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Equation 3, also known as the parallel axis theorem, is used to calculate the moment of inertia of an object that is rotating about an axis that is parallel to the object's center of mass. Equation 6, also known as the perpendicular axis theorem, is used to calculate the moment of inertia of an object that is rotating about an axis that is perpendicular to the object's plane of symmetry.
The equation to use depends on the specific situation. If the object is rotating about an axis that is parallel to its center of mass, use equation 3. If the object is rotating about an axis that is perpendicular to its plane of symmetry, use equation 6.
No, the equations are only applicable to objects with a known plane of symmetry. In addition, equation 3 can only be used for objects with a known center of mass and equation 6 can only be used for objects with a known axis of rotation.
Equations 3 and 6 are related through the moment of inertia tensor. Equation 3 is a special case of equation 6, where the axis of rotation is parallel to the object's center of mass.
No, moment of inertia is a physical quantity that represents the resistance of an object to changes in its rotational motion. It is always a positive value or zero for point masses.