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MAIN QUESTION
A mass body is held in place by a friction force. The object that generates this friction accelerates upwards. Because the acceleration is not acting inline with the center of mass of the body, the body starts to rotate around its contact point. Which is a result of the moment of friction that is not big enough to keep the body in place.

The main question is how to calculate the maximum linear acceleration to prevent any angular displacement of the body? (The acceleration is applied on the object that holds the body through the friction)

Some sub-questions that would help me are:

  • How to calculate the moment of friction?
  • How to translate the linear acceleration to a moment or angular momentum when it accelerates from the center of the friction connection?
  • Is it correct to use the center of the friction connection as the "origin" of the calculation? (Moments, inertia and angular acceleration would be calculated relative to this "origin")

Previous formulation of the question. It gives more background information and an example situation of the question to clarify the question.

Context
I am currently writing software that automatically calculates the maximum linear acceleration of a 6-axis robot when holding a product. The robot uses a gripper to pick and place products. The product may not displace or rotate relative to the gripper.

Problem
In the first place I assumed it would be as simple as: $\sum F=m*a$. But this would only suffice if the product is picked in its center of mass. When the product is not picked in its center of mass, the product starts to rotate a bit when the robot (de-)accelerates (Example situation can be seen in figure 1).

Example of the situation

Thoughts so far...
Assumed is that the clamping force is evenly spread over the contact area between the product and gripper. The gravitational force generates a moment relative to the center of the contact area. The friction force is spread over the area which would generate a opposing moment. The acceleration of the gripper would generate an angular momentum.

These moments together with the differential of the momentum would then be implemented in: $$\sum M + \dfrac{\Delta L}{\Delta t} = I * \alpha$$ Then assume $\alpha = 0 \hspace{2mm}rad/s^2$ and calculate the maximal momentum. Which would need to be translated back to a linear acceleration ...

Sketch of free body diagram

No idea if I am heading in the right direction. I cannot find any examples where a clamped body rotates around the center of the friction contact area due to linear motion.

Any help would be appreciated. Thanks in advance.

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  • $\begingroup$ The question in its present state may be marked as off-topic. Can you rephrase it to refer to the concepts you're trying to apply to the problem? $\endgroup$
    – user191954
    Commented Jun 21, 2018 at 12:05
  • $\begingroup$ Thanks for the tip. Thought it was better to describe the problem directly in an example situation, because I find it hard to explain the problem without it. Hopefully, it is better now... $\endgroup$
    – Jasper
    Commented Jun 21, 2018 at 13:01
  • $\begingroup$ It's better, particularly because your new first paragraph sets up a somewhat general situation. But the question " how to calculate the maximum linear acceleration of the object..." is still a bit sticky. I don't know how much this'll help, but maybe you could try asking about the factors to be considered while calculating the acceleration, or the causes of different forces that are experienced by the object... $\endgroup$
    – user191954
    Commented Jun 21, 2018 at 13:07
  • $\begingroup$ Edited the question again. Hopefully the main question is better described. Added some sub-questions which would help me in the right direction. $\endgroup$
    – Jasper
    Commented Jun 21, 2018 at 13:50
  • $\begingroup$ If your interest is purely practical, you can always increase the tangential frictional force $F$ and torque $M$ applied by the gripper by increasing the normal gripping force $N$. From a theoretical point of view the problem is much more difficult. Sliding friction is dealt with in the article Frictional Coupling between Sliding and Spinning Motion. In that case the local direction of friction can be found from the local direction of relative motion, and where there is relative motion the friction force is defined by $F=\mu N$. ... $\endgroup$
    – sammy gerbil
    Commented Jun 22, 2018 at 13:48

2 Answers 2

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Your intuition is correct. The problem is as "simple" as applying Newton's 2nd Law for linear and rotational motions : $$\vec{F}-m\vec{g}=m\vec{a}$$ $$M-mgx=I\alpha$$ where $F$ is the resultant static friction force, $M$ is the moment of the friction forces, and $x$ is the horizontal distance of the centre of the friction force from the centre of mass of the block.

$\vec{F}$ can be deduced quite easily from the 1st equation. If there were no torques involved we could then assume that $F$ is spread uniformly over the gripping surface, and is everywhere in the same direction. Then we could apply $F\le \mu N$ to calculate the maximum acceleration for a given gripping force $N$.

Likewise if the applied forces amount to a pure torque, and we know the centre of rotation so that we can find $x$, then we could again assume that this torque is spread uniformly [1] across the face of the gripper but in concentric rings. For a circular gripper we would find the maximum moment of friction is $M \le \frac23 \mu NR$ (see Single Friction Disk Clutch). Even for a rectangular or irregular shaped gripper, it would not be difficult to integrate over its surface to find the maximum torque it can supply by friction.

The difficulty comes when trying to combine translational and rotational forces acting on the gripper. We cannot deal with those forces separately because the friction forces which oppose them are not independent, they are coupled : the resultant friction force at each point on the gripper cannot exceed the static limit.

This situation is addressed for sliding friction in Rotational physics of a playing card. It persists for static friction because the direction of friction can still vary from point to point while its magnitude is limited. In the cited article Frictional coupling between sliding and spinning motion the analysis involves elliptic integrals.

This is not an easy problem to solve.

Note [1] :

How can friction act uniformly across the gripper if a torque is applied to it? Won't points furthest from the axis bear the most load?

Yes, outer points of the gripper furthest from the axis of rotation would have to supply the most torque at first. This is because microscopically the amount of friction force increases with shear displacement until there is slippage, then it is constant (assuming kinetic friction is the same as static).

Outer points reach the limit of friction first then slip microscopically but continue to supply maximum friction. Inner points progressively closer to the axis gradually reach the limit of friction but slip less. Microscopic slippage continues at each radius inwards until the total friction torque equals the applied torque. Friction has reached maximum at every radius except for a disk at the centre, but this radius will be small if the amount of slippage at maximum static friction is small.

The same mechanism also works when applied forces are not purely rotational. There will be microscopic slippage at some points to enable other points to provide more friction. This continues until either (i) the total friction force equals the applied forces and torques, or (ii) every point has reached the static frictional limit so that no more frictional force or torque can be supplied.

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As long as the acting forces do not pass through the barycenter of the object being manipulated, torque of imbalance will arise. These torques will cause turns in the manipulated object as long as the forces of friction and therefore the moment of friction, is not enough to contain the moment generated by the accelerations with which the manipulator moves the object. Therefore it is more a problem of friction.

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  • $\begingroup$ Thanks for your response. I know that the moment of friction limits the acceleration. But my question is how I can calculate the maximum acceleration if the friction force is already defined. How can I calculate the moment of friction? And how to translate the acceleration to an angular momentum if the object accelerates from the center of the moment of friction? $\endgroup$
    – Jasper
    Commented Jun 21, 2018 at 12:19
  • $\begingroup$ This may be more suitable as a comment. $\endgroup$
    – user191954
    Commented Jun 25, 2018 at 3:55
  • $\begingroup$ @Chair The times I answered the questions explicitly, I was advised that it should be shorter. I'm really not understanding the criteria adopted for a good response. $\endgroup$
    – Cesareo
    Commented Jun 25, 2018 at 10:49
  • $\begingroup$ The length usually isn't a solid standard: sometimes a short answer is appropriate, sometimes a long description is needed. More frequently, all the answers to the same question will be of extremely different lengths, each providing a different degree of specificity. The thing is that in this answer, you don't answer the explicit question: How do you calculate the moment of friction. Instead, you gave tips about how to think of the problem, along with a description of what's happening, which is hence more suitable as a comment. $\endgroup$
    – user191954
    Commented Jun 25, 2018 at 11:26
  • $\begingroup$ More generally, regarding the criteria for a good response, you can have any length, just think twice before posting a single-sentence answer: it's very rarely appropriate. Conversely, if your answer is really, really long, you may want to include some bolt text in the beginning which gives a short, 3-sentence summary of what you're trying to explain. Feel free to look at Physics SE meta, there's tonnes of advice there. $\endgroup$
    – user191954
    Commented Jun 25, 2018 at 11:28

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