Movement between two blocks

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Homework Statement
Block A with mass 3.5kg rests on block B with mass 4kg. Block B sits on a horizontal frictionless surface. The static friction coefficient of the two blocks 0.4. Horizontal force P is applied to block A. What is the largest value of force P can have and the blocks move together with the same acceleration.
Relevant Equations
ff=un
N=m*g
Ok so first I drew the blocks on top of each other and found both normal forces. The normal force acting on block A (Na) is 34.335 N, and the normal force acting on block B (Nb) is 73.575 N. Because P is acting on A, you can find the friction force by multiplying the friction coefficient (0.4) by the normal force of A. Ff = 13.734 N. Except it's wrong. It's also not the friction force by doing 0.4*Nb. It's also not 0.4*(Nb-Na). Even my tutor was stumped. The answer it gives you is 25.7 N. Following the Ff=un, that'd mean N=64.25.
So either, we are using the wrong friction coefficient, but it doesn't give us the kinetic one.
Or, we found the normal forces wrong. No idea how that would work.
Or, we aren't finding the Friction Force correctly.
Any help would be appreciated.
 
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When you multiply the coefficient of static friction by the normal force you have the maximum force of static friction, i.e. the value of ##f_s## at which sliding occurs. The force of static friction is "whatever is necessary to provide the observed acceleration of the system." Here the observed acceleration is provided by force P.
  1. What is the observed acceleration of the two-block system?
  2. What is the net force on block A that provides this observed acceleration?
  3. How large can P become before the blocks stop moving as one and slide relative to each other?
 
kuruman said:
When you multiply the coefficient of static friction by the normal force you have the maximum force of static friction, i.e. the value of ##f_s## at which sliding occurs. The force of static friction is "whatever is necessary to provide the observed acceleration of the system." Here the observed acceleration is provided by force P.
  1. What is the observed acceleration of the two-block system?
  2. What is the net force on block A that provides this observed acceleration?
  3. How large can P become before the blocks stop moving as one and slide relative to each other?
Ok, so my Ff that I got is the minimum force required to move the blocks at all? But then I don't understand how I'm supposed to solve for anything else if I'm not given any other values?
 
CassLovesKinematics said:
Ok, so my Ff that I got is the minimum force required to move the blocks at all? But then I don't understand how I'm supposed to solve for anything else if I'm not given any other values?

The two blocks together lie on a frictionless surface. So even an infinitesimal amount of force will cause the blocks (still together) to move along the frictionless surface a little (even if very slowly).


To help wrap your head around this problem, here are some hints:

(I.) Forget the given mass of block B for a second. Just for the moment, pretend that the mass of Block B is unknown. Don't worry we can put the known value back in later. But for the moment, pretend you don't know it. But keep the same coefficients of friction (i.e., 0.4 between the masses, and a frictionless surface between the ground and block B). No math on this one. Just ask yourself what you would expect if block B's mass were an extreme value.

How would the problem change if mass B were really large, say infinitely large?

How would the problem change if mass B were really small. Like say, what if mass A was made of lead, and mass B of styrofoam?

You can use this gathered intuition later as a sanity check for equation that brings about the final answer.

(II.) When analyzing your free body diagrams (FBDs), don't forget that this is a dynamics problem, not a statics problem. The sum of all forces do not equal 0. Rather the sum of all forces, [itex]\Sigma_i Fi = a \cdot \Sigma _j m_j[/itex], assuming that both blocks have the same acceleration*. This idea applies to individual blocks within the system too. So what's the overall acceleration of the system as a function of both masses and the applied force? Now do a FBD of block A. (intermediate hint: What must be the reactive force be on block A from block B, now that you know block B's acceleration?)

*[Edit: however, the frictional force applied from block B to block A must be equal-&-opposite the sum of all forces on block B, of course, because of Newton's 3rd law, and because block B is lying on a frictionless surface.]
 
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CassLovesKinematics said:
Ok, so my Ff that I got is the minimum force required to move the blocks at all? But then I don't understand how I'm supposed to solve for anything else if I'm not given any other values?
You are missing the point that "Block B sits on a frictionless surface." If P were, say, one millionth of ##\mu_sN## would the blocks accelerate or not?

Another way to look at it is to pretend that the blocks are glued together with super glue so there is no sliding. What would their acceleration be in this case?

Now make the glue so weak that the contact is frictionless. What happens then? Answer: Block A will accelerate with acceleration ##P/m_A## and block B will not move.

Imagine now that the glue strength is between "super" and "frictionless." What force accelerates block B? Certainly not P because P acts on block A.
 
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Two unknowns: the force ##P## and system acceleration ##a## and two equations: projections of Newton's second law onto the horizontal axis for each body.