Frictional Forces, Static Friction

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SUMMARY

The discussion centers on the mechanics of static friction between two blocks, A and B, with masses mA and mB, respectively. The critical point is that Block A will begin to slide out from under Block B when the applied force exceeds μs(mA + mB)g, where μs is the coefficient of static friction. The static friction force acts in the direction of the applied force, allowing Block B to accelerate alongside Block A until the maximum static frictional force is reached. Understanding the relationship between normal force, static friction, and Newton's laws is essential for solving the problem.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Knowledge of static friction and its coefficient (μs)
  • Familiarity with normal force calculations (Normal Force = mB*g)
  • Ability to apply equations of motion to multiple objects
NEXT STEPS
  • Study the concept of static friction and its role in multi-body systems
  • Learn how to apply Newton's second law to systems with multiple masses
  • Explore the derivation of frictional force equations in physics
  • Investigate real-world applications of static friction in engineering scenarios
USEFUL FOR

Students studying physics, particularly those focusing on mechanics and friction, as well as educators seeking to clarify concepts related to static friction and motion dynamics.

eprparadox
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Homework Statement


Block A, with mass mA, is initially at rest on a horizontal floor. Block B, with mass mB, is
initially at rest on the horizontal top surface of A. The coefficient of static friction between the two blocks is μs. Block A is pulled with a horizontal force. It begins to slide out from under B if the force is greater than:
A. mA*g
B. mB*g
C. μs*mA*g
D. μs*mB*g
E. μs(mA +mB)g
Ans: E

Homework Equations


Ff(static, max) = μs*NormalForce;


The Attempt at a Solution


So the answer is already given as E, but I really want to understand this.

I'm confused on a couple of things. So if we pull on A too hard, then B will fall out behind it. Does this mean that the force of static friction is acting in the direction of the applied force F? And the normal force acting on mass B is just mB*g correct?

That's all I got. I'm a little stuck from there. Any help would be great. Thanks a lot ahead of time.
 
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eprparadox said:
So the answer is already given as E, but I really want to understand this.

I'm confused on a couple of things. So if we pull on A too hard, then B will fall out behind it. Does this mean that the force of static friction is acting in the direction of the applied force F?
Yes, the static friction is acting on block B, and it is in the same direction as the applied force F (where F is attached to block A). And it makes sense if you think about it. It has to be acting in the same direction, otherwise block B wouldn't be accelerating in the same direction as block A.
And the normal force acting on mass B is just mB*g correct?
Yes, that's right. :approve:
That's all I got. I'm a little stuck from there. Any help would be great. Thanks a lot ahead of time.
Well, you seem to already have most everything you need. You know what the normal force acting on B is. So you can find the maximum static frictional force that can occur too (which is the normal force times μs).

Using Newton's second law (FB = mBa), solve for the acceleration a, of block B.

Invoke Newton's second law one more time to solve for the total applied force F, after realizing that blocks A and B are both accelerating at same rate a. :wink:

(I'll leave all the appropriate substitutions up to you.)
 

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