Work of kinetic friction on block in vertical circle

AI Thread Summary
A block of mass 0.015 kg on a vertical circular track loses contact at an angle of 130 degrees, and the work done by kinetic friction (Wk) needs to be calculated. The gravitational work done (Wmg) has been calculated as -0.072447 J, while the normal force (WN) is zero at the point of losing contact. The key to finding the final velocity (vf) before the block leaves the track involves understanding that only the radial component of the weight contributes to centripetal acceleration. It is concluded that the mass of the block affects the friction force but does not influence the calculation of vf directly, as it cancels out in the equations. The discussion emphasizes the importance of using the Work-Energy Theorem to relate work done by non-conservative forces to changes in potential and kinetic energy.
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Homework Statement



1. Homework Statement
A block of mass 0.015kg enters the bottom of a circular, vertical track with a radius R = 0.3m at an initial velocity of 4/ms. If the block loses contact with the track at an angle of 130 degrees, what is Wk, the work done by kinetic friction?


Homework Equations



F=ma
Wtot= Wmg+WN+WFk=1/2*mvf2-1/2*mvi2


The Attempt at a Solution



So far I have that Wmg=-mg*(Rcos50+R)=-0.072447J and that WN=0 J
The only part that I am having trouble with is finding vf right before that block leaves the track. Any help would be appreciated!

EDIT: I am not sure how to go about relating F=ma=mv2/R without knowing what the friction force is ie. fk
 
Last edited:
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galaticman said:

Homework Statement



1. Homework Statement
A block of mass 0.015kg enters the bottom of a circular, vertical track with a radius R = 0.3m at an initial velocity of 4/ms. If the block loses contact with the track at an angle of 130 degrees, what is Wk, the work done by kinetic friction?


Homework Equations



F=ma
Wtot= Wmg+WN+WFk=1/2*mvf2-1/2*mvi2


The Attempt at a Solution



So far I have that Wmg=-mg*(Rcos50+R)=-0.072447J and that WN=0 J
The only part that I am having trouble with is finding vf right before that block leaves the track. Any help would be appreciated!

EDIT: I am not sure how to go about relating F=ma=mv2/R without knowing what the friction force is ie. fk

Read the thread about 6 down, made by GGDK
 
When the block loses contact with the track, the normal force is 0. So only the radial component of the weight force contributes to the centripetal acceleration at that point.
 
PeterO said:
Read the thread about 6 down, made by GGDK

PhanthomJay said:
When the block loses contact with the track, the normal force is 0. So only the radial component of the weight force contributes to the centripetal acceleration at that point.

So if I am understanding this correctly would that mean that:
1. Fxmg=mv2/R
2. mg*sin40=mv2/R
3. vf=√(R*9.8*sin40)
4. vf=1.3747m/s

AND would that also mean that the mass of the block did not matter for Vf
 
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galaticman said:




So if I am understanding this correctly would that mean that:
1. Fxmg=mv2/R
2. mg*sin40=mv2/R
3. vf=√(R*9.8*sin40)
4. vf=1.3747m/s
yes
AND would that also mean that the mass of the block did not matter for Vf
Well, it cancels out, but if the mass was higher, the block would not travel 130 degrees, it would travel less since there is more friction force .. So it does matter, even though you don't need to know it to solve this problem.

I see that per PeterO, help is already being provided in a separate post from another OP. I might just add that instead of using W_t = \Delta KE,
which is OK to use, you might want to use the alternate form of the Work-Energy Theorem , W_{nc} = \Delta PE + \Delta KE,
where since the normal force does no work and since gravity is not a non-conservative force, then W_{nc} = W_{friction}
 
thanks so much! I understand the entire problem completely now! you were a huge help
 
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