What are the properties of a normalized wave function?

But, as I said, you don't have to do it that way. Expand the (b-x)2, and integrate. That's easier.b^2x + \frac{x^3}{3} - bx^2 \\\frac{b^3}{3} + \frac{a^3}{3} - \frac{ba^2}{2} - ( \frac{b^3}{3} + \frac{a^3}{3} - \frac{b^2a}{2} ) \\\frac{a^3}{3} - \frac{ba^2}{2} - \frac{a^3}{3} + \frac{
  • #1
vorcil
398
0
At time = 0 a particle is represented by the wave function

[tex] \Psi(x,0) = \left\{ \begin{array}{ccc}
A\frac{x}{a}, & if 0 \leq x \leq a, \\
A\frac{b-x}{b-a}, & if a \leq x \leq b, \\
0, & otherwise,
\end{array} \right
[/tex]where A, a, and b are constants.

(a) Normalize [tex] \Psi [/tex] (that is, find A, in terms of a and b).

(b) where is the particle most likely to be found, at t =0?

(c) What is the probability of finding the particle to the left of a? Check your result in the limiting cases b=a and b = 2a

(d) what is the expectation value of x?
 
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  • #2
My attempt:

no bloody idea where to start,

I know that to normalize a function,

[tex] \int_{-\infty}^{\infty} |\Psi(x,t)|^2 dx =1 [/tex]

But have no idea how I am supposed to incorporate that into my question...

I need EXAMPLES
I have no idea how to solve something I've never seen before!
 
  • #3
ok I'm just going to start guessing here,

if someone would be kind enough to correct me on mistakes

----------------------------------------------------------

since I want to find A,
and the wave function [tex] \Psi(x,0) = A \frac{x}{a} [/tex]

if I square it, it should = 1?
[tex] \Psi(x,0)^2 = A^2 \frac{x^2}{a^2} ==1 [/tex]

not too sure where to go from here
 
  • #4
the same with the middle equation,

[tex]
\Psi(x,0)^2 =(A\frac{(b-x}{b-a})^2) =1
[/tex]
 
  • #5
  • #6
You have the right idea but the two integrals added together should be equal to one I do believe. Also be sure to square the A/(b-a) on the second integral.
 
  • #7
When I am normalizing the wave function, do I add the equations from all the parts of the wave function?

i.e

[tex] \int_{-\infty}^{0} +\int_{0}^{a}+\int_{a}^{b}+\int_{b}^\infty [/tex]
 
  • #8
so adding that to concept to my question,

i'd get

[tex]|\Psi(x,0)|^2 = \int_{-\infty}^0 0^2dx + \frac{A^2}{a^2}\int_0^a x^2 dx + \frac{A}{(b-a)} \int_a^b (b-x)^2 dx + \int_b^\infty 0^2dx = [/tex]
 
  • #9
[tex]
= |\Psi(x,0)|^2 = \frac{A^2}{a^2}\int_0^a x^2 dx + \frac{A^2}{(b-a)^2} \int_a^b (b-x)^2 dx
[/tex]
then uh simplifying and such i get,
(since A^2 is in both equations)

[tex] \left( A^2 \left[ \left( \frac{1}{a^2} \frac{x^3}{3} \right) + \left( \frac{1}{(b-a)^2} \int_a^b (b-x)^2 dx \right) \right] \right) =1 [/tex]
 
Last edited:
  • #10
That is almost correct except A/(b-a) should be squared as well and then all of that will be equal to one. Then you should do each integral then just solve for A.
 
  • #11
how do I integrate (b-x)^2 ?

[tex] \int (b-x)(b-x)dx = \int (b^2 - 2bx + x^2 )dx= b^2 -\frac{2bx^2}{2} + \frac{x^3}{3} [/tex]

? then i evaluate that at [tex] & \left equation \right|_{a}^{b} [/tex]
 
  • #12
For b2, you can think of that as b2*x0. So when you take the integral of that, you would end up with b2*x1. Other than that, everything else looks correct.
 
  • #13
[tex]\int (b^2 - 2bx + x^2) dx = b^2x - \frac{2bx^2}{2} + \frac{x^3}{3} [/tex]

[tex]

b^2x - bx^2 +\frac{x^3}{3}

[/tex]

what now?
I was shown that the answer to that integral was

[tex] -\frac{(b-x)^3}{3} [/tex]

but how do i get that?
from

[tex] \int_a^b (b-x)^2 dx [/tex]
to
[tex] \left -\frac{(b-x)^3}{3} \right|_a^b [/tex]
 
  • #14
vorcil said:
[tex]\int (b^2 - 2bx + x^2) dx = b^2x - \frac{2bx^2}{2} + \frac{x^3}{3} [/tex]

[tex]

b^2x - bx^2 +\frac{x^3}{3}

[/tex]

what now?
I was shown that the answer to that integral was

[tex] -\frac{(b-x)^3}{3} [/tex]

but how do i get that?
from

[tex] \int_a^b (b-x)^2 dx [/tex]
to
[tex] \left -\frac{(b-x)^3}{3} \right|_a^b [/tex]

They used u=(b-x) => du=-dx

You are on a roll and almost there -- keep up the good work!
 
  • #15
embarassing

but I can't integrate that, I don't know how

can someone please explain to me how to integrate it?

[tex]\int_a^b (b-x)^2 dx [/tex]

:(
 
  • #16
vorcil said:
embarassing

but I can't integrate that, I don't know how

can someone please explain to me how to integrate it?

[tex]\int_a^b (b-x)^2 dx [/tex]

:(

You don't have to do it the way they did it. Just expand (b-x)2, and make three simple integrals. You should be able to do those.
 
  • #17
[tex]\int_b^a (b-x)^2dx \\[/tex]

[tex]\int_b^a (b-x)(b-x)dx \\[/tex]

[tex]\int_b^a (b^2 +x^2 -2bx)dx \\[/tex]

[tex]b^2x + \frac{x^3}{3} + \frac{-2bx^2}{2} \\
[/tex]

i Don't see how that equation,

[tex] b^2x + \frac{x^3}{3} + \frac{-2bx^2}{2} [/tex]
equals

[tex] \frac{(b-x)^3}{3} [/tex]

can someone just explain please
 
  • #18
They do it by making the "u" substitution I wrote in the earlier post. The integral becomes -u2du

Integrate that, then put the b-x back into u.
 

1. What is the purpose of normalizing a wave function?

The purpose of normalizing a wave function is to ensure that the total probability of finding a particle in any region of space is equal to 1. This allows for accurate predictions of the behavior of the particle.

2. How is a wave function normalized?

A wave function is normalized by dividing it by the square root of the integral of the absolute square of the function over all space. This ensures that the resulting function has a total probability of 1.

3. Why is it important to normalize a wave function?

It is important to normalize a wave function because it allows for accurate calculations and predictions of the behavior of a particle. A non-normalized wave function would not accurately represent the probability of finding the particle in a certain region of space.

4. Can a wave function be normalized to a value other than 1?

No, a wave function must be normalized to a value of 1 in order to accurately represent the probability of finding a particle in any region of space. Any other normalization would result in incorrect predictions.

5. What is the difference between a normalized and non-normalized wave function?

A normalized wave function has a total probability of 1, meaning that the probability of finding the particle in any region of space is accurately represented. A non-normalized wave function does not have a total probability of 1 and would result in incorrect predictions of the particle's behavior.

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