![]()
![]()
VIDEO LECTURE
COMMENTS
Feel free to leave any comments on the lesson - your views, improvements, mistakes, clarification of concepts, or vote to have this lesson revised. |
CONCEPT
We shall now see how the terms velocity and acceleration, as many of you are familiar with in 2-dimensional kinematics, are applied to 3-dimensional vectors. We will have to use a few concepts of geometry of curves in this whole chapter to define some of the definitions.Image a particle moving in 3D space. At time t, the particle is at the point
can be perceive as a movable arrow to the particle at time t. Much like previously thought, the functions From here onwards, let’s assume that x, y, and z are twice-differentiable functions of t. In any time interval ![]() The velocity of the particle at time t is defined to be The vector While this interpretation of the velocity vector and its magnitude seems correct, it is also consistent should we find the speed of the particle by finding the rate of change with respect to time of the distance traveled along the curve, as such. ![]() Finally the acceleration of the particle is defined as the rate of change of velocity with respect to time, that is, which I’ll kindly remind you is a vector quantity.Let’s look are a simple example where we shall explicitly find the velocity and acceleration of a position vector.Say, a particle is moving along a trajectory given by the parametric equations, From here, we get the position vector, The velocity vector is given by And the acceleration is and the speed is Just a reminder, the symbols All information presentated, less questions and exercises, is original content of Donny, with slight references to various books.
Video courtesy of YouTube.com service. |