Normalization of a wave function

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The discussion revolves around normalizing the wave function psi(x) = b(a^2 - x^2) for a particle confined within the interval -a to +a. The user successfully derived the normalization constant b as sqrt(15/16a^5) through integration, confirming the method is correct. For the probability of finding the particle at x = +a/2 within a small interval, the initial calculation yielded 0.7 percent, but an error was identified in squaring a term, revising the probability to 0.5 percent. The user has not yet attempted part C, which requires integration over a larger interval. Overall, the calculations for parts A and B are validated, with a minor correction needed for part B's final result.
leehufford
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Homework Statement


A particle is described by the wave function psi(x) = b(a2-x2) for -a < x < +a and psi(x) = 0 for x < -a and x > +a, where a and b are positive real number constants.

a) Using the normalization condition, find b in terms of a.
b) What is the probability to find the particle at x = +a/2 in a small interval of width 0.010a?
c) What is the probability for the particle to be found between x = +a/2 and x = +a?

Homework Equations



Psi(x) = b(a2-x2)
The integral of Psi(x)2 from negative infinity to infinity must equal one, so that way it can exist.
P(x) dx = (Psi(x))2

The Attempt at a Solution



I have an answer, but I was hoping someone could confirm I did this right, this concept is brand new to me and my answer from A looks weird to me.

Part A:

b2* Integral of (a2-x2)(a2-x2) dx = 1 (From -a to a, since everywhere else Psi is zero).

b2[a4x - (2/3)a2x2 + (1/5)x5] dx = 1 evaluated from -a to a...

b2[(a5-(2/3)a5+(1/5)a5) - (-a5 + (2/3)a5-(1/3)a5) = 1

b2(16a5/15) = 1, so b = sqrt(15/16a5).

Part B:

P(x)dx = (Psi(x))2 dx

= (15/16a5)(a2-x2)2 dx
= (15/16a5)(a2 - (1/4)a2)2(0.010a)
= (15/16a5)(3/4)a4(0.010a)
=0.007, or 0.7 percent chance of finding the particle there.

Part C: I didn't attempt part C because I wanted to hopefully get some feedback that I was on the right track before I started part C. Looks like I will actually have to integrate for part C since the interval is bigger. Thanks for reading.

Lee
 
Last edited:
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I did not check your computations in detail, but your approach is correct and assuming you did the math correctly your results for (a) and (b) should therefore be correct as well. Just watch out for (what I assume is) the typo in aa in your problem formulation.
 
Thank you Orodruin for your reply and noticing the typo. It's been corrected. I'm pleased to know the approach is correct since I have already double checked the math.
 
There are indeed many typos, but there is also an error in part b.

leehufford said:
= (15/16a5)(3/4)a4(0.010a)
That equation (and the number you get from it) is incorrect.
 
DrClaude - thank you for the reply. I noticed i forgot to square the (3/4), so my final equation is now

(15/16a5)(9/16)a4(0.010a) = 0.005 = 0.5 percent chance.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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