Force Components, Friction, etc. Check my work?

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SUMMARY

The discussion centers on calculating the force required to pull a sled up a slope, specifically addressing the force of friction and the normal force. The problem involves a sled with a mass of 26.0 kg, a static friction coefficient (μs) of 0.096, and a slope angle of 12 degrees. The calculated pulling force (FP) was initially determined to be 76.9 N, but further analysis revealed a more accurate value of 78.4 N due to the inclusion of the vertical component of the pulling force affecting the normal force. The participants engaged in a detailed examination of the forces at play, particularly the impact of the applied force on the sled's stability.

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Summer95
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Could someone credible please check my work on this one?

Homework Statement


This problem is "pulling a sled up a slope"
All relevant data is in the picture. I wanted to find FP (The force one has to pull to start the sled moving up with slope).

mass = 26.0kg
μs = 0.096
slope of hill = 12 degrees
FP = 23 degrees (from horizontal)

I did all my work in the rotated reference frame where the x direction is in line with the slope of the hill.

Homework Equations


I fully believe I got the right answer which is why I want this to be double and triple checked to make sure I really do understand everything here. I have my midterm on Friday so now is the time to learn!

The Attempt at a Solution


The solution I got was FP = 76.9N

Thank you so much in advance! <3‿<3
 
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I got a slightly higher number. To wit, 78.4N.

I notice a term μsFpsin(11) in your work which I did not have.
 
rude man said:
I got a slightly higher number. To wit, 78.4N.

I notice a term μsFpsin(11) in your work which I did not have.

Thanks for replying :) I see exactly what you did differently so I'll explain and can you tell me where/if I wrong in the following?

To find the Ffriction it is dependent on FN which ordinarily would be equal to the y component of Fg. However, there is also a y component to FP (an applied force in the y direction) which reduces FN by FPY. In other words because you are pulling up on the object the normal force is reduced. If this were not the case there would be a net force in the y direction and it would accelerate off the slope. That is where μsFpsin(11) in my work comes from. It is part of 0.096[mgcos(12)-FPsin(11)] where FPsin(11) is the y component of the applied force FP.
 
Well, guess what, I agree! Except one thing bothers me: the force Fpsin(11) is not applied at the c.g. of the sled, but at one edge. So the tendency of that vertical component of Fp is to tilt the sled upwards rather than lift it evenly off the ramp. So the part of the surface contact the sled makes with the ramp that is closest to the rope will get "lighter" but the part on the low end will hardly be affected. I guess you can say it averages out. Certainly I was remiss in neglecting that vertical component. So congrats! I'd say the apprentice beat the master except I'm no master!
 
Thanks! That is an interesting point. Would it balance out perfectly or would that factor into a more accurate answer?
 
I think it would balance out and your analysis was spot-on.
 
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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