Damped Driven Harmonic Oscillator

Click For Summary
SUMMARY

The discussion focuses on solving the damped-driven harmonic oscillator by rewriting the differential equation in terms of the complex variable z and its derivatives. The solution is expressed as z(t) = Ce^{i \omega t}, where the complex constant C is reformulated as A e^{-i \delta}. The participants clarify that any complex number can be represented in this form, with δ calculated using the formula δ = tan^{-1}(2βω / (ω₀² - ω²)). This approach utilizes trigonometric principles and Euler's formula to facilitate the solution process.

PREREQUISITES
  • Understanding of differential equations, particularly in the context of harmonic oscillators.
  • Familiarity with complex numbers and their polar representation.
  • Knowledge of Laplace transforms and their application in solving differential equations.
  • Basic trigonometry, specifically the use of arctangent in right triangles.
NEXT STEPS
  • Study the application of Laplace transforms in solving differential equations.
  • Learn about Argand diagrams and their role in visualizing complex numbers.
  • Explore Euler's formula and its implications in complex analysis.
  • Investigate the properties of damped harmonic oscillators and their physical significance.
USEFUL FOR

Students and professionals in physics and engineering, particularly those studying oscillatory systems, complex analysis, and differential equations.

AbigailM
Messages
46
Reaction score
0
Just have a few questions regarding the method of solving the damped-driven harmonic oscillator.

Once we have rewritten the differential equation in terms of z and it's derivatives, we try a solution z(t) = Ce^{i \omega t}. When we sub in z and it's derivatives we then rewrite the complex constant C as Ae^{-i \delta}. My book says that we can do this for any complex number. Why is this?

When we solve for A and sub that into C=Ae^{-i \delta} we find
f_{0}e^{i \delta}=A(\omega_{0}^{2} - \omega^{2} +2i \beta \omega).
My book says we can then rewrite \delta as \delta=tan^{-1}\left(\frac{2\beta\omega}{\omega_{0}^{2}-\omega^{2}}\right). Could someone please explain this? The right triangle explanation is confusing me.

Thank you all.
 
Physics news on Phys.org
I asked a question about this on another forum. I never got an answer, but I know the answer involves taking the laplace transform...
 
we can write any complex number in the form z = re^ig
thus they have just written that complex number in a convenient form for them.
that g (which i am using as my argument for the exponent) is just the angle in the polar representation of a complex number. thus it can be calculated from trigonometry if we know the adjacent and opposite sides of the triangle. this is where the arctan thing comes in.

Do you know how to draw Argand Diagrams? if so, do that for every complex number you see in the derivation and hopefully your trig training will kick in and help you.

hope that helps mate.
 
AbigailM said:
When we sub in z and it's derivatives we then rewrite the complex constant C as Ae^{-i \delta}. My book says that we can do this for any complex number. Why is this?
Do you know about the trigonometric representation of complex numbers and Euler's formula?
For you case, it will be:
e^{-i \delta}=cos\delta - i sin\delta
You can use this to solve your equation and find δ.
 
Awesome that makes sense, I think I'm clear on now. Thank you all for the help!
 

Similar threads

Replies
9
Views
2K
  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 13 ·
Replies
13
Views
1K
Replies
7
Views
1K
Replies
5
Views
1K
Replies
2
Views
956
  • · Replies 3 ·
Replies
3
Views
1K
Replies
3
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K