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Need help with a m1 friction question

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Original post by coconut64
I got the right answer by using your hint so thank you for that. But it doesn't make sense though because friction can be the same in both diagram and surely it is not right to assume that friction is the same in both cases....


No worries! Yeah, that's right but unfortunately it is assumed that they are the same because otherwise you cannot solve the question.
Reply 21
Original post by leaf3
Hey, wondering what the answer was as I've worked through it for practice so am curious if I got it right :P
Glad you got it sorted!


its 2.1 to 2sf thanks.
Reply 22
Original post by Mehrdad jafari
No worries! Yeah, that's right but unfortunately it is assumed that they are the same because otherwise you cannot solve the question.


At first, i thought you have to assume u is the same for both diagram...
Original post by coconut64
At first, i thought you have to assume u is the same for both diagram...


Well, μ\mu is definitely the same as it's a constant calculated for that slop and specific object. It's the reaction force that is not constant in both case.
Reply 24
Original post by Muttley79
The angle of the slope is greater than that at limiting friction so the frictional force is at its limiting value - it is also moving which means that the downward force of gravity has overcome the friction.

The frictional force acts of course up the slope - it opposes [or in this case tries to oppose] motion.

If you post your working I'll check it for you :smile:


I did post my work and I do understand limiting equilibrium. I think it means that when it is 30 degrees, the object is not moving because friction is equal to the other force going in the opposite direction which is why it stays still. Whereas for the second one :45 degrees, the other force is greater than the max friction and thats why it is accelerating downwards. What i don't get in this question it is why friction stays constant in both diagram although R is different. If it is based on assumption, then why not assume u is the same for both diagrams and go from there? But u can't be the same though because of different reaction forces. Does this question actually make sense?? ThANKS
Reply 25
Original post by Mehrdad jafari
Well, μ\mu is definitely the same as it's a constant calculated for that slop and specific object. It's the reaction force that is not constant in both case.


so it is pointless to work out u then?
Original post by coconut64
I did post my work and I do understand limiting equilibrium. I think it means that when it is 30 degrees, the object is not moving because friction is equal to the other force going in the opposite direction which is why it stays still. Whereas for the second one :45 degrees, the other force is greater than the max friction and thats why it is accelerating downwards. What i don't get in this question it is why friction stays constant in both diagram although R is different. If it is based on assumption, then why not assume u is the same for both diagrams and go from there? But u can't be the same though because of different reaction forces. Does this question actually make sense?? ThANKS


It's not in equlibrium when it's moving!

You can only put forces perpendicular to the plane equal ... does that help?
Original post by coconut64
so it is pointless to work out u then?


You couldn't work it out as you don't know the mass of the object.
Reply 28
Original post by Mehrdad jafari
You couldn't work it out as you don't know the mass of the object.


I left m as mass and they cancel out at the end. But I got 2.9 by using u
Original post by coconut64
I left m as mass and they cancel out at the end. But I got 2.9 by using u


Looking at it again, yeah, you can work out the coefficient of friction, but I got 0.29m/s2 for the acceleration of the body. How did you work that out?

Edit: yes, I got 2.93m/s2 (3 s.f) as well as I hadn't taken g into my calculation.
(edited 8 years ago)
Reply 30
Original post by Mehrdad jafari
Looking at it again, yeah, you can work out the coefficient of friction, but I got 0.29m/s2 for the acceleration of the body. How did you work that out?

Edit: yes, I got 2.93m/s2 (3 s.f) as well as I hadn't taken g into my calculation.


I somehow managed to but thats not right, so don't worry. Thanks for helping :smile:
Original post by coconut64
I somehow managed to but thats not right, so don't worry. Thanks for helping :smile:


Yeah, and I highly doubt the question required you to take account of the change in friction but here is my method:

When the object is in equilibrium, you can work out the horizontal components to the plane:
Let's take θ=30\theta=30 and the angle between reaction force and the horizontal component α=60\alpha=60. Therefore,

F1cosθ=R1cosαF_1 \cos \theta=R_1\cos\alpha,

F1=R1cosαcosθF_1=\dfrac{R_1\cos\alpha}{\cos \theta} , but R1=mgcosθR_1=mg\cos\theta

F1=mgcosθcosαcosθ=mgcosαF_1=\dfrac{mg\cos\theta\cos\alpha}{\cos \theta}=mg\cos\alpha

Therefore:
μ=F1R1=mgcosαmgcosθ=cosαcosθ\mu=\dfrac{F_1}{R_1}=\dfrac{mg \cos\alpha}{mg\cos\theta}=\dfrac{ \cos\alpha}{\cos\theta}

For when the angle of inclination is increased, that is when the raction force has decreased, we have:

R2=mgcos45R_2=mg\cos45

mgsin45F2=mamg\sin45 -F_2=ma
But F2=μR2=mgcos45(cosαcosθ)F_2=\mu R_2=mg\cos45 (\dfrac{ \cos\alpha}{\cos\theta})

So mgsin45mgcos45(cosαcosθ)=mamg\sin45 -mg\cos45 (\dfrac{ \cos\alpha}{\cos\theta})=ma

g(sin45cos45(cosαcosθ))=a\rightarrow g(\sin45 -\cos45 (\dfrac{ \cos\alpha}{\cos\theta}))=a

I hope this is correct.
(edited 8 years ago)
Reply 32
Original post by Mehrdad jafari
Yeah, and I highly doubt the question required you to take account of the change in friction but here is my method:

When the object is in equilibrium, you can work out the horizontal components to the plane:
Let's take θ=30\theta=30 and the angle between reaction force and the horizontal component α=60\alpha=60. Therefore,

F1cosθ=R1cosαF_1 \cos \theta=R_1\cos\alpha,

F1=R1cosαcosθF_1=\dfrac{R_1\cos\alpha}{\cos \theta} , but R1=mgcosθR_1=mg\cos\theta

F1=mgcosθcosαcosθ=mgcosαF_1=\dfrac{mg\cos\theta\cos\alpha}{\cos \theta}=mg\cos\alpha

Therefore:
μ=F1R1=mgcosαmgcosθ=cosαcosθ\mu=\dfrac{F_1}{R_1}=\dfrac{mg \cos\alpha}{mg\cos\theta}=\dfrac{ \cos\alpha}{\cos\theta}

For when the angle of inclination is increased, that is when the raction force has decreased, we have:

R2=mgcos45R_2=mg\cos45

mgsin45F2=mamg\sin45 -F_2=ma
But F2=μR2=mgcos45(cosαcosθ)F_2=\mu R_2=mg\cos45 (\dfrac{ \cos\alpha}{\cos\theta})

So mgsin45mgcos45(cosαcosθ)=mamg\sin45 -mg\cos45 (\dfrac{ \cos\alpha}{\cos\theta})=ma

g(sin45cos45(cosαcosθ))=a\rightarrow g(\sin45 -\cos45 (\dfrac{ \cos\alpha}{\cos\theta}))=a

I hope this is correct.

I got similar as that as well but I think the question is poorly worded because friction can be the same in both. Thank you
Original post by coconut64
I got similar as that as well but I think the question is poorly worded because friction can be the same in both. Thank you


No worries! I just posted my method to show why I thought the friction is not constant in both case but yeah, that wasn't supposed to be a substitute for the answer. :smile:
Reply 34
Original post by Mehrdad jafari
No worries! I just posted my method to show why I thought the friction is not constant in both case but yeah, that wasn't supposed to be a substitute for the answer. :smile:


Hi, sorry to bother but could you possibly give me some help on this question http://www.thestudentroom.co.uk/showthread.php?t=3794861&p=61558317#post61558317 thanks
Original post by coconut64
Hi, sorry to bother but could you possibly give me some help on this question http://www.thestudentroom.co.uk/showthread.php?t=3794861&p=61558317#post61558317 thanks


No worries! I see the bear has already helped you on the thread.

All the best.
This question is okay but the solution is totally wrong. Someone needs to point it out to the author of the material and please do not carry over that assumption unless explicitly stated.

Fr_max = (Meu)*R is the equation of "MAXIMUM" Static Friction.

Static friction may vary from zero to Fr_max for any given arrangement. Fr_max does not change just because a pull force is introduced, but Fr_max Changes whenever R changes and there is no theory or assumption that upturns this.

In our everyday life for example, merely stepping on a sliding object makes it stop.

Therefore, just as placing another body on the initial mass is enough to cause a greater maximum friction, so does a change in the mgcos(alpha) component or any resultant force in the vertical direction.

The correct answer is therefore 2.9 m/s^2
(edited 8 years ago)

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