general Hisenberg relation

The angular momentum of an electron with uniform circular motion is ћ (i.e., pr≈ћ). Δx•Δpx≥ћ is easily obtained from the deformation of pr≈ћ. The process of transitioning from classical motion law to the relation can indicate: Δx•Δpx≥ћ no longer strongly negates orbital motion; and formulas shaped like Δx•Δpx≥ћ possess determinism and indeterminism do..