In summary, the conversation discusses a problem involving a block of mass m attached to a spring with a force constant k, and another block of mass 2m placed a distance x/2 from the equilibrium point. After the spring is released, the blocks collide inelastically and stick together. The question asks for the distance (Δx) the blocks will slide beyond the collision point. The key stage in the motion after the block is released is the inelastic collision, and the kinetic energy is not conserved during this collision. The question can be solved by using conservation of energy and setting up equations for the initial and final potential energies.
  • #1
REVIANNA
71
1

Homework Statement


problems_MIT_boriskor_BKimages_10-mass-spring-two-block-collision.png
[/B]
A block of mass m is attached to a spring with a force constant k, as in the above diagram. Initially, the spring is compressed a distancex from the equilibrium and the block is held at rest. Another block, of mass 2m, is placed a distance x/2 from the equilibrium as shown. After the spring is released, the blocks collide inelastically and slide together. How far (Δx) would the blocks slide beyond the collision point? Neglect friction between the blocks and the horizontal surface.

The Attempt at a Solution


At first I thought that this question is very easy.But now I don't know how I should break the problem up such that I can write neat equations for momentum and energy conservation.
should I consider the intermediate position when m reaches its equilibrium position and its energy is purely kinetic ? the question asks for delx but the equations contain only velocity terns and why will it even stop post collision there is no friction?

edit:
I understood that it will stop because it would have a leftward velocity and would eventually crash into the spring compressing it by delx
 
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  • #2
I wouldn't worry about the equilibrium point. So, what is the key stage in the motion after the block is released?
 
  • #3
PeroK said:
what is the key stage in the motion after the block is released?
the inelastic collision .
but the kinetic energy is not conserved during such a collision.
so should I write an equation just before the collision and will m's velocity be the same at x/2 (pre collision) as it was at position x
 
  • #4
You're forgetting that the spring will pull the block back after the equilibrium point.
 
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  • #5
PeroK said:
spring will pull the block back after the equilibrium point.
actually I thought about the back and forth motion but it seemed too complicated so I thought that the block detaches itself at x

so How should I think?
at where it compresses to :we consider the P.E there ?
Or should I read the chapter on SHM for this ?
 
  • #6
REVIANNA said:
edit:
I understood that it will stop because it would have a leftward velocity and would eventually crash into the spring compressing it by delx
Not sure what you are saying there, but it doesn't sound right. You do not need to get to the point where anything has a leftward velocity. You are only interested in how far the blocks get before anything goes to the left.
The question is a little unclear. Do the blocks stick together or merely collide without bouncing at all? I think it means they stick together, otherwise they would start to separate immediately, even though there is no bounce.
 
  • #7
REVIANNA said:
the inelastic collision .
but the kinetic energy is not conserved during such a collision.
so should I write an equation just before the collision ...
Yes.
... and will m's velocity be the same at x/2 (pre collision) as it was at position x
No.

Use conservation of energy to determine the velocity of block of mass m immediately before the collision.
 
  • #8
haruspex said:
means they stick together
yes they do.

I am not understanding the situation here @PeroK said that the block will not detach itself from the spring at x(the equilibrium) so it will go back and forth until it hits 2m
than it will stick to 2m and go "leftwards" causing delx compression which we are supposed to figure out.
what is going on? what what point should I think about the energies?
 
  • #9
REVIANNA said:
yes they do.

I am not understanding the situation here @PeroK said that the block will not detach itself from the spring at x(the equilibrium) so it will go back and forth until it hits 2m
than it will stick to 2m and go "leftwards" causing delx compression which we are supposed to figure out.
It won't go back and forth before hitting 2m. If 2m were not there, how far would it go before going leftwards at all?
The question asks how far they go "beyond the collision point". That is, how far before reversing direction.
 
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  • #10
REVIANNA said:
yes they do.

I am not understanding the situation here @PeroK said that the block will not detach itself from the spring at x(the equilibrium) so it will go back and forth until it hits 2m
than it will stick to 2m and go "leftwards" causing delx compression which we are supposed to figure out.
what is going on? what what point should I think about the energies?
The problem statement says that the block of mass m is attached to the spring.
 
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  • #11
REVIANNA said:
actually I thought about the back and forth motion but it seemed too complicated so I thought that the block detaches itself at x

so How should I think?
at where it compresses to :we consider the P.E there ?
Or should I read the chapter on SHM for this ?
It says the block is attached to the spring. If it wasn't attached it would be jettisoned at the equilibrium point. But, it is attached so it stays attached.

Although you may want to calculate the velocity at the collision you don't have to.

As Haruspex says, the blocks must stay stuck together after the collision.
 
  • #12
haruspex said:
That is, how far before reversing direction.
so m will go beyond x , collide with m2 at x/2 , stick with it, and then they both move forward .
we have to calculate how far before spring pulls them back


I wrote an equation with equilibrium as 0 position
and equating the initial potential energy of m (##0.5kx^2##)and the final potential energy of 3m (##0.5k((x/2)+(Δx))^2##)
but I don't get the correct answer on solving this quadratic equation
 
  • #13
REVIANNA said:
so m will go beyond x , collide with m2 at x/2 , stick with it, and then they both move forward .
we have to calculate how far before spring pulls them backI wrote an equation with equilibrium as 0 position
and equating the initial potential energy of m (##0.5kx^2##)and the final potential energy of 3m (##0.5k((x/2)+(Δx))^2##)
but I don't get the correct answer on solving this quadratic equation
For the inelastic collision:
There will be a loss of kinetic energy. Right?
 
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  • #14
first I considered the situation b/w the launch and the collision
here the mechanical energy is conserved.
It gets converted from purely potential to partly kinetic and partly potential(because it moves past the equilibrium point )
I used this to find the velocity of m right before the collision

during the INELASTIC collision the momentum is conserved(because of negligible internal forces) and energy is not
I found the velocity of (now) 3m right after the collision

then again 3m moves further out until it gains max potential energy
we know that the post collision -part K.E and part P.E gets converted wholly into potential energy

the displacement after the the collision gave me the answer . thanks everyone!
 

Related to Energy and momentum conservation

What is energy conservation?

Energy conservation is the principle that energy cannot be created or destroyed, but can only be converted from one form to another. This means that the total amount of energy in a closed system remains constant over time.

What is momentum conservation?

Momentum conservation is the principle that the total momentum of a closed system remains constant over time. This means that the combined mass and velocity of all objects in the system will not change, unless acted upon by an external force.

How are energy and momentum related?

Energy and momentum are related through the conservation of mass and the conservation of energy. When energy is conserved, momentum is also conserved since energy is a function of mass and velocity. This means that any changes in energy will result in corresponding changes in momentum.

What are some examples of energy conservation in everyday life?

Some examples of energy conservation in everyday life include turning off lights and electronics when not in use, using energy-efficient appliances, carpooling or using public transportation, and using renewable energy sources such as solar or wind power.

Why is it important to conserve energy and momentum?

Conserving energy and momentum is important for several reasons. It helps to reduce our impact on the environment, as well as save money on energy costs. It also ensures the sustainability of our resources for future generations, and promotes efficiency and innovation in technology and industry.

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