Momentum Operator and Wavefunction problem

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SUMMARY

The discussion centers on determining the linear momentum and kinetic energy of a particle with the wavefunction psi=cos(ax). The linear momentum operator is defined as P(sub)x=(h/(2πi))d/dx, and the Schrödinger equation is applied to find the energy term E. The calculations reveal that both the linear momentum and kinetic energy have well-defined values, specifically E = -h^2a^2/(2m(2πi)^2). The potential energy term is not included in the equation as it varies by system but can be incorporated if needed.

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grahamfw
Okay this should be fairly easy, not really sure why it's not working for me.

Suppose a particle moving along the x-axis is in a state with a wavefunction psi=cos(ax). Determine whether (i) the linear momentum and the (ii) kinetic energy of the particle has a single well-define value. If so what is it?

The operator we are given is P(sub)x=(h/(2πi))d/dx. I know to set it up using the Hpsi= Epsi. What I don't know is what to use for E. Classically, we have used just T + V and I know that T=(P(sub)x)^2/(2m) . But what about V? Can I leave it out? Is it not important?

Once, I get that, I can find out if it has a sharp observable for both of those.

Any help is greatly appreciated. Thanks in advance.

Graham
 
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Hi Graham,

First, let's start by finding the linear momentum operator for our given wavefunction. As you correctly stated, the linear momentum operator is given by P(sub)x=(h/(2πi))d/dx. So, we can plug this into the Schrödinger equation Hpsi= Epsi and solve for the energy term.

Hpsi= Epsi
P(sub)x^2/(2m)psi= Epsi
(h^2/(2m(2πi)^2))(d^2psi/dx^2)= Epsi

Now, we can substitute our given wavefunction psi=cos(ax) into this equation and solve for E.

(h^2/(2m(2πi)^2))(d^2(cos(ax))/dx^2)= Ecos(ax)

Using the chain rule, we can find the second derivative of cos(ax).

d^2(cos(ax))/dx^2= -a^2cos(ax)

So, our equation becomes:

(h^2/(2m(2πi)^2))(-a^2cos(ax))= Ecos(ax)

Simplifying, we get:

(-h^2a^2/(2m(2πi)^2))= E

Therefore, we can see that the energy term for our given wavefunction is -h^2a^2/(2m(2πi)^2). This means that the linear momentum and kinetic energy of the particle do have well-defined values, which are given by -h^2a^2/(2m(2πi)^2).

As for the potential energy term, it is not explicitly included in the Schrödinger equation because it depends on the specific system and is not a fundamental property of the particle. However, it can be added into the equation if necessary.

I hope this helps and clarifies the problem for you. Let me know if you have any further questions. Good luck!
 

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