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Design of Antennas for Handheld DVB-H ... - Lunds tekniska högskola

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2.3 Antenna theory<br />

This section describes basic antenna theory, to easier understand later discussions.<br />

2.3.1 Efficiency, directivity and gain<br />

Radiation efficiency ηrad is defined as the ratio between the radiated power Prad<br />

and the power accepted by the antenna Pin (see figure 2.8)<br />

P<br />

rad η rad =<br />

(2.1)<br />

Pin<br />

The directivity D and the gain G <strong>of</strong> an antenna are connected to each other by ηrad<br />

as<br />

G = ηrad<br />

D<br />

(2.2)<br />

Directivity describes the directional property <strong>of</strong> an antenna and the gain takes into<br />

account the losses in the antenna structure. For an ideal antenna the gain and the<br />

directivity are equal.<br />

Figure 2.8. Voltage reflection from a mismatched load.<br />

Γ is the refection coefficient, ZL and Z0 are the impedances <strong>of</strong> the load and<br />

transmission line, respectively. Pt, Pin and Prad are the (total) incident power to the<br />

load, the power accepted by the load and the power radiated by the load,<br />

respectively.<br />

2.3.2 Reflection from a mismatched antenna<br />

The antenna impedance, ZL, must be equal to the characteristic impedance <strong>for</strong> the<br />

transmission line feeding the antenna, Z0, otherwise part <strong>of</strong> the voltage will be<br />

reflected from the antenna. How large this reflected voltage is can be measured in<br />

a network analyser as the parameter S11. The reflection coefficient can be<br />

calculated with following equation:<br />

Z<br />

Z<br />

− Z<br />

+ Z<br />

L 0<br />

Γ =<br />

(2.3)<br />

L<br />

0<br />

19

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