Finding Turning Points of Morse Potential V(x)

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Logarythmic
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How can I find the turning points for the one dimensional Morse potential

[tex]V(x) = D(e^{-2ax}-2e^{-ax})[/tex]

??
 
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That's probably my problem then, what is the definition of "turning point"?
 
Yes I have graphed the potential.
 
Should I invert the function and find the min and max for x(V) ?
 
Turning points are related to the "classically forbidden regions", they are boundaries for these regions. It's easier to see if the problem is unidimensional and you can graph the potential.

Daniel.
 
Yes, but how do I determine the turning points?
 
But isn't
[tex]E = \frac{1}{2}m \dot{x}^2 + V(x)[/tex]?
 
Nope and yes. I assumed you wish to find the classical turning points of the Morse potential and for that you need to solve the eqn i wrote. At these turning points the classical KE is zero.

Daniel.
 
Yes of course. But then I've only got V(x) = V(x) ??
 
Ok, but I'm studying classical mechanics so I think I have to use another approach...
 
Logarythmic said:
Ok, but I'm studying classical mechanics so I think I have to use another approach...

I'm not aware of another approach. You start off with a certain amount of energy, which is a constant in a conserved system. But the classical turning points are when [tex]\dot{x} = 0[\tex], and then a moment later the velocity changes signs (i.e. the particle goes from going to the right to going to the left), so then you do what Dexter suggests, and hopefully understand why you're doing it.[/tex]
 
I understand this now. I get the equation

[tex]D(e^{-2ax}-2e^{-ax})-E=0[/tex]

Any tricks on how to solve this?