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