- #1
tommy01
- 40
- 0
Hi together ...
In many textbooks on particle physics i encounter - at least in my mind - a misuse of the Heisenberg uncertainty principle.
For completeness we talk about
[tex]\Delta p \Delta x \geq \hbar/2 [/tex]
For example they state that the size of an atom is of the order of a few Angstroms. Therefore [tex]\Delta x[/tex] of an Electron is [tex]\approx 10^{-10}m[/tex] then the conclude that the momentum is [tex]\approx \hbar/\Delta x[/tex].
But what justifies this? The only thing you get is [tex]\Delta p[/tex] this means the momentum is about [tex]p \pm \Delta p[/tex] how one can conclude from the uncertainty of an observable its mean value?
In many textbooks on particle physics i encounter - at least in my mind - a misuse of the Heisenberg uncertainty principle.
For completeness we talk about
[tex]\Delta p \Delta x \geq \hbar/2 [/tex]
For example they state that the size of an atom is of the order of a few Angstroms. Therefore [tex]\Delta x[/tex] of an Electron is [tex]\approx 10^{-10}m[/tex] then the conclude that the momentum is [tex]\approx \hbar/\Delta x[/tex].
But what justifies this? The only thing you get is [tex]\Delta p[/tex] this means the momentum is about [tex]p \pm \Delta p[/tex] how one can conclude from the uncertainty of an observable its mean value?