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16.10:

Torque Free Motion

JoVE Core
Mechanical Engineering
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JoVE Core Mechanical Engineering
Torque Free Motion

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Torque-free motion refers to the movement of a rigid body without any external torques acting upon it. Consider an axisymmetric object, with the z-axis being the axis of symmetry, having the center of mass defined at the origin of the rotating frame of reference. Here, the moment of inertia about the x and y axes are equal. Consider the inertial frame of reference defined such that the positive Z-axis of the inertial frame is along the angular momentum vector and makes an angle θ with the positive z-axis of the rotating frame. So, the angular momentum can be expressed in terms of unit vectors in two ways, and by equating the components of unit vectors, the equation for the object's angular velocity is derived. Additionally, writing the angular velocity in terms of angular displacement and equating the components again gives the equation of motion for a torque-free axisymmetric rigid body. Here, the object's angular momentum, precession, and spin remain constant throughout the motion along with angle θ.

16.10:

Torque Free Motion

The torque-free motion refers to the movement of a rigid body in space when no external torques are acting upon it. This type of motion can be observed in environments where there are no external forces or frictions, like in outer space. For example, a rotation of Mars in space is a torque-free motion. Mars is an axisymmetric object, meaning it has an axis of symmetry along which it rotates, designated as the z-axis. The rotating frame of reference is defined such that the center of mass of Mars is at the origin. This arrangement ensures that the moments of inertia about the x and y axes are equal.

An additional inertial frame of reference is used to further analyze Mars's motion. In this inertial frame, the positive Z-axis aligns with the angular momentum vector of Mars. It forms an angle theta (θ), with the positive z-axis of the rotating frame. The angular momentum of Mars can be expressed in two different ways using unit vectors. By equating these unit vectors' components, one can derive an equation for the object's angular velocity. Furthermore, by expressing the angular velocity in terms of angular displacement and equating the components once again, one arrives at the equation of motion for our torque-free, axisymmetric, rigid object living on Mars.

Throughout the motion of Mars, its angular momentum, precession, spin, and the angle θ remain constant. These constants reveal the intriguing dynamics of torque-free motion for Mars.