Normalization of the infinite square well.

In summary, the conversation was about deriving equations for a test on Quantum Mechanics and a discrepancy in the result obtained from the textbook and Wolfram Alpha. It was resolved by realizing that the extra term in the equation disappears due to the restriction on the values of k.
  • #1
Jdraper
51
0
I have been going through my textbook deriving equations in preparation for my test on QM tomorrow. I noticed in the infinite square well that i was unable to complete the normalization.

My textbook, Griffiths reads :

(integral from 0 to a) ∫|A|^2 * (sin(kx))^2 =|A|^2 * (a/2) =1 Therefore, |A|^2 = 2/a

When i do this integral i do not get this result, furthermore when i put this integral into wolfram alpha i get this result:

http://www.wolframalpha.com/input/?i=integrate+sin^2(kx)+dx+from+0+to+a

Which is also not the required result.

It's probably something stupid but help would be appreciated none the less,

Thanks in advance, John.
 
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  • #2
Using the result from Wolfram Alpha, your equation becomes
$$|A|^2 \left( \frac{a}{2} - \frac{\sin(2ak)}{4k} \right) = 1$$
Recall that k is restricted to certain values because of the boundary conditions. What are those values?
 
  • #3
I derived the wave equation to be:

[itex]\Psi[/itex](x) = Asin(kx), So this means k takes integer values of n?

So k's values are restricted to (n*pi/a) where n=1,2,3

Just as i was writing that out i understood, k can only take integer values so sin(2kx) will always equal 0 meaning the expression is just a/2.

Thanks a bunch :)
 
  • #4
Right, ##\sin(ka) = \sin(2n\pi)## which is always zero for integer n. It's nice when "extra" terms in an equation disappear like that. :smile:
 

FAQ: Normalization of the infinite square well.

What is the infinite square well potential?

The infinite square well is a theoretical potential used in quantum mechanics to describe the behavior of a particle confined to a finite region. It consists of an infinitely deep potential well with infinitely high walls, creating a finite space in which the particle can exist.

What is normalization in the context of the infinite square well?

Normalization is a mathematical process used to ensure that the wavefunction of a particle confined in the infinite square well has a total probability of 1. This means that the particle has a 100% chance of being found somewhere within the well.

How is normalization achieved in the infinite square well?

To normalize the wavefunction in the infinite square well, we use the normalization condition, which states that the integral of the square of the wavefunction over all space must equal 1. This can be achieved by adjusting the coefficients of the wavefunction to satisfy this condition.

What is the significance of normalization in the infinite square well?

Normalization is significant because it ensures that the wavefunction of the particle is physically meaningful. It also allows us to calculate the probability of finding the particle in a specific region of the well, which is crucial in understanding the behavior of quantum systems.

Can the normalization constant be different for different wavefunctions in the infinite square well?

Yes, the normalization constant can vary for different wavefunctions in the infinite square well. This is because the shape and energy of the wavefunctions can differ, leading to different probability distributions and therefore requiring different normalization constants to satisfy the normalization condition.

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