dimensionless
- 460
- 1
I have a particle of mass m in a box of length L. The energy eigenstates of this particle have wave functions
\phi_{n}(x)=\sqrt{2/L}sin(n \pi x/L)
and energies
E_n = n^{2}\pi^{2}\hbar^{2}/2mL^{2}
where n=1, 2, 3,... At time t=0, the particle is in a state described as follows.
\Psi(t=0)=\frac{1}{\sqrt{14}}[\phi_1 + 2\phi_2 + 3\phi_3]
To find the energy for state \Psi I did the following.
\sum_{1, 2, 3} E_n = (1^2 + 2^2 +3^2) \frac{\pi^2\hbar^2}{2mL^2}=14\frac{\pi^2\hbar^2}{2mL^2}= 14E_1
where E_1=\frac{\pi^2\hbar^2}{2mL^2}
I have made a mistake somewhere because the actual answer is 9 E_1. Does anyone know where my error is?
\phi_{n}(x)=\sqrt{2/L}sin(n \pi x/L)
and energies
E_n = n^{2}\pi^{2}\hbar^{2}/2mL^{2}
where n=1, 2, 3,... At time t=0, the particle is in a state described as follows.
\Psi(t=0)=\frac{1}{\sqrt{14}}[\phi_1 + 2\phi_2 + 3\phi_3]
To find the energy for state \Psi I did the following.
\sum_{1, 2, 3} E_n = (1^2 + 2^2 +3^2) \frac{\pi^2\hbar^2}{2mL^2}=14\frac{\pi^2\hbar^2}{2mL^2}= 14E_1
where E_1=\frac{\pi^2\hbar^2}{2mL^2}
I have made a mistake somewhere because the actual answer is 9 E_1. Does anyone know where my error is?
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