Expectation value of energy in infinite well

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SUMMARY

The discussion centers on calculating the expectation value of energy for a particle in an infinite potential well, specifically using the normalized wave function ψ(x) = √(1/a) (1 + 2cos(∏x/a))sin(∏x/a). The participants agree on the rearrangement of the wave function into a superposition of states and confirm that the expectation value can be derived as = 1/2 (E(1) + E(2)). This method is validated as correct, emphasizing the importance of understanding superposition in quantum mechanics.

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Homework Statement


Given the following normalised time-independent wave function the question asks for the expectation value of the energy of the particle. The well has V(x)=0 for 0<x<a


Homework Equations



ψ( x ) = √(1/a) ( 1+2cos(∏x/a) )sin(∏x/a)

The Attempt at a Solution



I disagree with the given answer but we both start off the same way. We rearrange the equation as
ψ ( x ) = √(1/a) ( sin(∏x/a) + sin(2∏x/a) )

The given solution then performs then calculates <E> = ∫ ψ H ψ to arrive at <E> = E(1) + E(2).

I wrote ψ down as the superposition of the wavefunction √(2/a) sin (n∏x/a) which means ψ(1) and ψ(2) both have a coefficient of 1/(√2) in front of them. I then squared this coefficient and multiplied by E(1) +E(2) to get <E> = 1/2 ( E(1) + E(2) )

Is my method ok ? and is my answer correct ?

Thanks
 
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Yes your method and answer are correct. :smile:

<E> = ∫ ψ H ψ = 1/2 ( E(1) + E(2) )
 

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