Wavefunctions and boundaries of a 1D-potential well

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The discussion centers on the formulation of wavefunctions within a one-dimensional potential well, specifically addressing boundary conditions at x = -a, 0, and b. The proposed wavefunctions are: (1) 0 for x < -a, (2) Asin(k1x) + Bcos(k1x) for -a < x < 0, (3) Csin(k2x) + Dcos(k2x) for 0 < x < b, and (4) 0 for x > b. The participants confirm that the wavefunction must be continuous at boundaries and that the first derivative is also continuous at x = -a and x = b, while discussing the implications of infinite potential on the wavefunction's behavior.

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indie452
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the attachment here shows a potential well and i am practicing writing down wave functions in each region and boundary conditions (for this problem I suppose the boundaries would be x= -a, 0, b.

i think that for this problem i need 4 functions and i thought that they may be:

when
x<-a (1) = 0
-a<x<0 (2) = Asin(k1x) + Bcos(k1x)
0<x<b (3) = Csin(k2x) + Dcos(k2x)
b>x (4) = 0

where
k1 = (\sqrt{}2mE)/\hbar
k2 = (\sqrt{}2m(E-Vo))/\hbar

and i think at the boundary x = -a and b the wave function is continuous and at x=0 the wave function and the first derivative is continuous.

Is this right?
thanks
 

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|.........|
|.........| Vo < E
|.........|
|......__________|
|......|
|......|
|......|
|......|
-a......0....b

V(x)=
infinity --- x<-a --- region 1
0 --- -a<x<0 --- region 2
Vo --- 0<x<b --- region 3
infinity --- b<x --- region 4

if you can't see the pic
 
first thing:

maybe you want to think again about what you stated here when you said "b>x (4) = 0", i believe you have done simple mistake since you wrote the first three equations correctly, it actually should be "x>b (4) = 0"

second thing:

dont you think that you should make your wavefunction continuous by appliying the fact that the wavefunction and its derivative (1st) in region(1) = the wavefunction and its derivative (1st) in region(2) and that when x = -a , and the same goes with region(2) and (3) when x = 0 , also region(3) and (4) when x = b ..

hmm, well .. I think so .. what do you think?
 
for the first thing your right i did write it down wrong t=it was meant to be b<x.

but with the the reason i wrote that the first derivative of the wavefunction is not continuous at the boundary x=-a, and b was cause i thought that when on the otherside of a boundary the potential->infinity, so KE->-infinty at boundaries so first derivative->infinity also. this is cause it seems to be infinite potential and so not physically realistic.
 
for the first thing your right i did write it down wrong t=it was meant to be b<x.

but with the the reason i wrote that the first derivative of the wavefunction is not continuous at the boundary x=-a, and b was cause i thought that when on the otherside of a boundary the potential->infinity, so KE->-infinty at boundaries so first derivative->infinity also. this is cause it seems to be infinite potential and so not physically realistic.
 
thats mainly the reason behind choosing the wavefunction = 0 in both regions 1 and 4..

lets first consider the situation when we say that the wavefunction and its derivative should be continuos in region (1) and (2) when x = -a ..

you have in region (2) that the wavefunction = A sin(k1x) + B cos(k1x) .. so when x = -a

in region(2) the wavefunction = - A sin(k1a) + B cos(k1a) & you know that the wavefunction in region(1) at x = -a is zero >>> then 0 = -A sin(k1a) + B cos(k1a)
im not allowed to proceed more than this, but i think you got the point (I hope!) .. continue with the derivatives .. and don't forget the other regions ..

good luck..
 
for the first thing your right i did write it down wrong t=it was meant to be b<x.

but with the the reason i wrote that the first derivative of the wavefunction is not continuous at the boundary x=-a, and b was cause i thought that when on the otherside of a boundary the potential->infinity, so KE->-infinty at boundaries so first derivative->infinity also. this is cause it seems to be infinite potential and so not physically realistic.
 

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