Force (object is suspended connected to a block on table and pulled up)

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The discussion revolves around a physics problem involving two masses connected by a cord over a pulley, with a force applied at an angle to one mass on a rough surface. Participants focus on creating a free body diagram and applying Newton's second law to derive equations for acceleration and tension in the cord. Key points include the need to account for the angle of the applied force when calculating the normal force and friction, as well as the relationship between the two masses' accelerations. The final equations for acceleration and tension are derived by combining the forces acting on both masses. The discussion emphasizes the importance of correctly incorporating the normal force and friction in the calculations.
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Homework Statement



A block of mass m1 on a rough horizontal surface is connected to a ball of mass m2 by a lightweight cord over a lightweight frictionless pulley as shown. A force of magnitude F at an angle theta with the horizontal is applied to the block. The coefficient of friction between the block and surface is \mu_k

a.) draw a free body diagram of the 2 masses

b.) use Newton's dynamic equation to determine the magnitude of the acceleration of theh 2 objects in terms of their masses, F, theta, and \mu_k

c.) what is the tension in the cord
http://img518.imageshack.us/img518/1023/picture1dn4.png

Homework Equations



F= ma

Ffk= uk* Fn

and a Newton's dynamic equation? ==> what is that exactly??

The Attempt at a Solution



a)for the free body diagram

http://img484.imageshack.us/img484/2900/90134448jw8.th.jpg

b) how would I do this question...not sure and I'm stuck after the free body diagram...hm..


c) I guess I would need to solve part b to get part c


~I do know that they both have the same accelration but how would I know if the total forces \sum Fx= 0?

I need help please..
 
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~christina~ said:
and a Newton's dynamic equation? ==> what is that exactly??
That's Newton's 2nd law.

One problem with the FBD: That applied force F is at an angle, not horizontal.

Analyze the forces parallel to the direction of motion for each block and apply Newton's 2nd law. You'll get two equations--one for each mass--that you'll solve together for the two unknowns: the acceleration and tension.
 
I was wondering why I don't analyze the horizontal component of the block but I think it's b/c the total forces = 0 but...this is what I got.

for m2 (only movement in y direction)
\sum Fx= 0
\sum Fy= T- m_2 g= m_2 ay

for m1 (block)
\sum Fx= max= Fcos theta- (T+ \muk m1g)
\sum Fy= may= Fsin theta + N- mg= 0

Well I just wanted to check first...
 
~christina~ said:
for m2 (only movement in y direction)
\sum Fx= 0
\sum Fy= T- m_2 g= m_2 ay
Good. I would just call the acceleration "a".

for m1 (block)
\sum Fx= max= Fcos theta- (T+ \mu_k m1g)
Careful here: What's the normal force? Again: call the acceleration "a".
\sum Fy= may= Fsin theta + N- mg= 0
Good. Use this to figure out N.
 
for m2 (only movement in y direction)
\sum Fx= 0
\sum Fy= T- m_2 g= m_2 a

for m1 (block)
\sum Fx= ma= Fcos theta- (T+ \muk m1g) => was this incorrect (see below for my correction)??

~I do know that that is the Fx component right? but I guess I need to incorperate the N?


\sum Fy= ma= Fsin theta + N- mg= 0
from the Fy

N= mg - Fsin theta


I think that since the Ffk = uk*FN
then the equation on the top for the Fx wouldn't be uk* m1g since the normal force is lighter so it would be instead

\sum Fx= ma= Fcos theta- (T+u_k (m_1g- Fsin theta))


Is it fine now?

I guess whenever I have to find the x component of the force when there is friction I need to incorperate the normal force the angle it is being pulled at if there is a angle so that the normal force is not just m*g right?
 
~christina~ said:
Is it fine now?
Yes, all better.

I guess whenever I have to find the x component of the force when there is friction I need to incorperate the normal force the angle it is being pulled at if there is a angle so that the normal force is not just m*g right?
Right. Friction depends on the normal force, which may or may not equal the weight of the object, depending upon the situation.
 
\sum Fy= T- m_2 g= m_2 a

\sum Fy= ma= Fsin theta + N- mg= 0
from the Fy

N= mg - Fsin theta

\sum Fx= ma= Fcos theta- (T+u_k (m_1g- Fsin theta))

________________________________________________________________
but how would I find the part b) which is...

b) b.) use Newton's dynamic equation to determine the magnitude of the acceleration of the 2 objects in terms of their masses, F, theta, and \mu_k

(I'm not sure what they want)

would it be adding the 2 equation??

the first object and second object's forces like this?

\sum Fy= T- m_2 g= m_2 a

\sum Fx= ma= Fcos theta- (T+u_k (m_1g- Fsin theta))

so adding them I get..
+ T- mg= m2a
+ Fcos theta - T- uk (m1g- Fsin theta) = m1a
______________________________________

Fcos theta- m2g- uk(m2g- Fsin theta)= (m1 + m2)a

a= (Fcos theta- m2g - uk(m2g- Fsin theta))/ m1+ m2
Is this what they want?


Assuming it is...
for part c.) I need to find

c.) tension in cord..

I think that I would plug this into a original equation while using the acceleration I found...

\sum Fy= T- m_2 g= m_2 a

T= m2a + m2g

substituting a

T= m2( (Fcos theta- m2g - uk(m2g- Fsin theta))/ m1+ m2) + m2g


I think this is okay but not sure..
 
Looks good to me!

As a practical matter, I would solve for a and then plug the numerical value into the other equation to get T.
 
Oh okay..I would plug in the numbers if I had numbers given...

I usually find it challenging to not have numbers though..

Thanks for your help Doc Al !
 
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