If a rigid body is subject to planar motion in the xy-plane, then the angular momentum about the rigid body's center of mass can be expressed as the body's angular velocity times the body's moment of inertia about the z-axis through the center of mass plus the body's angular velocity time the sum of two products of inertia. If a rigid body is subject to planar motion in the xy-plane, then the angular momentum about the rigid body's center of mass can be expressed as the body's angular velocity times the body's moment of inertia about the z-axis through the center of mass plus the body's angular velocity time the sum of two products of inertia. True False
If a rigid body is subject to planar motion in the xy-plane, then the angular momentum about the rigid body's center of mass can be expressed as the body's angular velocity times the body's moment of inertia about the z-axis through the center of mass plus the body's angular velocity time the sum of two products of inertia. If a rigid body is subject to planar motion in the xy-plane, then the angular momentum about the rigid body's center of mass can be expressed as the body's angular velocity times the body's moment of inertia about the z-axis through the center of mass plus the body's angular velocity time the sum of two products of inertia. True False
If a rigid body is subject to planar motion in the xy-plane, then the angular momentum about the rigid body's center of mass can be expressed as the body's angular velocity times the body's moment of inertia about the z-axis through the center of mass plus the body's angular velocity time the sum of two products of inertia. If a rigid body is subject to planar motion in the xy-plane, then the angular momentum about the rigid body's center of mass can be expressed as the body's angular velocity times the body's moment of inertia about the z-axis through the center of mass plus the body's angular velocity time the sum of two products of inertia. True False
If a rigid body is subject to planar motion in the xy-plane, then the angular momentum about the rigid body's center of mass can be expressed as the body's angular velocity times the body's moment of inertia about the z-axis through the center of mass plus the body's angular velocity time the sum of two products of inertia.
If a rigid body is subject to planar motion in the xy-plane, then the angular momentum about the rigid body's center of mass can be expressed as the body's angular velocity times the body's moment of inertia about the z-axis through the center of mass plus the body's angular velocity time the sum of two products of inertia.
True
False
Definition Definition Product of the moment of inertia and angular velocity of the rotating body: (L) = Iω Angular momentum is a vector quantity, and it has both magnitude and direction. The magnitude of angular momentum is represented by the length of the vector, and the direction is the same as the direction of angular velocity.
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