Numerical Methods Introduction to Fourier Series Part: Introduction to Fourier Series http://numericalmethods.eng.usf.edu For more details on this topic Go to http://numericalmethods.eng.usf.edu Click on Keyword Click on Introduction to Fourier Series You are free to Share – to copy, distribute, display and perform the work to Remix – to make derivative works Under the following conditions Attribution — You must attribute the work in the manner specified by the author or licensor (but not in any way that suggests that they endorse you or your use of the work). Noncommercial — You may not use this work for commercial purposes. Share Alike — If you alter, transform, or build upon this work, you may distribute the resulting work only under the same or similar license to this one. Lecture # 1 Chapter 11.01: Introduction to Fourier Series Major: All Engineering Majors Authors: Duc Nguyen http://numericalmethods.eng.usf.edu Numerical Methods for STEM undergraduates 4/8/2015 http://numericalmethods.eng.usf.edu 5 Background The following relationships can be readily established T T 0 0 sin( kw0t )dt cos(kw0t ) dt 0 (1) T sin ( kw0t )dt cos ( kw0t ) dt 0 0 2 (2) T 2 T 2 1 6 http://numericalmethods.eng.usf.edu Background cont. T (3) cos(kw0t ) sin( gw0t ) dt 0 0 T sin( kw0t ) sin( gw0t ) dt 0 (4) 0 T cos(kw0t ) cos( gw0t ) dt 0 (5) 0 7 http://numericalmethods.eng.usf.edu Background cont. w 2f (6) 1 f T (7) 0 Where f and represents the frequency in (cycles/time) and period (in seconds) respectively. T A periodic function with a period the following equation: f (t T ) f (t ) 8 T should satisfy (8) http://numericalmethods.eng.usf.edu Background cont. Example 1 Let T A sin( kw0t )dt (9) 0 1 T cos(kw0t )0 kw0 9 http://numericalmethods.eng.usf.edu Background cont. 1 cos(kw0T ) cos(0) A kw0 1 cos(k 2 ) 1 kw0 (10) 0 10 http://numericalmethods.eng.usf.edu Background cont. Example 2 Let T B sin (kw0t )dt 2 (11) 0 Recall 1 cos(2 ) sin ( ) 2 (12) 1 1 B cos(2kw0t ) dt o 2 2 (13) 2 T 11 http://numericalmethods.eng.usf.edu Background cont. T 1 1 1 sin( 2kw0t ) t 2 2 2kw0 0 T 1 B sin( 2kw0T ) 0 2 4kw0 12 (14) http://numericalmethods.eng.usf.edu Background cont. T 1 sin( 2k * 2 ) 2 4kw0 T 2 Example 3 Let T C sin( gw0t ) cos(kw0t )dt (15) 0 13 http://numericalmethods.eng.usf.edu Background cont. Recall that sin( ) sin( ) cos( ) sin( ) cos( ) (16) C sin g k w0t sin( kw0t ) cos(gw0t )dt T (17) 0 14 http://numericalmethods.eng.usf.edu Background cont. sin ( g k ) w0t dt sin( kw0t ) cos(gw0t )dt (18) T T 0 T 0 C 0 sin( kw0t ) cos( gw0t )dt (19) 0 Adding Equations (15), (19), T T 0 0 2C sin( gw0t ) cos(kw0t )dt sin( kw0t ) cos(gw0t )dt sin gw0t (kw0t )dt sin ( g k ) w0t dt T 0 15 T 0 (20) http://numericalmethods.eng.usf.edu Background cont. 2C 0, since the right side of the above equation is zero Thus, T C sin( gw0t ) cos(kw0t )dt 0 (21) o 16 http://numericalmethods.eng.usf.edu THE END http://numericalmethods.eng.usf.edu Acknowledgement This instructional power point brought to you by Numerical Methods for STEM undergraduate http://numericalmethods.eng.usf.edu Committed to bringing numerical methods to the undergraduate For instructional videos on other topics, go to http://numericalmethods.eng.usf.edu/videos/ This material is based upon work supported by the National Science Foundation under Grant # 0717624. Any opinions, findings, and conclusions or recommendations expressed in this material are those of the author(s) and do not necessarily reflect the views of the National Science Foundation. The End - Really