Phy5645/Uncertainty Relations Problem 2: Difference between revisions
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<math> \Delta E\cong \frac{\hbar ^2}{2m(\Delta x) ^2}= \frac{\hbar ^2 c ^2}{2mc ^2(\Delta x) ^2 }= \frac{(197 \times 10 ^{-13}\,\text{MeV}\cdot\text{cm}) ^2} {(2) (938\,\text{MeV}) (10 ^{-12}) ^2} \approx 0.2\,\text{MeV}</math> | <math> \Delta E\cong \frac{\hbar ^2}{2m(\Delta x) ^2}= \frac{\hbar ^2 c ^2}{2mc ^2(\Delta x) ^2 }= \frac{(197 \times 10 ^{-13}\,\text{MeV}\cdot\text{cm}) ^2} {(2) (938\,\text{MeV}) (10 ^{-12}) ^2} \approx 0.2\,\text{MeV}</math> | ||
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Revision as of 12:32, 5 April 2013
This is a problem from the book of W.Greiner named Quantum Mechanics.
Consider a box with a particle (a nucleon) in it. The width of the box is . Determine the magnitude of kinetic energy of the particle.
According to the Heisenberg Uncertanity Principle, and so . On the other hand, as we know that Therefore,
If we plug into the energy equation, we obtain
Let the length of a side of the box
Knowing that the size of a nucleon is about that their mass , and that , we can calculate kinetic energy.
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