When microwave radiation is shot at a diatomic molecule, the observed energy splitting is inversely proportional to this non-constant quantity, which appears in the denominator of the formula for a constant denoted B.
When microwave radiation is shot at a diatomic molecule, the observed energy splitting is inversely proportional to this non-constant quantity, which appears in the denominator of the formula for a constant denoted B. This quantity is represented by a symmetric and positive-definite rank-2 tensor which is diagonalized in rigid body analysis to yield three (*) "principal values" of it. Deforming an object in the direction of a principal axis does not change this quantity according to the stretch rule. In general, this quantity is defined as the volume integral of R squared Â times dM. When this quantity is known for one axis, it can be calculated for other axes by the aptly-named parallel axis theorem. Angular momentum equals this quantity times angular velocity. For 10 points, I is the symbol for what quantity, the rotational analogue of mass?
When microwave radiation is shot at a diatomic molecule, the observed energy splitting is inversely proportional to this non-constant quantity, which appears in the denominator of the formula for a constant denoted B.
moment of inertia 