The principle that it is not possible to know with unlimited accuracy both the position and momentum of a particle. This principle, discovered in 1927 by Werner Heisenberg, is usually stated in the form: ΔxΔpx ≥ h/4π, where Δx is the uncertainty in the x-coordinate of the particle, Δpx is the uncertainty in the x-component of the particle’s momentum, and h is the Planck constant. An explanation of the uncertainty is that in order to locate a particle exactly, an observer must be able to bounce off it a photon of radiation; this act of location itself alters the position of the particle in an unpredictable way. To locate the position accurately, photons of short wavelength would have to be used. The high momenta of such photons would cause a large effect on the position. On the other hand, using photons of lower momenta would have less effect on the particle’s position, but would be less accurate because of the longer wavelength. See also generalized uncertainty principle.