Particle in a box question in classical mechaincs

In summary, the lecturer is explaining that if the particle is moving inside of a box at a certain energy, then it has less momentum than if the particle is not inside of the box. However, if the particle is moving outside of the box, then it has more momentum.
  • #1
Taylor_1989
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Hi guys, I am having an issue with what my lecture is saying in these slides, I have attched my slides below.
upload_2017-12-15_21-37-16.png

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upload_2017-12-15_21-38-12.png


Here is my issue. I am very confused by the ##E<\Delta ## Beacuse I can't see how this has any momentum as it would produce an imagery number. And ye say that ##E<\Delta ## cannot be a solution yet on these diagrams he show the particle has momentum, at E=0 which can't be correct. I know I have this back to front, because he also mentions that at ##E>\Delta ## that is has less momentum than but I just can't see how, could someone please explain to me what my lecture is conveying here.
 

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  • #2
Taylor_1989 said:
Here is my issue. I am very confused by the ##E<\Delta ## Beacuse I can't see how this has any momentum as it would produce an imagery number. And ye say that ##E<\Delta ## cannot be a solution yet on these diagrams he show the particle has momentum, at E=0 which can't be correct. I know I have this back to front, because he also mentions that at ##E>\Delta ## that is has less momentum than but I just can't see how, could someone please explain to me what my lecture is conveying here.
If E<Δ the particle is confined in one of the boxes, where the potential is zero.
 
  • #3
This is confusing, if I look at the equation it tell me that momentum dose not exist it imaginary. I can't seem to think how this particle is moving inside the box.

I mean if I look over this again he states that at 0 poteinal the particle is in the right of left box, so the particle as I see it is moving to the left and right at the bottom of one of the boxes. But how if E=0 the ##P=\sqrt(2m(E-\Delta))## then the solution give an imaginary value so tho I can see it physically I can see how it is relating to the equation.

Is there a link to either a website or video that will help me understand this concept?

Also where is this energy barrier I can't see how this particle is moving from box to to box
 
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  • #4
Okay so I have been thinking about this a bit more. I have attched photos of my workings, and tryed to explain best to what I think is going on, I know normally it not great to post photo but I couldn’t draw a decent enough diagram to convey what I was thinking.

25465818_10159697059840635_136173687_n.jpg


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  • #5
Taylor_1989 said:
This is confusing, if I look at the equation it tell me that momentum dose not exist it imaginary. I can't seem to think how this particle is moving inside the box.

I mean if I look over this again he states that at 0 poteinal the particle is in the right of left box, so the particle as I see it is moving to the left and right at the bottom of one of the boxes. But how if E=0 the ##P=\sqrt(2m(E-\Delta))## then the solution give an imaginary value so tho I can see it physically I can see how it is relating to the equation.

Remember, the equation is p2/2m +V(x) =E
There are walls of infinite high at x1 and x4. There is a barrier between x2 and x3. The function is defined between x1 and x2, outside it is infinite.

x1<x ≤ x2 V(x) = 0
x2 <x ≤ x3 V(x) = Δ
x3 < x ≤ x4 V(x) = 0

If E < Δ the particle can not exist in the interval x2 <x ≤ x3. It is confined "inside" one of the boxes, either between x1 and x2 or between x3 and x4.

Taylor_1989 said:
Also where is this energy barrier I can't see how this particle is moving from box to to box
If E ≥ Δ the particle can exist in the whole interval x1 <x ≤ x4, only its kinetic energy changes above the barrier. It is not "inside" any boxes
 
  • #6
Taylor_1989 said:
Okay so I have been thinking about this a bit more. I have attched photos of my workings, and tryed to explain best to what I think is going on, I know normally it not great to post photo but I couldn’t draw a decent enough diagram to convey what I was thinking.

View attachment 216869

View attachment 216870

View attachment 216871
The drawing is right, but I can not read your handwriting.
 
  • #7
ehild said:
The drawing is right, but I can not read your handwriting.
Sorry, from your pervious comment, and a couple more hours, I realized what was going on. Thank you for the advice.
 

FAQ: Particle in a box question in classical mechaincs

1. What is a particle in a box in classical mechanics?

A particle in a box is a theoretical model used in classical mechanics to study the behavior of a single particle confined within a potential well. The particle is considered to be a point mass and is subject to the laws of classical mechanics.

2. How is a particle in a box described mathematically?

The particle in a box is described by the Schrödinger equation, which is a partial differential equation that predicts the wave function of the particle at any given time. The solutions to this equation are standing waves, also known as wave functions, which describe the probability of finding the particle at a certain position in the box.

3. What are the boundary conditions for a particle in a box?

The boundary conditions for a particle in a box are determined by the size and shape of the potential well. The particle is assumed to have zero potential energy outside of the box, and the wave function must be continuous and have a derivative of zero at the boundaries of the box.

4. What is the significance of the energy levels in a particle in a box?

The energy levels in a particle in a box correspond to the different energy states that the particle can occupy within the potential well. These energy levels are quantized, meaning that they can only take on certain discrete values. This concept is important in understanding the behavior of particles in quantum systems.

5. How does the behavior of a particle in a box differ from that of a free particle?

A free particle can have any energy and can move freely in space, while a particle in a box is confined to a specific energy level and position within the potential well. The particle in a box also exhibits wave-like behavior due to the wave nature of the Schrödinger equation, whereas a free particle behaves more like a classical particle with a defined position and momentum.

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