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600<br />

Wire and Wireless Communication Applications Chap. 8<br />

In Eq. (8–10), the free-space loss † is<br />

(L FS ) dB = 20 log a 4pd<br />

l<br />

b dB<br />

(8–11)<br />

For example, the free-space loss at 4 GHz for the shortest path to a synchronous satellite from<br />

Earth (22,300 miles) is 195.6 dB.<br />

Note that from Eq. (8–8), the received power increases as the square of the wavelength<br />

(free space condition). That is, if the carrier frequency is reduced by a factor of 2, then the<br />

received power will increase by a factor of 4. This is equivalent to the loss decreasing by 6 dB<br />

as shown by Eq. (8–11).<br />

Thermal Noise Sources<br />

The noise power generated by a thermal noise source will be studied because the receiver noise<br />

is evaluated in terms of this phenomenon. A conductive element with two terminals may be<br />

characterized by its resistance, R ohms. This resistive, or lossy, element contains free electrons<br />

that have some random motion if the temperature of the resistor is above absolute zero. This<br />

random motion causes a noise voltage to be generated at the terminals of the resistor. Although<br />

the noise is small, when the noise is amplified by a high-gain receiver it can become a problem.<br />

(If no noise were present, we could communicate to the edge of the universe with infinitely<br />

small power, since the signal could always be amplified without having noise introduced.)<br />

This physical lossy element, or physical resistor, can be modeled by an equivalent circuit<br />

that consists of a noiseless resistor in series with a noise voltage source. (See Fig. 8–17.)<br />

From quantum mechanics, it can be shown that the (normalized) power spectrum corresponding<br />

to the voltage source is [Van der Ziel, 1986]<br />

v (f) = 2Rc h ƒ f ƒ<br />

2<br />

+<br />

h ƒ f ƒ<br />

d<br />

e hƒfƒ>(kT) - 1<br />

(8–12)<br />

Physical<br />

resistor<br />

R<br />

Noiseless<br />

resistor<br />

Equivalent<br />

noise<br />

source<br />

R<br />

v(t)<br />

p v (f)<br />

(a) A Lossy Circuit Element<br />

Characterized by Its<br />

Resistance<br />

Figure 8–17<br />

(b) Thevenin Equivalent<br />

Circuit Model of the<br />

Lossy Circuit Element<br />

Thermal noise source.<br />

† This free-space path loss expression can be modified to include effects of a multipath channel within an<br />

urban building environment. [See Eq. (8–67).]

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