Calculation of Box's Acceleration on a Trailer with Friction

In summary: I get it’s just a drawing, but when we are examining internal forces in materials we slice them, making the internal forces external to the slice. To me, leaving part of the box... or part of the trailer... in the drawing makes it less clear to me as to what is being exerted on the other parts.
  • #1
Heexit
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Homework Statement
On a trailer (mass M), there is a box (mass m). A rope runs from the box over a fixed pulley to the back end of the trailer. A pulling force F acts on the trailer. There is friction between the box and the trailer. The trailer is considered to be moving easily on the ground. Calculate the acceleration of the box relative to the ground (see picture for better understanding of question under Attempt at a Solution).
Relevant Equations
f = (mu)*FN, f=ma
Question picture:
1684497141899.png

My solution:
1684497841441.png


Where:
S is the lineforce
Ff is the force as a result of friction
a is the resulting acceleration
F is the acting force

The answear is supposed to be a=(F-2mg(mu))/(m+M)

Any idea what i could have missed?

Thanks for your help on beforehand!
 

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  • #2
Heexit said:
Homework Statement: On a trailer (mass M), there is a box (mass m). A rope runs from the box over a fixed pulley to the back end of the trailer. A pulling force F acts on the trailer. There is friction between the box and the trailer. The trailer is considered to be moving easily on the ground. Calculate the acceleration of the box relative to the ground (see picture for better understanding of question under Attempt at a Solution).
Relevant Equations: f = (mu)*FN, f=ma

Question picture:
View attachment 326774
My solution:
View attachment 326779

Where:
S is the lineforce
Ff is the force as a result of friction
a is the resulting acceleration
F is the acting force

The answear is supposed to be a=(F-2mg(mu))/(m+M)

Any idea what i could have missed?

Thanks for your help on beforehand!
Please take a few moments to learn how to use Latex for posting the mathematics on this site. Your hand writing is not particularly neat. It also helps would be helpers quote where may be wrong directly. The pictures are ok for diagrams, not for the math.

Also you should have separate FBD's for the box and the trailer, and fix a coordinate system ( I would suggest at the pulley ).
 
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  • #3
You seem to think that equation 1 is what you get for the trailer + box system. It is not because friction is not taken into account. Does it make sense that the equation for the two-component system is the same whether friction is there or not?

Write separate equations from separate FBDs as @erobz suggested. When you add them, you should get the correct equation for the trailer + box system and it will not be what you have now.
 
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  • #4
Remember that friction acts on both surfaces (the box and the trailer)
 
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  • #5
erobz said:
Please take a few moments to learn how to use Latex for posting the mathematics on this site. Your hand writing is not particularly neat. It also helps would be helpers quote where may be wrong directly. The pictures are ok for diagrams, not for the math.

Also you should have separate FBD's for the box and the trailer, and fix a coordinate system ( I would suggest at the pulley ).
Thanks for your help!

As per request, here comes the new improved FBD's:
1684500938700.png


And the following equations:
1. ##F_f-S=-ma\Rightarrow -S=-ma-F_f##
2. ##F-S-F_f=Ma\Rightarrow -S=Ma-F+F_f##
This gives:
##-ma-F_f=Ma-F+F_f##
##-a(M+m)=-F+2F_f##, where ##F_f=mg\mu##
##a=\frac {F-2mg\mu} {M+m}##

Thanks for your time and advice!
 
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  • #6
Heexit said:
Thanks for your help!

As per request, here comes the new improved FBD's:
View attachment 326781

And the following equations:
1. ##F_f-S=-ma\Rightarrow -S=-ma-F_f##
2. ##F-S-F_f=Ma\Rightarrow -S=Ma-F+F_f##
This gives:
##-ma-F_f=Ma-F+F_f##
##-a(M+m)=-F+2F_f##, where ##F_f=mg\mu##
##a=\frac {F-2mg\mu} {M+m}##

Thanks for your time and advice!
For future reference, you are "freeing" the trailer of the box, replacing the box with forces it produces on the trailer. There shouldn't be a partial box in the trailers FBD, nor should there be a partial trailer in the boxes FBD.
 
  • #7
erobz said:
For future reference, you are "freeing" the trailer of the box, replacing the box with forces it produces on the trailer. There shouldn't be a partial box in the trailers FBD, nor should there be a partial trailer in the boxes FBD.
Meh. It's an artist's conception, intended to visually depict the source of the normal force ##F_n## on the bottom of the box and the [identically named] normal force ##F_n## on the top of the trailer.

I expect that is also the reason for depicting the string on the left of both drawings. I did find the arrow on the end of the string to be off-putting. However, I think I grasp the intended meaning. The depiction there is of an interface between string and box (or string and trailer). The string is being pulled rightward by the box/trailer. Hence the right arrows. The box/trailer is being pulled leftward by the string. Hence the left arrows.
 
  • #8
jbriggs444 said:
Meh. It's an artist's conception, intended to visually depict the source of the normal force ##F_n## on the bottom of the box and the [identically named] normal force ##F_n## on the top of the trailer.

I expect that is also the reason for depicting the string on the left of both drawings. I did find the arrow on the end of the string to be off-putting. However, I think I grasp the intended meaning. The depiction there is of an interface between string and box (or string and trailer). The string is being pulled rightward by the box/trailer. Hence the right arrows. The box/trailer is being pulled leftward by the string. Hence the left arrows.
I get it’s just a drawing, but when we are examining internal forces in materials we slice them, making the internal forces external to the slice. To me, leaving part of the box (or part of the trailer) hasn’t properly externalized the internal force of friction in this system. That’s why I mentioned it.
 
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  • #9
erobz said:
I get it’s just a drawing, but when we are examining internal forces in materials we slice them, making the internal forces external to the slice. To me, leaving part of the box (or part of the trailer) hasn’t properly externalized the internal force of friction in this system. That’s why I mentioned it.
I would agree with @jbriggs444 on this one. Drawing part of the source as a reference becomes necessary especially in cases of circular motion on surfaces such as a mass sliding on a track. The contact force is centripetal or centrifugal depending on which side of the track the mass is riding. So the curvature of the track is needed for drawing the contact force and the acceleration consistently with the given physical situation. Personally, I draw such reference surfaces in dotted lines to indicate their evanescent nature.
 
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  • #10
kuruman said:
I would agree with @jbriggs444 on this one. Drawing part of the source as a reference becomes necessary especially in cases of circular motion on surfaces such as a mass sliding on a track. The contact force is centripetal or centrifugal depending on which side of the track the mass is riding. So the curvature of the track is needed for drawing the contact force and the acceleration consistently with the given physical situation. Personally, I draw such reference surfaces in dotted lines to indicate their evanescent nature.
Dotted lines are a good compromise (in my opinion), I just wasn’t sure the OP was fully getting that concept given the first “FBD”. If they were just being "efficient" by not separating the bodies, it was that efficiency that lead to the error (I think).
 
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FAQ: Calculation of Box's Acceleration on a Trailer with Friction

How do you calculate the acceleration of a box on a trailer with friction?

To calculate the acceleration of a box on a trailer with friction, you need to apply Newton's second law of motion. The net force acting on the box is the difference between the applied force and the frictional force. The frictional force can be calculated using the coefficient of friction and the normal force. The formula is: \( a = \frac{F_{\text{applied}} - F_{\text{friction}}}{m} \), where \( F_{\text{friction}} = \mu \cdot N \), \( \mu \) is the coefficient of friction, \( N \) is the normal force, and \( m \) is the mass of the box.

What role does the coefficient of friction play in the calculation?

The coefficient of friction (\( \mu \)) is crucial in determining the frictional force that opposes the motion of the box. It quantifies the amount of frictional resistance between the surfaces in contact. A higher coefficient of friction means greater resistance, which reduces the net force and thus the acceleration of the box. The frictional force is calculated as \( F_{\text{friction}} = \mu \cdot N \).

How do you determine the normal force acting on the box?

The normal force (\( N \)) is the force exerted by a surface to support the weight of an object resting on it, acting perpendicular to the surface. For a box on a horizontal trailer, the normal force is equal to the gravitational force acting on the box, which is \( N = m \cdot g \), where \( m \) is the mass of the box and \( g \) is the acceleration due to gravity (approximately 9.8 m/s²).

What if the trailer is moving on an incline?

If the trailer is on an incline, the normal force changes because it is no longer equal to the full weight of the box. The normal force is calculated as \( N = m \cdot g \cdot \cos(\theta) \), where \( \theta \) is the angle of the incline. Additionally, the gravitational component along the incline affects the net force and must be considered: \( F_{\text{gravity, parallel}} = m \cdot g \cdot \sin(\theta) \). The net force then becomes \( F_{\text{net}} = F_{\text{applied}} - F_{\text{friction}} - F_{\text{gravity, parallel}} \).

How do you account for dynamic versus static friction in these calculations?

Static friction acts when the box is at rest relative to

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