Difference between revisions of "Forest UCM Ch3 AngMom"
Jump to navigation
Jump to search
Line 32: | Line 32: | ||
Consider a planet orbiting the Sun such that the sun if Fixed at the origin. | Consider a planet orbiting the Sun such that the sun if Fixed at the origin. | ||
− | The line segment that joins the planet and the Sun is just the radius vector from the origin of a coordinate system where the sun is located to the position of the planet orbiting the sun. | + | The line segment that joins the planet and the Sun is just the radius vector <math>(\vec r )</math> from the origin of a coordinate system where the sun is located to the position of the planet orbiting the sun. |
[[Forest_UCM_MnAM#Angular_Momentum]] | [[Forest_UCM_MnAM#Angular_Momentum]] |
Revision as of 12:57, 14 September 2014
Definition of Angular Momentum
The angular momentum of a single particle is defined as
An coordinate must be defined in order to express the vectors for the particles position and momentum. The resulting angular momentum is defined with respect to the origin (rotation point) of the particle.
Torque
If I take the derivative of angular momentum with respect to time I get
- cross product of parallel vectors
- Definition of Torque
- Newton's second law for angular motion
Kepler's second Law
Kepler's second Law
- A line segment joining a planet and the Sun sweeps out equal areas during equal intervals of time.
The above law is the result of the conservation of angular momentum when two bodies are attracted to eachother by a central force.
Consider a planet orbiting the Sun such that the sun if Fixed at the origin.
The line segment that joins the planet and the Sun is just the radius vector
from the origin of a coordinate system where the sun is located to the position of the planet orbiting the sun.