Work-energy v.s. impulse-momentum bar charts

In summary, the text argues against using a work-energy bar chart to represent the collision between Spiderman and Mary Jane because it is not possible to determine the lost kinetic energy.
  • #1
otownsend
12
0
Member advised to use the formatting template for all homework help requests
My question unfortunately does not fit in the Homework template, so I hope this is okay.

I attached a question below which involves multiple parts using the concepts related to energy, work, impulse, and momentum. Under the "Simplify and Diagram" section (you will notice it is in bold text), I want to better understand why Part II cannot be understood with a work-energy bar chart. The texts reasoning for why it is not a good idea to use a work-energy bar charts is because "we don't have a way to independently determine internal energy change". Why is this the reason? Isn't the reason more that we want to find the velocity of Jane and Spiderman after the collision occurred and using a work-energy expression (in this case the work energy expression would be something like kinetic energy = change in internal energy) wouldn't allow us to determine this velocity?

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IMG_20181112_223421.jpg
 

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  • #2
otownsend said:
kinetic energy = change in internal energy
Did you mean that? Which kinetic energy, exactly?
 
  • #3
haruspex said:
Did you mean that? Which kinetic energy, exactly?
Well there's the kinetic energy coming from the collision, which then gets changed into internal energy (since its an inelastic collision)
 
  • #4
otownsend said:
Well there's the kinetic energy coming from the collision, which then gets changed into internal energy (since its an inelastic collision)
That's the lost KE. But in that case you seem to be saying the same thing as the text, that we don't know what the lost KE is because we don't know the gained internal energy.
 
  • #5
otownsend said:
The texts reasoning for why it is not a good idea to use a work-energy bar charts is because "we don't have a way to independently determine internal energy change".
In a perfectly inelastic collision the "internal energy change" is (in practise) crash energy lost. For example in a car accident it would be all the energy dissipated as the cars crumple up and deform along with various other forms of irreversible energy dissipation. So - yes - it can't be independently determined but one can use conservation of momentum to determine energy before and after collision and hence the difference. It turns out that the energy loss (internal energy change in your textbook's lexicon) in a perfectly inelastic collision (collide and coalesce collision) is given by the following relatively simple equation: $$ΔE=½μΔv^2$$ where μ is the reduced mass of the colliding objects: $$μ=\frac{m_1m_2}{m_1+m_2}$$ and Δv is their relative velocity along the line of collision. In this case $$Δv=\sqrt{2gh_1}$$ as shown in your textbook.

Using this equation you could have just one energy bar chart showing Ui and Uf with the W column showing the inelastic collision loss per formula as Spiderman swoops to the rescue!

Edit: not quite true - I guess you would still need the first work-energy bar chart to determine ##Δv=\sqrt{2gh_1}##.
 
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  • #6
Just to be annoyingly pedantic and almost entirely unhelpful :smile:, note that according to the supplied diagram Spiderman will not encounter Mary Jane at the bottom of his arc:

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  • #7
gneill said:
Spiderman will not encounter Mary Jane at the bottom of his arc:
Which, at that speed, will be a relief for all concerned.
 
  • #8
haruspex said:
Which, at that speed, will be a relief for all concerned.
Very much :smile:!
 
  • #9
gneill said:
according to the supplied diagram Spiderman will not encounter Mary Jane at the bottom of his arc:
In the interests of appropriate drama (and Science!), I think we have to assume that Mary Jane - with precious seconds ticking away - rushes to the right hand side of the platform and launches herself into the air just as Spiderman swoops in ...
 
  • #10
neilparker62 said:
In the interests of appropriate drama (and Science!), I think we have to assume that Mary Jane - with precious seconds ticking away - rushes to the right hand side of the platform and launches herself into the air just as Spiderman swoops in ...
...and smacks into her at 50 kph.
 

1. What is the difference between work-energy and impulse-momentum bar charts?

The main difference between work-energy and impulse-momentum bar charts is the physical quantities represented. In work-energy bar charts, the bars represent the work done on an object, while in impulse-momentum bar charts, the bars represent the impulse exerted on an object.

2. How are work-energy and impulse-momentum related?

Work-energy and impulse-momentum are related through the work-energy theorem, which states that the net work done on an object is equal to the change in its kinetic energy. This means that the area under the work-energy bar chart is equal to the change in kinetic energy, and the area under the impulse-momentum bar chart is equal to the change in momentum.

3. Can both work-energy and impulse-momentum bar charts be used to solve problems?

Yes, both work-energy and impulse-momentum bar charts can be used to solve problems involving the motion of objects. Work-energy bar charts are typically used for problems involving conservative forces, while impulse-momentum bar charts are used for problems involving non-conservative forces or collisions.

4. How do you interpret the height and width of bars in work-energy and impulse-momentum bar charts?

In both work-energy and impulse-momentum bar charts, the height of the bars represents the magnitude of the physical quantity (work or impulse), while the width of the bars represents the time interval over which the physical quantity is applied. This can help in visualizing the relationship between the physical quantities and the motion of the object.

5. Are there any limitations to using work-energy and impulse-momentum bar charts?

While work-energy and impulse-momentum bar charts can be useful tools for solving problems, they do have some limitations. They are only applicable for one-dimensional motion and do not account for rotational motion. Additionally, they can only be used for problems where the forces are constant and the motion is uniform.

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