis of the cylinder.
If the cylinder rolls without slipping over the surface and the coefficient of kinetic friction between the block Mb and the surface is μ, then:

a. Deduct an expression for the linear acceleration of the system.

This problem didn't come with a figure, but I made one based on what I think the system looks like.
See figure http://imgur.com/HyiUSLu


Homework Equations



Linear acceleration

The Attempt at a Solution



I've tried a few ways, like calculating the linear acceleration of each object (the cylinder and the block) but there are some things I don't get.
I have tried calculating
a_{cylinder} = \frac{gsinθ}{k}
given that k is a constant that equal 1/2 from the first equation. Then I got the linear acceleration of the block with a_{block} = gsinθ and also considered the friction, but I'm not any close to the answer.

The given solution is:

a = \frac{2g[(M+M_b)sinθ-μM_bcosθ]}{3M + 2M_b}

If anyone can guide me a little bit in this one I would really appreciate it. Thank you.
Draw a free body diagram for the cylinder, and one for the block.

Here's your image:
attachment.php?attachmentid=70542&stc=1&d=1402529651.png
 

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See post 4
dean barry
 
Last edited:
Sorry, made a hash of that, here's the revised effort :

Assuming its a homogenous cylinder, then the equivalent mass (Me) of the non slipping cylinder for acceleration calculation purposes = 1.5 * M
(kg)

The total mass (Mt) being accelerated = Me + Mb
(kg)

The force due to gravity driving the system = ( M * g * sine θ ) + ( Mb * g * sine θ )
(Newtons)

The drag force of the block = Mb * g * cosine Ѳ * µ
(Newtons)

So :
The net force (fn) driving the system :
fn = ( ( M * g * sine θ ) + ( Mb * g * sine θ ) ) - ( Mb * g * cosine Ѳ * µ )

The acceleration (a) of the system = fn / Mt
So :
a = ( ( ( M * g * sine θ ) + ( Mb * g * sine θ ) ) - ( Mb * g * cosine Ѳ * µ ) ) / ( Me + Mb )

Comments ?
deanbarry365@yahoo.com
 
dean barry said:
Sorry, made a hash of that, here's the revised effort :

Assuming its a homogenous cylinder, then the equivalent mass (Me) of the non slipping cylinder for acceleration calculation purposes = 1.5 * M
(kg)
What?
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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