1 / 15

Slide Presentations for ECE 329, Introduction to Electromagnetic Fields, to supplement “Elements of Engineering Electrom

Slide Presentations for ECE 329, Introduction to Electromagnetic Fields, to supplement “Elements of Engineering Electromagnetics, Sixth Edition”. by Nannapaneni Narayana Rao Edward C. Jordan Professor of Electrical and Computer Engineering

ricky
Download Presentation

Slide Presentations for ECE 329, Introduction to Electromagnetic Fields, to supplement “Elements of Engineering Electrom

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. Slide Presentations for ECE 329,Introduction to Electromagnetic Fields,to supplement “Elements of Engineering Electromagnetics, Sixth Edition” by Nannapaneni Narayana Rao Edward C. Jordan Professor of Electrical and Computer Engineering University of Illinois at Urbana-Champaign, Urbana, Illinois, USA Distinguished Amrita Professor of Engineering Amrita Vishwa Vidyapeetham, Coimbatore, Tamil Nadu, India

  2. 5.3Poisson’s and Laplace’s Equations

  3. Poisson’s Equation For static electric field, Then from If e is uniform, Poisson’s equation

  4. If eis nonuniform, then using Thus Assuming uniform e, we have For the one-dimensional case of V(x),

  5. D5.7 Anode, x = d V = V0 Vacuum Diode Cathode, x = 0 V = 0 (a)

  6. (b)

  7. (c)

  8. Laplace’s Equation If r = 0, Poisson’s equation becomes Let us consider uniform efirst Parallel-plate capacitor x = d, V= V0 x = 0, V = 0

  9. Neglecting fringing of field at edges, General solution

  10. Boundary conditions Particular solution

  11. area of plates For nonuniform e, For

  12. Example x = d, V = V0 x = 0, V = 0

More Related