
Explain how a rigid body’s point velocity arises from a fixed absolute frame plus a body-fixed rotation, using a rotation matrix R and the angular velocity Omega.
Derive the angular velocity vector Omega such that the velocity of point B equals Omega cross B. The lecture links this to a skew-symmetric matrix and determinant representation.
Demonstrates how a rotating disc produces tangential velocity at the circumference using angular velocity and v equals omega cross r. Connects 2d rotation matrices to the vector form of omega.
Compute angular velocity as a function of three angles by composing rotations about the x, y, and z axes and differentiating the rotation matrix with respect to time.
Present the velocity of a point on a moving rigid body as v = v' + ω × r, and derive its acceleration including the Coriolis term.
Examine how a rigid body's instantaneous motion follows a motss axis parallel to the angular velocity, producing rotation about and translation along that axis—a helical motion.
Demonstrate the Mozzi theorem for a rigid body by showing a unique line, the Mozzi axis, along which all points share the same velocity, parameterized by lambda along omega.
Examine special cases of rigid-body motion around the Mozzi axis, where zero along-axis velocity yields rotation, and vanishing angular velocity while velocities along the Mozzi axis persist yields translation.
Explore the dynamics of a general rigid body by linking distributed forces to the total external force, and derive that whole-body acceleration equals mass times the center of gravity's acceleration.
This lecture shows that in three-dimensional rigid body motion, the equation of moments supplies three equations and complements the center of mass position, velocity, and angular velocity descriptions.
We derive the equation of moments by applying Newton's laws to a six-degree-of-freedom rigid body, summing infinitesimal forces and reactions, and using a cross product to relate angular momentum.
Derive the equation of moments by integrating external moments over the system mass. Explore how reactions, center of gravity, and a six-equation, six-unknown framework influence the moment balance.
Derive the three-dimensional rigid body moment equations by converting the mass integral to a volume integral, using center-of-mass coordinates and orientation angles with angular velocity concepts.
Derive the external moment about the center of gravity using the inertia tensor (inertia matrix) and a cross product with angular velocity.
Explore how the rate of energy input relates to the kinetic energy of a rigid body, illustrating conservation of energy, moments, and the inertia matrix.
Derive torque and moments from forces using cross products and mixed products. Link power to torque and introduce the virtual work theorem for energy conservation.
Derive the virtual work theorem for a rigid body. Relate the sum of forces times velocity to the time derivative of kinetic energy and introduce the inertia matrix.
Derives the kinetic energy of a rigid body in terms of angular velocity and the inertia matrix, then links it to the virtual work theorem and energy conservation.
Explore the inertia matrix properties, including symmetry and relation to the center of mass, and diagonalize the matrix to reveal the principal axes and moments of inertia.
Derive the components of the rigid body equations of motion in three dimensions using a diagonal inertia tensor in principal axes, with two-dimensional simplifications and omega aligned with eigenvectors.
Explore torque-free motion of a rigid body with no external forces, analyzing stability of the angular velocity under various initial conditions and principal-axis alignments.
Explore stability analysis of torque-free motion in three dimensions; derive elliptical relations for omega2 and omega3 under perturbations, and note that case three reveals instability along certain axes.
Analyze the motion of a four bar linkage, a one degree of freedom mechanism, using kinematic equations to express gamma and phi as functions of theta, illustrated with Matlab simulations.
Investigate the kinematically possible motion of a four-bar linkage within advanced rigid body mechanics in three dimensions.
Analyze a four-bar parallelogram linkage with cranks and a connecting rod, and determine the torque needed to balance external force, gravity, and inertia using the virtual work principle.
This course delves into the fundamental equations and concepts that govern the mechanics of rigid bodies. It provides a comprehensive and detailed derivation of all key equations, ensuring that students understand the underlying principles from first principles. To fully engage with the material, a solid understanding of the following mathematical concepts is required: vectors, dot and cross products, basic linear algebra (including matrices, determinants, eigenvectors, and eigenvalues), and essential calculus (with a focus on derivatives and volume integrals). On the physics side, the only prerequisite is familiarity with Newton's laws of motion, as they serve as the foundational framework for the entire course. Specifically, the laws governing point-particle dynamics (F = ma, where F is the total force acting on a particle, m is its mass, and a is its acceleration) are extended to construct the equations governing rigid body motion.
Throughout the course, we will derive the inertia matrix, which plays a crucial role in the equation of moments and in the expression of the kinetic energy of a rigid body. The concept of angular velocity will also be introduced, and its uniqueness will be demonstrated, setting the stage for a deeper understanding of rotational dynamics. Additionally, we will explore several important kinematic formulas that relate the velocities and accelerations of arbitrary points on a rigid body.
One of the key highlights of the course is the derivation of Chasles' theorem (also known as Mozzi–Chasles' theorem), which states that the most general displacement of a rigid body can be achieved by combining a translation along a line, known as the Mozzi axis, with a rotation about the same axis. This result has profound implications for the analysis of rigid body motion and serves as a cornerstone for further study in mechanics.
By the end of the course, students will gain a deep understanding of the mathematical and physical principles that govern the motion of rigid bodies, laying a strong foundation for advanced studies in mechanics, robotics, and engineering applications.