Expectation Value of Energy for Nonstationary State in Infinite Square Well

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The discussion focuses on calculating the expectation value of energy for a particle in an infinite square well, specifically for a wavefunction that is a superposition of the ground and first excited states. The normalization constant C is determined to ensure the wavefunction is properly normalized. The time-dependent wavefunction is derived, allowing for the calculation of the expectation value of the Hamiltonian operator. The key result shows that the expectation value of energy in this state is the average of the energies of the first two stationary states, expressed as (E1 + E2)/2. This confirms the relationship between the wavefunction and its energy expectation in a nonstationary state.
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Consider a particle in an infinite square well of width L. Initially, (at t=0) the system is
described by a wavefunction that is equal parts a superposition of the ground and first
excited states:
Ψ(x, 0)=C[Ψ1(x)+Ψ2(x)]
a) Find C so that the wavefunction is normalized
b) Find the wave function at any later time t.
c)show that the expectation value of the energy in this state is (E1+E2)/2, where E1 AND E2 ARE THE ENERGIES OF THE FIRST TWO STATIONARY STATES.


I DID a) and b) , i don't how to do c) , could you help me
 
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So, if \psi(x,t) is your wavefunction, what is the expectation value of the Hamiltonian operator?
 
p.s. you may just do it at t=0, but don't forget to prove that you *can*.
 

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