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The UP (Uncertainty Principle) is subtler than that. The HUP (Heisenberg Uncertainty Principle) refers to preparation and measurement of the position and momentum of a single particle. If you have read popular sources on the HUP, they may have emphasised the "old" UP. In any case, here is a modern view. Note that the HUP is a statistical law. It puts no limitations on the accuracy with which we can measure either the position or the momentum of a particle! (I know that contradicts most popular science sources, but there you have it.)vadadagon said:I'm trying to understand with my limited capacity of education. Yes, I get that people are people and it may not be a good example as quantum particles. My idea is that people have many different properties (age, height, girth, weight, gender, skin color, hair color, eye color, etc) just like quantum particles have many properties. If we measure one property we get one answer.
The reality is that particles have more than the single property we measure. What those properties are we don't know until we measure them, but as far as I am aware is that we can only measure one thing at a time. The uncertain principle says we can only know one thing, we can only get a binary answer to a question (yes/no) or is that not correct?
Suppose we try to contain an electron. We have it confined to a small region - let's call it a box. We know that if we measure its position, we must get an answer that is in the box. If we repeat this many times, then we get a random spread of values - all in the box. There is a statistical measure called the variance of a set of data, denoted by ##(\Delta x)^2## in the case of position. In this case, the variance is on the scale of the width of the box.
Now, we measure the momentum of the electron in the box. What we find is a large variance in the measurements of momentum. This is denoted by ##(\Delta p)^2##. Note that this excludes any experimental uncertainty in the measuring apparatus. We are assuming that we have a near perfect mechanism for measuring momentum. And, again, note that the HUP does not forbid these near perfect measurements.
What the HUP says is:$$\Delta x \Delta p \ge \frac \hbar 2$$Where ##\hbar## is the reduced Planck constant. It's about ##1 \times 10^{-34}## joule-seconds.
What does this mean? First, if the box is quite big, then the variance in position measurements will be quite large. And, that allows the measurements of momentum to have similar values. And, as the box is made progressively smaller, and the variance in position measurements gets smaller, then the variance in momentum measurements gets larger. In other words, we cannot both confine the electron to a very small space and control its momentum to a small range.
Note that we can apply this to the single-slit experiment. If we fire electrons through a wide slit at a detection screen, then we get a band related to the width of the slit. As we narrow the slit, the band narrows. All very classical. But, then, when the slit reaches a critical width where the value of ##\hbar## becomes relevant, the HUP kicks in. And by this I mean the HUP has a significant effect. At that point the the band on the detection screen begins to widen. And the narrower the slit becomes, the wider the band becomes. Moreover, the band begins to break up into sub-bands of light and dark.
Note that the HUP does not say you can only know position or momentum. You can simultaneously know both quite precisely - but only up to a point. You can't know both to arbitrary precision. And by "know" I mean predict the variance in measurements of position and momentum.
In this post I've tried to be as precise as possible. And have avoided woolly generalisations to try to explain precisely what the HUP says.
PS ##\Delta x##, the square root of the variance, is also called the standard deviation.