Single degree of freedom damped free vibrations: Difference between revisions
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== Governing Equation == | == Governing Equation == | ||
Governing equation for the motion of single of freedom oscilator can be written as: | |||
This is a [[second-order linear ordinary differential equation with constant coefficients]] that yields the following solution | {| width="100%" | ||
|- | |||
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| <tex>m\ddot{u}(t) + c\dot{u}(t) + ku(t) = 0</tex> | |||
| align = "right" | (1) | |||
|} | |||
This is a [[second-order linear ordinary differential equation with constant coefficients]] that can be rearranged as follows: | |||
{| width="100%" | |||
|- | |||
| width = "50px" | | |||
| <tex>\ddot{u}(t) + \frac{c}{m}\dot{u}(t) + \frac{k}{m}u(t) = 0</tex> | |||
| align = "right" | (2) | |||
|} | |||
After substitution of <tex>\omega = \sqrt{\frac{k}{m}}</tex> (Eqn. 2) becomes | |||
{| width="100%" | |||
|- | |||
| width = "50px" | | |||
| <tex>\ddot{u}(t) + \frac{c}{m} \dot{u}(t) + \omega^2 u(t) = 0</tex> | |||
| align = "right" | (3) | |||
|} | |||
which yields the following [[characteristic equation]] | |||
{| width="100%" | |||
|- | |||
| width = "50px" | | |||
| <tex>\lambda^2 + \frac{c}{m} \lambda + \omega^2 = 0</tex> | |||
| align = "right" | (3) | |||
|} | |||
with a solution | |||
{| width="100%" | |||
|- | |||
| width = "50px" | | |||
| <tex>\lambda_{1,2} = \frac{-\frac{c}{m} \pm \sqrt{(\frac{c}{m})^2 - 4 \omega^2}}{2} = -\frac{c}{2m} \pm \sqrt{(\frac{c}{2m})^2 - \omega^2}</tex> | |||
| align = "right" | (3) | |||
|} | |||
=== Critically-Damped Systems === | |||
=== Undercritically-Damped Systems === | |||
=== Overcritically-Damped Systems === | |||
== Derivation == | |||
{{To Do | who = user:ok | comment = Provide solution for single degree of freedom damped free vibrations}} | {{To Do | who = user:ok | comment = Provide solution for single degree of freedom damped free vibrations}} | ||
Revision as of 03:02, 6 October 2009
Governing Equation
Governing equation for the motion of single of freedom oscilator can be written as:
| <tex>m\ddot{u}(t) + c\dot{u}(t) + ku(t) = 0</tex> | (1) |
This is a second-order linear ordinary differential equation with constant coefficients that can be rearranged as follows:
| <tex>\ddot{u}(t) + \frac{c}{m}\dot{u}(t) + \frac{k}{m}u(t) = 0</tex> | (2) |
After substitution of <tex>\omega = \sqrt{\frac{k}{m}}</tex> (Eqn. 2) becomes
| <tex>\ddot{u}(t) + \frac{c}{m} \dot{u}(t) + \omega^2 u(t) = 0</tex> | (3) |
which yields the following characteristic equation
| <tex>\lambda^2 + \frac{c}{m} \lambda + \omega^2 = 0</tex> | (3) |
with a solution
| <tex>\lambda_{1,2} = \frac{-\frac{c}{m} \pm \sqrt{(\frac{c}{m})^2 - 4 \omega^2}}{2} = -\frac{c}{2m} \pm \sqrt{(\frac{c}{2m})^2 - \omega^2}</tex> | (3) |
Critically-Damped Systems
Undercritically-Damped Systems
Overcritically-Damped Systems
Derivation
To Do: Provide solution for single degree of freedom damped free vibrations (who: user:ok; priority: 100; hours: 0) (all) (cat)
References
- Ray W. Clough and Joseph Penzien: Dynamics of Structures, 2nd edition, McGraw-Hill, New York, 1993. 738 pages. ISBN 0-07-011394-7, section 2-6, p. 26
External Links
- SDOF Damped Free Vibrations at eFunda
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