the normalized wave function for the first excited state of particle in one dimensional box
The wave function can be written as
"\\Psi_n(x)=A_nsin(\\dfrac{n\\pi x}{L})"
The constant "A_n" is determined by normalization condition
"\\int\\Psi^2_n dx=\\int A_n^2sin^2(\\dfrac{n\\pi x}{L})dx=1"
The result of evaluating the integral and solving for "A_n=\\sqrt{\\dfrac{2}{L}}" is independent from n.
The normalized wave function for a particle in a box are thus
"\\Psi_n(x)=\\sqrt{\\dfrac{2}{L}}sin(\\dfrac{n\\pi x}{L})"
For first excited state n = 2
"\\therefore\\space \\Psi_2(x)=\\sqrt{\\dfrac{2}{L}}sin(\\dfrac{2\\pi x}{L})"
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