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Phase II Final Report - NASA's Institute for Advanced Concepts

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Chapter 4.0 Entomopter Flight Operations<br />

4.3 Entomopter-borne Active Emitters <strong>for</strong> Navigation and Communication<br />

power compared to conventional systems. Lastly, the subsystem could be reconfigured in real<br />

time to per<strong>for</strong>m the desired function autonomously by the Entomopter itself.<br />

The radiated wave<strong>for</strong>m is assumed to be a modulated<br />

Gaussian wave<strong>for</strong>m (MGW), with its frequency<br />

spectrum shifted to the appropriate<br />

operating frequency. A time-domain plot of a<br />

MGW centered at 18 GHz is shown in Figure 4-14.<br />

f(t)<br />

f()<br />

t<br />

1<br />

Figure 4-14: Time-domain Plot of Modulated<br />

Gaussian Wave<strong>for</strong>m (MGW) Centered at<br />

18 GHz<br />

−0.95<br />

0 t<br />

t (s)<br />

4.24×<br />

10 − 10<br />

4.3.5.1 Communications Analysis<br />

An analysis was per<strong>for</strong>med by Volpe National Transportation System Center [291] in which<br />

peak powers were calculated <strong>for</strong> MGW pulses <strong>for</strong> communication and surveillance applications.<br />

For communications, Volpe found that the required peak power is independent of the signal<br />

wave<strong>for</strong>m. Thus, <strong>for</strong> communications, the conventional range equation can be used or<br />

2 2<br />

(4π<br />

) r k<br />

BTo<br />

BW SNR Lo<br />

P<br />

T<br />

= Equation 4-5<br />

2<br />

G G λ<br />

T<br />

R<br />

where P T is the required peak transmitter power; r is the distance from the receiver to the transmitter;<br />

k B is Boltzman's constant; T o is the effective system noise temperature; SNR is the<br />

received signal to noise ratio; G T and G R are the gains of the transmitting and receiving antennas,<br />

respectively; BW is the signal bandwidth; λ is the wavelength; and L o is additional losses<br />

due to propagation losses, dust, etc. For ultra wideband signals, the time-bandwidth product is<br />

given approximately by [95]<br />

BW ≈ 1<br />

Equation 4-6<br />

T w<br />

where T w is the pulse width in time. Assuming all of the received power is in the in<strong>for</strong>mational<br />

signal, Equation 4-5 also can be expressed in terms of the bit energy to noise ratio E b /N o as<br />

2<br />

(4π<br />

) r<br />

P =<br />

T<br />

2<br />

E<br />

k<br />

BTo<br />

BW<br />

N<br />

2<br />

G G λ<br />

T<br />

R<br />

b<br />

o<br />

F L<br />

o<br />

Equation 4-7<br />

where F is the noise figure. Expressed in this manner, we can relate the required power to<br />

achieve bit error rate (BER) per<strong>for</strong>mance. Assuming we will use on-off keying (OOK) modulation,<br />

the BER can be expressed as [267]<br />

249

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