Uncertainty of position in an infinite potential well

In summary, the conversation discusses the ground state energy and momentum of a particle trapped in an infinite potential well of width a. It is noted that the momentum is a precise value and the uncertainty in position would be infinite. However, further analysis shows that the uncertainty of momentum is actually not zero, but rather given by the standard deviation formula. This is demonstrated by the momentum probability distribution for the ground state, which is not a constant value but rather a curve.
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Ananthan9470
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The ground state energy of a particle trapped in an infinite potential well of width a is given by (ħ2π2)/2ma2. So the momentum is given by (2mE)1/2 = ħπ/a. Since this is a precise value, doesn't that mean that we know momentum with 100% certainty? And if that is the case shouldn't the uncertainty in position be infinite?
 
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  • #2
Your relation for the momentum is incorrect.
You can find the momentum in QM by applying the momentum operator - just like you find the energy by applying the energy operator. So what happes when you apply the momentum operator to the ground-state energy eigenfunction for a particle in a box?

Note: The momentum wavefunction is the Fourier transform of the position wavefunction.
 
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Ananthan9470 said:
The ground state energy of a particle trapped in an infinite potential well of width a is given by (ħ2π2)/2ma2. So the momentum is given by (2mE)1/2 = ħπ/a. Since this is a precise value, doesn't that mean that we know momentum with 100% certainty? And if that is the case shouldn't the uncertainty in position be infinite?

But if all you know is [itex]E[/itex], then the momentum is [itex]\pm \sqrt{2mE}[/itex]. So the expectation value of [itex]p[/itex] is 0 (it's just as likely to be pointing in one direction as another). A rough estimate of the uncertainty in a quantity is the standard deviation, which would tell us:

[itex]\delta p = \sqrt{\langle p^2\rangle - \langle p \rangle^2}[/itex] where [itex]\langle X \rangle[/itex] means the expectation value, or average value. So for this problem:

[itex]\langle p \rangle = 0[/itex]
[itex]\langle p^2 \rangle = 2mE[/itex]

So
[itex]\delta p = \sqrt{2mE} = \frac{\hbar \pi}{a} [/itex]

So the uncertainty of [itex]p[/itex] is not zero.
 
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Related to Uncertainty of position in an infinite potential well

1. What is the Uncertainty Principle?

The Uncertainty Principle is a fundamental concept in quantum mechanics that states it is impossible to know both the exact position and momentum of a particle simultaneously. This means that the more precisely we know the position of a particle, the less we know about its momentum, and vice versa.

2. How does the Uncertainty Principle relate to the infinite potential well?

In the infinite potential well, a particle is confined to a certain region and its momentum is constrained by the walls of the well. This means that the uncertainty in the particle's position is very small, and therefore the uncertainty in its momentum must be large to satisfy the Uncertainty Principle.

3. What is the effect of increasing the size of the potential well on the uncertainty of position?

As the size of the potential well increases, the uncertainty of position decreases. This is because the larger the well, the more spread out the particle's wave function becomes, leading to a more well-defined position.

4. Can the uncertainty of position ever be zero in an infinite potential well?

No, according to the Uncertainty Principle, the uncertainty of position can never be exactly zero. This is because a particle's position and momentum are fundamentally linked, and it is impossible to know both values with complete certainty.

5. How does the uncertainty of position in the infinite potential well compare to other systems?

The uncertainty of position in the infinite potential well is unique in that it is the lowest possible value for a confined particle. In other systems, such as a particle in a finite potential well or a free particle, the uncertainty of position can be larger.

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