• If you are citizen of an European Union member nation, you may not use this service unless you are at least 16 years old.

  • You already know Dokkio is an AI-powered assistant to organize & manage your digital files & messages. Very soon, Dokkio will support Outlook as well as One Drive. Check it out today!

View
 

Gauss gun energy bar representation

Page history last edited by Mark Eichenlaub 6 years, 5 months ago

6.4.P12

 

In a molecule, the atoms are bound together by interactions whose effect is described by a potential energy.  (See Chemical bonding) As a model of this we consider "four atoms bound together" -- a magnet and three steel spheres, shown in the figure at the right. The magnet exerts an attractive force on each of the steel spheres that falls off rapidly as a function of distance (i.e., the attraction is stronger when the sphere is closer).

 Just looking at the system consisting of the strong magnet and the steel spheres labeled 1, 2, and 3, I would conjecture that "sphere 1 is the most strongly bound, sphere 2 is less strongly bound, and sphere 3 is weakly bound." 

 

If an external metal sphere (labeled "0" collides with this molecule, it is strongly attracted.  Watch the video of what happens below.

 

If we think of this as a collision between the two mechanical objects, it is a super-elastic collision*, that is, the kinetic energy of the two objects after the collision is greater than the kinetic energy of the two objects well before the collision.  Let's analyze where the energy comes from. You can assume mechanical energy is conserved in your analysis.

 

We will assume that our magnet and track are attached to a heavy table and the combination of magnet+table doesn’t move significantly (although the spheres can move). This means we can ignore momentum conservation since the heavy table can carry away excess momentum without it moving observably. All our motions are horizontal so we ignore gravity.

 

If a sphere is put within a few inches of the magnet it sticks to the magnet. We can describe the interaction of the spheres with the magnet in terms of a potential energy, U. Take the energy of a sphere to be 0 when it is at rest and far from the magnet.  Three situations, A, B, and C, are shown at the right. We describe position in our system using the x coordinate shown with the zero taken to be in the center of the magnet.  

A. If you try to pull the sphere away from the magnet in case A, you will find that it is held by a strong attractive force that gets weaker as the sphere gets farther from the magnet. A force is no longer detectable once you are more than 30 cm away. On the graph at the right sketch the potential energy of the sphere-magnet system as a function of x where x represents the position of Sphere 1. Your graph should correctly represent the qualitative features of the interaction.    

At the left is shown a different kind of representation – an energy bar chart. This chart uses bars to identify the energy of the various components of the system. The horizontal axis is for position. A bar at a certain part of the x-axis shows the energy of a component of the system at that same x-value. The vertical axis is an energy axis. The height of the bar shows the energy of a component of the system, and can be positive or negative.

 

The position of the magnet is x=0, where the axes cross. The leftmost chart represents sphere 0 moving on the left of the magnet and shows its KE. The chart at the right represents the potential energy of sphere 1 and the magnet (shown attached to the position of sphere 1).  So the left bar might represent the KE of sphere 0 in situation C, while the right one represents the PE of the magnet and sphere 1 in situations A, B, or C.

 

B. In situation B, sphere 3 is fairly easy to remove from the complex, sphere 2 harder, and sphere 1 very difficult. On a chart like the one at the right, assuming that everything is stationary (and ignoring any possible potential energies from interactions between the spheres themselves) draw bars representing the various energies (for each sphere) in situation B.    

C. In situation C, sphere 0 is released about 30 cm from the magnet with a small KE. It slowly speeds up until it slams into the magnet going fast and sticks to the magnet. As a result, sphere 3 flies off to the right at a high speed. In the charts below, draw bar charts representing the energies in the initial state and after the collision when sphere 3 is moving away at a distance of 30 cm. Draw your diagrams carefully to represent any important relations among the energies. Explain what considerations you used to draw your diagrams. 

 

D. To see how this works, choose arbitrary numbers like integers to represent each of the energies -- ignoring units. For example we might call the blue KE bar in the figure at the left of part A, "4", and the red PE bar in the figure as "-10". Use your numbers to write the total energy in the initial situation and the total energy in the final situation, choosing numbers that both represent the relative scale of the bars you drew and add up correctly to show energy conservation.

 

Now answer the question: In this reaction a particle came in at a low kinetic energy and another went out at a high kinetic energy. Where did the extra energy come from?

 

E. To what extent do you think that this is a decent analogy for an exothermic chemical reaction -- one in which some energy is made available to do other things as a result of the reaction? Explain why you think so.

 

 

Joe Redish and Dave Buehrle 4/17/14

 

Comments (0)

You don't have permission to comment on this page.