Statics problem: towing force and friction

AI Thread Summary
The discussion revolves around a statics problem involving a car with locked brakes, where participants are trying to determine the towing force required to move it. The original approach of summing moments and forces was found to be incorrect due to missing terms related to the towing force and the reactions at the wheels. Participants emphasized the importance of including the towing force in the equations of equilibrium and suggested using the vector form of moments for accuracy. Confusion arose regarding the necessity of determining frictional forces and the equality of normal forces at the wheels. Ultimately, the problem was resolved, but the participants expressed a need for further clarification from the professor to solidify their understanding.
jaguar ride
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Homework Statement


Apologies in advance if this problem has been brought here before, I searched and couldn't find it.


The automobile has a mass of 1.7 Mg and center of mass at G. Both the front and rear brakes are locked.
Take μs = 0.3
Determine the towing force F required to move the car.
Hibbeler14.ch8.p5.jpg

Homework Equations


ΣM = 0
ΣFx = 0
ΣFy = 0
friction = μs * normal force

The Attempt at a Solution



The previous question to this was identical (although with different values), but with only the rear brakes locked. I summed the moments about A to find the reaction at B (normal force), and then multiplied that by the coefficient of static friction to find the frictional force, and solved for F using the horizontal force equation.

I tried the same approach for this problem. Summed the moments about A to find the reaction at B, and summed the forces in the Y-direction to find the reaction at A. I then multiplied those by the coefficient of friction to find their respective frictional forces. Then I summed the forces in the X-direction to solve for F. Wrong.

Clearly this approach is incorrect. Am I way off?

My thoughts are: the frictional force at A is greater than at B, will that have an effect? Does tipping somehow come into play in this problem?

Thanks in advance for any help you can offer. I tried to follow the guidelines, but I can show more work if need be.
 
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jaguar ride said:

Homework Statement


Apologies in advance if this problem has been brought here before, I searched and couldn't find it.The automobile has a mass of 1.7 Mg and center of mass at G. Both the front and rear brakes are locked.
Take μs = 0.3
Determine the towing force F required to move the car.
Hibbeler14.ch8.p5.jpg

Homework Equations


ΣM = 0
ΣFx = 0
ΣFy = 0
friction = μs * normal force

The Attempt at a Solution



The previous question to this was identical (although with different values), but with only the rear brakes locked. I summed the moments about A to find the reaction at B (normal force), and then multiplied that by the coefficient of static friction to find the frictional force, and solved for F using the horizontal force equation.

I tried the same approach for this problem. Summed the moments about A to find the reaction at B, and summed the forces in the Y-direction to find the reaction at A. I then multiplied those by the coefficient of friction to find their respective frictional forces. Then I summed the forces in the X-direction to solve for F. Wrong.

Clearly this approach is incorrect. Am I way off?

My thoughts are: the frictional force at A is greater than at B, will that have an effect? Does tipping somehow come into play in this problem?

Thanks in advance for any help you can offer. I tried to follow the guidelines, but I can show more work if need be.
It would be desirable to see your calculations for F.
 
FullSizeRender(1).jpg
The 16660 N is the 1.7*1000*9.8
 
A term is missing from your ∑Ma = 0 expression and your ∑Fx = 0 expression.
Drawing a FBD may help...
 
I do have one, I didn't include it though. I'm failing to see what term I'm missing. I'm using the same technique for the problem I described initially, with the addition of the front wheels' friction. What other force is there to add to my moment equation without giving me too many unkowns? As for the ∑Fx = 0, what other forces are acting in this direction besides both the frictional forces and x-component of F?

Can someone explain why this problem might be different than the other one I mentioned?
FullSizeRender(2).jpg

(oops, the distance between A and where F is applied is 0.75)
 
billy_joule said:
A term is missing from your ∑Ma = 0 expression and your ∑Fx = 0 expression.
Drawing a FBD may help...

Sorry, that was a typo, it should have been ∑Fy = 0.

Your FBD is correct.
Your moment equation is missing the moment about A due to 'F' and a similar term is missing from the ∑Fy = 0 equation
 
jaguar ride said:
I do have one, I didn't include it though. I'm failing to see what term I'm missing. I'm using the same technique for the problem I described initially, with the addition of the front wheels' friction. What other force is there to add to my moment equation without giving me too many unkowns? As for the ∑Fx = 0, what other forces are acting in this direction besides both the frictional forces and x-component of F?

Can someone explain why this problem might be different than the other one I mentioned? View attachment 91877
(oops, the distance between A and where F is applied is 0.75)
Your original approach assumed that the force applied by the tow rope had no effect on the reactions at the wheels A and B.

Since the force in the tow rope has an upward component, the reactions at A and B in the towing situation do not have the same values as when the car is just sitting there.
 
So if include the force of the tow rope in my moment equation, I won't be able to solve for the reactions will I?

Is determining the frictional forces unimportant in this case? I'm pretty confused now.
 
jaguar ride said:
So if include the force of the tow rope in my moment equation, I won't be able to solve for the reactions will I?
Sure you will.

Just before the car starts to move, it is in static equilibrium. The force F is related to the reactions at A and B by the coefficient of friction and the angle of the towline, so you should be able to write the equations of equilibrium for the car and solve for the value of F.
Is determining the frictional forces unimportant in this case? I'm pretty confused now.
You don't need to determine the actual friction forces at each wheel, unless you want to. You know the relationship between the friction forces at each wheel and the force in the towline, which is what you are looking for.

You still use ΣF = 0 and ΣM = 0, but you can't ignore the presence of the towline force F when you write these equations.
 
  • #10
I'm lost now. If I sum the moments about A, then I won't have a reaction at A in my moment equation. Yet I'll still need to know that for the rest of my force equations, won't I?

To top it off, a classmate just told me I need to assume the normal forces are equal, and solve it without even using a moment equation. That can't be right, can it?
 
  • #11
jaguar ride said:
I'm lost now. If I sum the moments about A, then I won't have a reaction at A in my moment equation. Yet I'll still need to know that for the rest of my force equations, won't I?

Why not try it and find out?
Your approach in post #3 is correct and will lead to the answer, all you need to do is include the missing terms mentioned. You will find the reactions in terms of 'F', you don't need to find the numerical values of the reactions to find F.
To top it off, a classmate just told me I need to assume the normal forces are equal, and solve it without even using a moment equation. That can't be right, can it?
Yeah, that's not right, don't listen to them.
 
  • #12
Ok, am I on the right track with these equations? I only have two more attempts to answer this so I can't risk it

EDIT: my vertical force equation includes -16660, I forgot to add it until after I'd uploaded the photo.
FullSizeRender(3).jpg
 
  • #13
jaguar ride said:
Ok, am I on the right track with these equations? I only have two more attempts to answer this so I can't risk it

EDIT: my vertical force equation includes -16660, I forgot to add it until after I'd uploaded the photo.
View attachment 91893
I would say you have approximately the correct approach.

However, the points of application of the reactions A and B, the towing force F, and the weight of the car G, are located at different points with respect to one another. I think you moment equation needs to be more general than you have shown here. You should use the vector form of the moment, M = r × F , here when writing the moments of the various forces about a common reference point.
 
  • #14
I don't understand what you mean by more general. For the moment cause by F, do I not need to use both the components? If I use the cross product rather than what I'm showing here, I'm still ending up with the same answer for that... I'm sorry, It's been a very long day for me and it's hard to understand exactly what you're implying when you say that.

I'm not sure why I'm having such a hard time understanding only this problem. It's making me feel like I've never done statics before.
 
  • #15
jaguar ride said:
I don't understand what you mean by more general. For the moment cause by F, do I not need to use both the components?
M = r × F by definition uses all components of r and F to determine M.

By 'more general', I mean use the cross product to calculate all the moments present in the free body of the car with the tow line attached.

If I use the cross product rather than what I'm showing here, I'm still ending up with the same answer for that...
Are you? You can't know that until you make the calculations.
 
  • #16
Alright, I ended up getting it correct, but this entire problem was really confusing for some reason, and I'm still not sure I actually understand it completely. Thank you both for helping me (or at least trying to). I'm going to talk to my professor in the morning when my brain is actually functioning at a normal level and see if I can really get a grasp on it.
 
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