1 / 15

External Forcing

External Forcing. SHO with an additional external force. PHYSICS 1. Why this particular type of force?. Somnath Bharadwaj and Pratik Khastgir, Department of Physics and Meteorology, IIT Kharagpur, 721 302 India http://www.cts.iitkgp.ernet.in/~phy1/. Fourier Series.

ghackworth
Download Presentation

External Forcing

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. External Forcing SHO with an additional external force PHYSICS 1 Why this particular type of force? • Somnath Bharadwaj and Pratik Khastgir, Department of Physics and Meteorology, IIT Kharagpur, 721 302 India http://www.cts.iitkgp.ernet.in/~phy1/

  2. Fourier Series For any arbitrary time varying force

  3. Solution using Fourier Series Find solution for a single frequency Superpose solutions

  4. The equation where Solution=Complementary Function + Particular Integral

  5. Particular Integral

  6. Amplitude and Phase

  7. Amplitude and Phase

  8. Low Frequency Response Stiffness Controlled Regime

  9. High Frequency Response Mass Controlled Regime solution of

  10. Effect of Damping Solution=Complementary Function + Particular Integral

  11. Solutions Complementary Functions are transients Steady State behaviour is decided by the Particular Integral

  12. Solution with Damping

  13. Amplitude and Phase (again)

  14. Amplitude and Phase (again) -

  15. Some Key Points High frequency and low frequency behaviour unchanged by damping Amplitude is finite throughout Maximum Amplitude at

More Related