How Do You Calculate the Minimum Angle to Push a Mop Considering Friction?

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To calculate the minimum angle to push a mop considering friction, the force required to initiate movement is given by P = (U_k * mg) / (sinθ - U_k * cosθ). The discussion revolves around finding the angle θ where it becomes impossible to push the mop, concluding that this occurs when tanθ > U_k. Participants clarify that θ is relative to the horizontal and explore the implications of static versus kinetic friction. Ultimately, the correct relationship for determining the minimum angle is derived as tanθ > U_k. This highlights the importance of understanding friction in relation to the angle of applied force.
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Hi, I need help with the following problem:

You are pushing a mop of mass m with a force P at an angle theta. The coefficiant of friction is U_k.

Find P so that the mop will start moving in terms in \theta,U_k ,m,g.

I solved this part and got:

<br /> P = \frac {(U_k *mg )}{( \sin\theta- U_k*\cos\theta)}

Now, for part 2 I have to find the minimum angle \theta for which it will be impossible for me to push the mop in terms of \theta,U_k ,m,g,P..

Like at 90 degrees It is impossible to push the mop. Any help on part 2 would be appreciated.

Thanks
 
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is theta relative to to the vertical or to the horizontal ?
if it is relative to the horizontal, i got 45 degree. Pcos(theta) = miu*N
 
Theta is relative to the Vertical. Can you explain how you got 45?

Thanks
 
45 degree is wrong, sorry. i think you have got the right anwer ninety degree.
 
The answer is below 90 degrees. From theta to 90 it will not move.
 
if theta is below ninety degree if it won't move, i don't know how the p found in the first part can move the mop.
 
P is the force required for it to move at the angle Theta. The 2nd part of the problem is to find an angle theta such that any amount of P would not be able to move the mop.

My guess is that theta is somewhere around 80 degrees, however I am looking for the true solution.
 
sorry, can't help you with that !

i found a similar question in my book. it introdueces both \mu_s for coefficient of static friction and \mu_k as coeffiecient of kinetic friction.

if the force P can't move the mop, then Psin\theta&lt;\mu_s*N; then
Psin\theta&lt;\mu_s*N
Psin\theta&lt;\mu_s*(mg+Pcos\theta)
sin\theta-\mu_s*cos\theta&lt;\frac{\mu_s*mg}{P}
\sqrt{1+\mu_s^2}*sin(\theta-tan^{-1}\mu_s)&lt;\frac{\mu_s*mg}{P}
\theta&lt;sin^{-1}\frac{\mu_s*mg}{P*\sqrt{1+\mu_s^2}}+tan^{-1}\mu_s
so \theta_{min}=sin^{-1}\frac{\mu_s*mg}{P*\sqrt{1+\mu_s^2}}+tan^{-1}\mu_s so that the mop will move.
 
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thank you Leong, for the help
Unfortunately, it it a little too complex and there is no U_s in the problem.

The correct answer is that \tan\theta &gt; U_k

I am still looking for how to arrive at this answer.
 
  • #10
to move a thing in a frictional surface, don't we need to overcome the static friction first to get started to move, we use uk to relate the friction when it is in motion, a little weird i think for the answer to have uk.
 
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  • #11
I found the answer. It was actually very simple

From the answer I got for part 1:

<br /> P = \frac {(U_k *mg )}{( \sin\theta- U_k*\cos\theta)}

We can say that \sin\theta- U_k*\cos\theta &gt; 0

Working it out you get that \frac{\sin\theta}{\cos\theta} &gt; U_k

And then you get that \tan\theta &gt; U_k
 
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