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1. Show that the directivity for a source with a unidirectional power pattern given by $U = U_m \cos^n \theta$ can be expressed as $D = 2(n+1)$. U has a value only for $0 \le \theta \le \frac{\pi}{2}$ and $0 \le \phi \le 2\pi$ and is zero elsewhere.

          1. Show that the directivity for a source with a unidirectional power pattern given by $U = U_m \cos^n \theta$ can be expressed as $D = 2(n+1)$. U has a value only for $0 \le \theta \le \frac{\pi}{2}$ and $0 \le \phi \le 2\pi$ and is zero elsewhere.
        
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1. Show that the directivity for a source with a unidirectional power pattern given by U = Um cos^n θ can be expressed as D = 2(n+1). U has a value only for 0 ≤θ≤(π)/(2) and 0 ≤ϕ≤ 2π and is zero elsewhere.

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University Physics with Modern Physics
University Physics with Modern Physics
Hugh D. Young 14th Edition
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1. Show that the directivity for a source with a unidirectional power pattern given by U = Um cos can be expressed as D = 2(n+1). U has a value only for 0 /2 and 0 2 and is zero elsewhere
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Transcript

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00:01 Okay, so during chapter 29, problem 39.
00:03 So it says show that the rms output of an ac generator is given by n -a -b -o -mega over root 2, and it says omega equals 2 pi -f.
00:20 So if we look back at equation 294, sorry, that was, i mean to write that better, equation 294, and that kills us what the peak voltage is.
00:35 So that means that gives us the peak voltage here is in a omega...
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