kevin0960
- 12
- 0
Hi guys,
I earned that
\Delta E \Delta t \gtrapprox \frac{\hbar}{2}
But one thing that's really strange is, according to Planck's assumption on black-body radiation problem, it just say that energy of each osciliator can be written as
E = nhf
where n is an integer. (I hope this would be true)
So, my question is that if we can measure the energy of an osciliator precisly enough so that Energy of a certain osciliator can meet this inequality.
(n - 1)hf < E < (n+1)hf
At the same time, we can measure \Delta t in some way but it won't be \infty cause \Delta E is obviously not 0.
But here is the problem, we can actually know the energy of osciliator because the energy of it have to be multiple of n. So, E is nhf, and we can get the \Delta t not an infinity value which is not reasonable. Because if we measure the energy of an object, the uncertainty of t have to be infinite.
So, what is the problem?
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I'm not good at eng though :(
I earned that
\Delta E \Delta t \gtrapprox \frac{\hbar}{2}
But one thing that's really strange is, according to Planck's assumption on black-body radiation problem, it just say that energy of each osciliator can be written as
E = nhf
where n is an integer. (I hope this would be true)
So, my question is that if we can measure the energy of an osciliator precisly enough so that Energy of a certain osciliator can meet this inequality.
(n - 1)hf < E < (n+1)hf
At the same time, we can measure \Delta t in some way but it won't be \infty cause \Delta E is obviously not 0.
But here is the problem, we can actually know the energy of osciliator because the energy of it have to be multiple of n. So, E is nhf, and we can get the \Delta t not an infinity value which is not reasonable. Because if we measure the energy of an object, the uncertainty of t have to be infinite.
So, what is the problem?
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I'm not good at eng though :(