 However, to understand contextuality in Bohmian mechanics almost nothing needs to be explained. Consider an operator \(A\) that commutes with operators \(B\) and \(C\) (which however don’t commute with each other). What is often called the “result for \(A\)” in an experiment for “measuring \(A\) together with \(B\)” usually disagrees with the “result for \(A\)” in an experiment for “measuring \(A\) together with \(C\)”. This is because these experiments differ and different experiments usually have different results. The misleading reference to measurement, which suggests that a pre-existing value of \(A\) is being revealed, makes contextuality seem more than it is.