Why Does a Block Lose Contact with a Frictionless Sphere When Sliding Down?

Please be more considerate in the future. Thank you.In summary, the problem involves a block with mass m on top of a frictionless sphere with radius R. The block is hit and slides down the sphere until it loses contact with the surface. The conditions for losing contact are when the normal force is equal to the centripetal force and when the two accelerations are equal. The angle at which the block loses contact can be found by using the formula for centripetal acceleration and setting it equal to the formula for gravitational acceleration multiplied by the cosine of the angle. The problem can also be solved using conservation of energy, but this method was not allowed in this particular case.
  • #1
Lisa...
189
0
A little block with mass m lies still on the top of a frictionless sphere with radius R. Somebody gently hits the block, causing it to slide down the sphere. The mass loses contact with the sphere when the angle between the positionvector and the vertical equals 0c. The drawing below shows the position of the block on two moments in the movement. The velocity caused by the hit in the beginning is negligible.

http://img453.imageshack.us/img453/6496/sphericalsurface0qu.gif

With this problem I found a couple of answers and I'd like to know if I'm doing it correctly. There are a few questions I don't know how to answer so help would be appreciated very very much!
----------------------------------------------------------------------
a) Express the distance s in R and 0.

s= R * 0 right? That is when 0= in rad. If 0 is in degree it should be s= R (2pi *0 / 360) correct?

b) Which forces work on the block if it's sliding down the sphere? Draw them.

I guess that'll be the gravitationforce and the normal force, drawn below:

http://img173.imageshack.us/img173/4374/sphericalsurface25zz.gif


c) Split the forces in tangential components and perpendicular components on the spherical surface.

I did it this way, could somebody please tell me if I put the angle 0 between the right vectors?:

http://img467.imageshack.us/img467/2815/sphericalsurface35tt.gif


d) Express the centripetal acceleration Ac and the tangential acceleration At in the forces found by b.

If 0 is chosen well in the x-direction (the direction of the tangential acceleration) Fres= Fz,//= Fz sin 0 = m * At. Therefore At= (Fz sin (0))/m

In the y-direction (the direction of the centripetal acceleration) Fres= Fz,|- Fn= Fz cos 0 - Fn= m* Ac. Therefore Ac= (Fz cos(0) -Fn)/m. Correct?

----------------------------------------------------------------------
From here I don't get the problem any longer:

e) At the point where the mass begins losing contact with the surface there are two conditions:

Condition 1: |Ac|= g cos(0)
Condition 2: |Ac|= v^2/R where v= the speed of the block.

Explain why these conditions are set here.

f) Vind the angle 0c where the block begins losing contact with the surface.

Please help! I'd appreciate it very much! Thanks for your effort!
 
Last edited by a moderator:
Physics news on Phys.org
  • #2
a) correct
b) correct
c) correct
You place theta right as:
[tex]\theta = \frac{\pi}{2} - \theta _c = \theta _1[/tex]
Where [itex]\theta _1[/itex] is the angle at the point of the block.
d) looks right
e) This is the essential part of the problem. Give it some more thought. When does the block lose contact?
f) See conditions from e). How can you determine the speed of the block at a certain point?
 
  • #3
e) The block loses contact when the normal force is equal to the centripal force, then there is nothing no keep the block on the sphere. Or in other words, when the 2 accelerations are equal, that explains the two conditions.
 
  • #4
Thank you! I just don't get what you did with theta. I see you used pi/2, but the picture of 1/4 of a circle I drew doesn't mean the block will go off the circle at pi/2...

Concerning e) I know the block loses contact when Fn =0 (do you mean that?), therefore Ac= (Fz cos(0) -Fn)/m becomes Fz cos(0)/m= mg cos(0)/m= g cos(0) and condition 2... well all I know is that that's the formula for the centripetal acceleration But is that all I needed to answer there? I mean at any point on this movement on the sphere there are these two conditions, only g cos(0) would be (Fz cos(0) -Fn)/m ...

About f) well I know v= 2pi s/T, so v= 2pi R 0/T. Substitution in condition 2 gives Ac= (4 pi^2 R 0^2)/T^2 but I don't know what to do now...
 
  • #5
Oh thanks Daniel! I missed your post when I posted mine :) I think I understood e) now...I'm just figuring it out for myself...
 
  • #6
Lisa... said:
Concerning e) I know the block loses contact when Fn =0
That isn't precise, the normal force will always be bigger than 0 as long as the theta_c is bigger than zero. But even if the normal force isn't zero, the block will lose contact when the sum of the forces on the block is zero.
EDIT: Sorry Lisa, I just missed your post as I was posting mine:smile:
 
  • #7
Use conservation of energy. The potential energy at the top is mgR, right? Now find the potential energy at the point it loses contact, as well as the kinetic energy. It will be useful to note that:

[tex]a_c=\frac{v^2}{R}=mgR\cos{\theta_c}[/tex]

...now do a little algebra and you're done.
 
  • #8
apmcavoy said:
Use conservation of energy. The potential energy at the top is mgR, right? Now find the potential energy at the point it loses contact, as well as the kinetic energy. It will be useful to note that:
[tex]a_c=\frac{v^2}{R}=mgR\cos{\theta_c}[/tex]
...now do a little algebra and you're done.

That's a bit of a problem... I also thought of that way, but my teacher told me I need to do it without using any energy laws, because he wants me to know to work with other laws... I know it REALLY sucks...
 
  • #9
Lisa... said:
Thank you! I just don't get what you did with theta. I see you used pi/2, but the picture of 1/4 of a circle I drew doesn't mean the block will go off the circle at pi/2...
I just showed that your thinking in placing theta where you placed it was correct. pi/2 has nothing to do with the point where there's no longer contact. It's merely a right angle.

daniel_i_l said:
e) The block loses contact when the normal force is equal to the centripal force, then there is nothing no keep the block on the sphere. Or in other words, when the 2 accelerations are equal, that explains the two conditions.
Although correct, I don't quite appreciate you cramming in and ruining the thought process for the OP. This is especially irritating as you posted before the OP had responded to my reply.
 
  • #10
Sorry Päällikkö.
 
  • #11
So if I understood it correctly the answer to e is:

'The block gets off the sphere when Fn= Fz,|=Fmpz therefore if Fn= mg cos 0 = mv^2/r and (according to F=m*a) when a= mg cos 0/m= g cos 0 needs to equal a= (mv^2/r)/m= v^2/r'
 
  • #12
I think I still don't get it, when Fn= Fz,| there is no Fmpz and ac=0 therefore ? Why does it need to equal g cos(0) and v^2/R ?
 
  • #13
And what about f... I still don't know from where to start :S...
 
  • #14
Lisa... said:
I think I still don't get it, when Fn= Fz,| there is no Fmpz and ac=0 therefore ? Why does it need to equal g cos(0) and v^2/R ?
What is Fmpz?Fc = Fz,| - Fn
c indicating centripetal.

When is there no contact?
 
  • #15
Oops sorry :D Fmpz= Fc :D My book is Dutch and calls the centripetal force 'middelpuntzoekende kracht' (Fmpz)
 
  • #16
What I ment is when there is no contact Fz,| = Fn and Fc= 0 therefore... but why is ac= g cos 0 and v^2/r ? If Fc=0 ac needs to be 0 too right?
 
  • #17
Lisa... said:
What I ment is when there is no contact Fz,| = Fn and Fc= 0 therefore... but why is ac= g cos 0 and v^2/r ? If Fc=0 ac needs to be 0 too right?
No.
When there's no contact, there's no supporting force from the surface.
Thus Fn = 0.

Lisa... said:
Oops sorry :D Fmpz= Fc :D My book is Dutch and calls the centripetal force 'middelpuntzoekende kracht' (Fmpz)
Ok :smile:. Maybe I should add some Finnish terms to add to the confusion :smile:.

EDIT: As a sidenote, using (i)tex-tags or sub and sup -tags clarifies the notation quite a bit. I now know what you mean by different markings, but just a hint for future posts, as I usually rather reply to posts where the problem and work are clearly stated.
 
Last edited:
  • #18
Ah well in that case my original thought was correct right?:
Lisa... said:
Concerning e) I know the block loses contact when Fn =0 (do you mean that?), therefore Ac= (Fz cos(0) -Fn)/m becomes Fz cos(0)/m= mg cos(0)/m= g cos(0) and condition 2... well all I know is that that's the formula for the centripetal acceleration But is that all I needed to answer there? I mean at any point on this movement on the sphere there are these two conditions, only g cos(0) would be (Fz cos(0) -Fn)/m ...
 
  • #19
Päällikkö said:
No.
When there's no contact, there's no supporting force from the surface.
Thus Fn = 0.


Ok :smile:. Maybe I should add some Finnish terms to add to the confusion :smile:.

EDIT: As a sidenote, using (i)tex-tags or sub and sup -tags clarifies the notation quite a bit. I now know what you mean by different markings, but just a hint for future posts, as I usually rather reply to posts where the problem and work are clearly stated.

Thanx for the tip! I didn't know it was possible! I'll surely use them in the future!
 
  • #20
Lisa... said:
Ah well in that case my original thought was correct right?:
Yes.

I mean at any point on this movement on the sphere there are these two conditions, only g cos(0) would be (Fz cos(0) -Fn)/m ...

I'm not quite sure what you meant here, though.
 
  • #21
Nvm I think I got it... now I only need to solve f. I know v= 2pi s/T, so v= 2pi R 0/T. Substitution in condition 2 gives Ac= (4 pi 2 R 02 )/T2 but I don't know what to do now...
 
  • #22
What's f?

That's not quite the way I'd try to solve the problem. Try energy conservation.
 
  • #23
I cannot use energy conservation :( My teacher said he wants me to solve the problem with any law, as long as it aren't energy conservation laws...
 
  • #24
Btw f is (question f): f) Find the angle 0c where the block begins losing contact with the surface.
 
  • #25
Lisa... said:
I cannot use energy conservation :( My teacher said he wants me to solve the problem with any law, as long as it aren't energy conservation laws...
Ouch...

Lisa... said:
Nvm I think I got it... now I only need to solve f. I know v= 2pi s/T, so v= 2pi R 0/T. Substitution in condition 2 gives Ac= (4 pi 2 R 02 )/T2 but I don't know what to do now...
What happened here?
 
  • #26
What do you mean by that? I substituted the formula for the speed into the acceleration formula, but I don't know if that's the right way to get to an answer...
 
  • #27
?
..........
 

Related to Why Does a Block Lose Contact with a Frictionless Sphere When Sliding Down?

1. What is circular motion?

Circular motion is a type of motion where an object moves in a circular path around a central point or axis. This can occur in both two-dimensional and three-dimensional space.

2. What makes a circular motion problem "weird"?

A weird circular motion problem is one that presents a unique or unusual scenario, often involving multiple objects or forces acting on the system. These problems require creative thinking and may have unexpected solutions.

3. How do you approach solving a weird circular motion problem?

The key to solving any circular motion problem is to first identify all the forces acting on the system and then use Newton's laws of motion to analyze the motion of the objects involved. It is also helpful to draw a free-body diagram and use equations such as centripetal force and tangential velocity to find the solution.

4. What are some real-life examples of weird circular motion?

Some examples of weird circular motion in everyday life include a car turning a corner, a roller coaster looping upside down, and a satellite orbiting around the Earth. These scenarios involve complex forces and motions that can be analyzed using circular motion principles.

5. How can understanding circular motion be useful in other fields of science?

Circular motion is a fundamental concept in physics and is used to explain various phenomena in other fields of science such as astronomy, biology, and engineering. Understanding circular motion can also help in designing and analyzing machines and structures that involve circular motion, such as turbines or amusement park rides.

Similar threads

  • Introductory Physics Homework Help
Replies
12
Views
2K
  • Introductory Physics Homework Help
Replies
10
Views
5K
  • Introductory Physics Homework Help
Replies
9
Views
3K
  • Introductory Physics Homework Help
Replies
14
Views
1K
  • Introductory Physics Homework Help
Replies
13
Views
3K
  • Introductory Physics Homework Help
Replies
6
Views
1K
  • Introductory Physics Homework Help
Replies
5
Views
2K
  • Introductory Physics Homework Help
Replies
9
Views
2K
  • Introductory Physics Homework Help
Replies
4
Views
7K
  • Introductory Physics Homework Help
Replies
2
Views
12K
Back
Top