Difference between revisions of "Forest UCM Osc Damped"
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− | =1-D Damped | + | =1-D Damped Oscillations= |
− | == | + | ==Newton's 2nd Law== |
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:<math> \ddot x + 2 \beta \dot x + \omega^2_0x = 0</math> | :<math> \ddot x + 2 \beta \dot x + \omega^2_0x = 0</math> | ||
+ | ==Solve for the Equation of Motion== | ||
As see in section [[Forest_UCM_Osc_SHM#Equation_of_motion]], you can determine solutions to the above | As see in section [[Forest_UCM_Osc_SHM#Equation_of_motion]], you can determine solutions to the above |
Revision as of 13:04, 5 October 2014
1-D Damped Oscillations
Newton's 2nd Law
As in the case of air resistance, assume there is frictional force proportional to the velocity of the oscillation body.
- : in 1-D
or
or
let
- undamped oscillation frequency
- damping constant
then
Solve for the Equation of Motion
As see in section Forest_UCM_Osc_SHM#Equation_of_motion, you can determine solutions to the above by writing the analogous auxilary equation:
Setting the term in parentheses to zero and using the quadratic formula
You have change the second order differential equation into two first order differential equations
constructing a complete solution from the two solutions (orthogonal functions) above.