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The concept of noise power spectral density was introduced in Sec. 12.5 for a flat frequency spectrum. Where the spectrum is not flat, an average value for the spectral density can be calculated. To illustrate this, the very much simplified spectrum curve of Fig. 13.10 will be used. The maximum spectrum density is flat at 3 W/Hz from 0 to 2 kHz and then slopes linearly down to zero over the range from 2 to 8 kHz. The noise power in any given bandwidth is calculated as the area under the curve, the width of which is the value of the bandwidth. Thus, for the first 2 kHz, the noise power is 3 W/Hz 2000 6000 W. From 2 to 8 kHz, the noise power is 3 (8 2) 1000/2 9000 W. The total power is therefore 15,000 W, and the average spectral density is 15,000/8000 1.875 W/Hz. The noise power spectral density over the worst 4-kHz bandwidth must include the highest part of the curve and is therefore calculated for the 0- to 4-kHz band. The power over this band is seen to be the area of the rectangle 3 W/Hz 4 kHz minus the area of the triangle shown dashed in Fig. 13.10. The power over the 0- to 4-kHz band is therefore (3 4000) (3 2) (4 2) 1000/2 11,000 W, and the spectral density is 11,000/4000 2.75 W/Hz. The units for spectral power density are often stated as watts per hertz (W/Hz). Expressed in this manner the units are descriptive of the way in which the power spectral density is arrived at. In terms of fundamental units, watts are equivalent to joules per second and hertz to cycles per second or simply seconds 1, since cycles are a dimensionless asp.net ean 13 EAN - 13 ASP . NET Control - EAN - 13 barcode generator with free ...
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