Dynamics of Rigid Bodies Formula : Dynamics of rigid bodies refers to the branch of classical mechanics that deals with the motion of objects that maintain a constant shape and size under the influence of external forces. In other words, it involves the study of how rigid bodies move and respond to forces and torques (rotational forces) applied to them.
Understanding this topic is important because it is a part of NEET 2024 Syllabus . Read this and improve your NEET UG 2024 preparation level.Translational Motion - Translational motion refers to the movement of an object in which every point of the object moves along parallel paths. In translational motion, the entire object moves from one place to another without changing its orientation.
Newton's Second Law: F = ma, where F is the net force, m is the mass, and a is the acceleration. Linear Momentum: p = mv, where p is the linear momentum, m is the mass, and v is the velocity.Rotational Motion - Rotational motion, is the movement of an object in a circular path around a fixed point or axis. In rotational motion, the object spins or rotates about a central point. Each point of the object moves in a circular path, and the object changes orientation.
I=mr 2
This formula expresses the rotational inertia of a single-point mass. For more complex objects or systems, where mass is distributed continuously or there are multiple masses, the moment of inertia is determined by summing or integrating the contributions of each mass element along the object.Moment of Inertia for Different Objects | ||
---|---|---|
Object | Axis of Rotation | Moment of Inertia Formula |
Point Mass | Axis passing through the mass | I = mr^2 |
Thin Rod (about end) | Axis perpendicular to the rod | I = (1/3)mL^2 |
Thin Rod (center) | Axis perpendicular to the rod | I = (1/12)mL^2 |
Rectangular Plate | Axis through the center, parallel to sides | I = (1/12)m(a^2 + b^2) |
Hollow Cylinder | Axis through the center | I = (1/2)m(R 1 ^2 + R 2 ^2) |
Solid Cylinder | Axis through the center | I = (1/2)mR^2 |
Hollow Sphere | Axis through the center | I = (2/3)mR^2 |
Solid Sphere | Axis through the center | I = (2/5)mR^2 |
Thin Circular Ring | Axis through the center | I = mR^2 |
Solid Disk | Axis through the center | I = (1/2)mR^2 |
Hollow Disk | Axis through the center | I = (1/2)m(R 1 ^2 + R 2 ^2) |
T-shaped Object | Axis through the center of mass | I = I 1 + I 2 (sum of individual moments of inertia) |
τ=Iα
Where: τ is the torque applied to the object, I is the moment of inertia of the object, and α is the angular acceleration of the object The relationship indicates that the torque applied to an object is equal to the product of its moment of inertia and angular acceleration. This equation is fundamental in understanding and predicting the rotational motion of objects subjected to torques, such as a force applied at a distance from the axis of rotation.Where:
τ=dt/dL
Here,