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Consider a particle in a 1-dimensional box defined by V(x)=0, for 0

User Pzin
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The question is incomplete. The complete question is :

Consider a particle in a one-dimensional box defined by V(x)=0, a>x>0 and V(x)=infinity, x a, x 0. Explain why each of the following un-normalized functions is or is not an acceptable wave function based on criteria such as being consistent with the boundary conditions, and with the association of psi^+(x)psi(x)dx with the probability.

a).
$A \cos (n \pi x)/(a)$

b).
$B(x+x^2)$

c).
$Cx^3(x-a)$

d).
$(D)/(\sin (n \pi x)/(a))$

Solution :

a). The function of cosine here do not go to the value 0 at the boundary of the box (that is to be expected as V is infinite there).


$ \Psi (0) = A$ and
$ \Psi (a) = A \cos(n \pi) = \pm 1$

Therefore it is not an acceptable function.

b). The function in this case goes to 0 at
$x=0, $ but is non zero at
$x=a$. So this function is also not acceptable.

c). The function here goes to 0 at both
$x=a$ and
$x=b$ . But this wavelength can never satisfy the time independent Schrodinger equation.


-(\hbar^2)/(2m)(d^2)/(dx^2)\Psi(x)\\eq E\Psi(x)\quad \text{for} \ \quad \Psi(x)=Cx^3(x-a)

Therefore,
$\Psi + \Psi $ here can not be associated with the probability.

d). Here, the function goes to the infinite at
$x=0 $ and
$x=a$. Thus this is also not valid choice for the wave function.

User Will Neithan
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