![]() The moment of inertia of a rotating flywheel is used in a machine to resist variations in applied torque to smooth its rotational output. Planar movement has a single scalar that defines the moment of inertia, while for spatial movement the same calculations yield a 3 × 3 matrix of moments of inertia, called the inertia matrix or inertia tensor. There is an interesting difference in the way moment of inertia appears in planar and spatial movement. Moment of inertia also appears in momentum, kinetic energy, and in Newton's laws of motion for a rigid body as a physical parameter that combines its shape and mass. Comparison of this natural frequency to that of a simple pendulum consisting of a single point of mass provides a mathematical formulation for moment of inertia of an extended body. ![]() The natural frequency of oscillation of a compound pendulum is obtained from the ratio of the torque imposed by gravity on the mass of the pendulum to the resistance to acceleration defined by the moment of inertia. The term moment of inertia was introduced by Leonhard Euler in his book Theoria motus corporum solidorum seu rigidorum in 1765, and it is incorporated into Euler's second law. In 1673 Christiaan Huygens introduced this parameter in his study of the oscillation of a body hanging from a pivot, known as a compound pendulum. m 2) in SI units and pound-square feet (lb m.Moment of inertia may be expressed in terms of kilogram-square meters (kg The amount of torque needed for any given change in angular momentum is proportional to the size of that change. When a body is rotating around an axis, a torque must be applied to change its angular momentum. Each body has a set of mutually perpendicular axes, called principal axes, for which the off-diagonal terms of the inertia matrix are zero, and a torque around a principal axis only affects the acceleration about that axis. The inertia matrix includes off-diagonal terms called products of inertia that couple torque around one axis to angular acceleration about another axis. circular plate The inertia matrix is often described as a symmetric rank two tensor, having six independent components. In this case, the body has a single moment of inertia, which is measured around this axis.įor spatial movement of a body, the moment of inertia is defined by its symmetric 3 × 3 inertia matrix. In classical mechanics, moment of inertia may also be called mass moment of inertia, rotational inertia, polar moment of inertia, or the angular mass.įor planar movement of a body, the trajectories of all of its points lie in parallel planes, and the rotation occurs only about an axis perpendicular to this plane. For example, if m a + m b = m c, then I a + I b = I c. Moment of inertia depends on the amount and distribution of its mass, and can be found through the sum of moments of inertia of the masses making up the whole object, under the same conditions. ![]() ![]() A larger moment of inertia around a given axis requires more torque to increase the rotation, or to stop the rotation, of a body about that axis. Moment of inertia depends on the shape of the body and may be different around different axes of rotation. Moment of inertia is the mass property of a rigid body that determines the torque needed for a desired Circular cylinder around the axis angular acceleration about an axis of rotation.
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