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5 =4 10 7 ln[10+ p 99]=1:2 (mH/m): G0=0 because s =0 C0= pe 0 ln d 2a + q d 2a 2 1 = p 8:85 10 12 ln[10+ p 99] =9:29 (pF/m): Fawwaz T. Ulaby and Umberto Ravaioli, Fundamentals of Applied Electromagnetics c 2015 Prentice Hall. Exercise 2.2 Calculate the transmission line parameters at 1 MHz for a rigid coaxial air line with an inner conductor

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By the end of Chapter 5, we will know (among other things) how to use the DFT to convolve two generic sampled signals stored in a computer. By the end of Ch. 6, we will know that by using the FFT, this approach to convolution is generally much faster

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from 1 to 5. Verify that it has the same value as the Simpson’s Rule formula for the three points (1, 5), (3, 12) and (5, 9). 1b. Verify Simpson’s Rule using the quadratic y = 2x2 + 5x + 12 on the interval [-1, 5]. 1c. Verify Simpson’s Rule using the cubic y = x3 + 2x2 –5x –2 on the interval [0, 2]

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### Fundamentals of Applied Electromagnetics

5 =4 10 7 ln[10+ p 99]=1:2 (mH/m): G0=0 because s =0 C0= pe 0 ln d 2a + q d 2a 2 1 = p 8:85 10 12 ln[10+ p 99] =9:29 (pF/m): Fawwaz T. Ulaby and Umberto Ravaioli, Fundamentals of Applied Electromagnetics c 2015 Prentice Hall. Exercise 2.2 Calculate the transmission line parameters at 1 MHz for a rigid coaxial air line with an inner conductor

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