Lecture3 2009 Antennas

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    Lecture3 2009 Antennas - Presentation Transcript

    1. Antennas
    2. RF RF systems complement wired networks by extending them. Different components may be used depending on the frequency and the distance that signals are required to reach g Two RF components are of particular interest to wireless users: Antennas Amplifiers
    3. Amplifiers A lifi Amplifiers make signals bigger. Signal boost, or gain, is measured in g , g, decibels (dB). Amplifiers can be broadly classified into three categories: low-noise high-power other
    4. Low N i A lifi L Noise Amplifiers (LNA ) (LNAs) Low-noise amplifiers (LNAs) are usually connected to an antenna to boost the received signal to a level that is recognizable by the electronics the RF system is connected to. LNAs are also rated for noise factor, which is the measure of how much unwanted information the amplifier introduces. Smaller noise factors allow the receiver to hear smaller signals and thus allow for a greater range. range
    5. High Power A lifi Hi h P Amplifiers (HPA ) (HPAs) High-power amplifiers (HPAs) are used to boost a signal to the maximum g power possible before transmission. Output power is measured in dBm Amplifiers generate heat in addition to amplifying the signal. signal
    6. Antennas At They convert electrical signals on wires into radio waves and vice versa. An antenna must be made of conducting material. Radio waves hitting an antenna cause electrons to flow in the conductor and create a current. Likewise, applying a current to an antenna creates an electric field around the antenna. As the current to the antenna changes so changes, does the electric field. A changing electric field causes a magnetic field, and the wave is off. off
    7. The size of the antenna you need depends on the frequency: the higher the frequency, the smaller the frequency antenna. The shortest simple antenna you can make at any frequency i ½ wavelength long (though antenna f is l th l (th ht engineers can play tricks to reduce antenna size further). This l f th b Thi rule of thumb accounts for the huge size of t f th h i f radio broadcast antennas and the small size of mobile phones. An AM station broadcasting at 830 kHz has a wavelength of about 360 meters and a correspondingly large antenna But an 802.11b network interface operating in the 2.4-GHz band has a wavelength of just 12.5 centimeters. With some engineering tricks, an antenna can b incorporated into a PC Card, and a t be i t di t Cd d more effective external antenna can easily be carried in a backpack.
    8. Antenna Theory At Th A theoretical isotropic antenna has h a perfect 360º ft vertical and horizontal beamwidth This is a reference for ALL antennas
    9. Antenna Variables At V i bl Bandwidth Beamwidth Gain Polarization P l i ti Diversity Power
    10. Bandwidth B d idth The bandwidth of an antenna is the band of frequencies, over which it is considered frequencies to perform acceptably. The wider the range of frequencies a band encompasses, the wider the bandwidth of the antenna.
    11. Beamwidth B idth Beamwidth is a measurement used to describe directional antennas. Beamwidth is sometimes called half-power beamwidth. It is the total width in degrees of the main radiation lobe, at the angle where the radiated power has fallen below that on the centerline of the lobe, by 3 dB (half-power).
    12. Gain Gi
    13. Polarization P l i ti
    14. Polarization P l i ti cont. t
    15. Radiation Patterns R di ti P tt
    16. Dipole Antennas Di l A t
    17. Diversity Di it Space diversity
    18. Diversity cont. Di it t Frequency diversity
    19. Omnidirectional A t O idi ti l Antennas An omnidirectional antenna is designed to provide a 360 degree radiation pattern This type of antenna is used when yp coverage in all directions from the antenna is required. q
    20. Omnidirectional A t O idi ti l Antennas cont. t In a perfect world, all the omnidirectional antennas would radiate perfectly i all di ti t ld di t f tl in ll directions. Unfortunately, this is not the case. H-Plane E-Plane
    21. Omnidirectional A t O idi ti l Antennas cont. t
    22. Antenna Theory- Di l At Th Dipole Energy lobes are gy ‘pushed in’ from Side View the top and bottom ( (Vertical Pattern) ) Higher gain Vertical Beamwidth Smaller vertical New Pattern (with Gain) beamwidth Top View Larger horizontal (Horizontal Pattern) lobe Typical dipole pattern
    23. Directional A t Di ti l Antennas Lobes are pushed in a certain direction, causing Side View (Vertical Pattern) the energy to be co de sed condensed in a particular area Top View Very little energy is (Horizontal Pattern) in the back side of a directional antenna
    24. Directional A t Di ti l Antennas This type of antenna does not offer any added power to the signal, and instead simply redirects the energy it received from the transmitter. By redirecting this energy, it has the effect of providing more energy in one direction, and less energy in all other directions gy
    25. Directional t Di antennas l antennas cont. ti t Patch The patch antenna is great for indoor and outdoor applications. Mechanically they M h i ll th are small rectangles about a 1/2 i h thi k Th ll t l bt inch thick. The patch works well and fits aesthetically into most work environments. 6 dBi Patch Antenna – 65 degree
    26. Directional antennas cont. Di ti lt t Yagi antennas Yagi antennas are directional and designed for long distance communication Horizontal Vertical
    27. Directional antennas cont. Di ti lt t Solid dish antennas H-Plane H Pl E-Plane
    28. Back lobe d id lobes B k l b and side l b
    29. Beamwidth vs. G i B idth Gain
    30. High Gain Omni-Directionals Hi h G i O i Di ti l More coverage area in a circular pattern Energy level directly above or below the antenna will become lower
    31. Link Engineering and RF Path Planning
    32. Path Considerations P th C id ti Radio line of sight Earth bulge Fresnel zone
    33. Line f Sight Li of Si ht The following obstructions might obscure a visual li k i l link: Topographic features, such as mountains Curvature of the Earth C t f th E th Buildings and other man-made objects Trees Line of sight!
    34. Longer Di t L Distances Line of Sight disappears at 6 miles ( (9.7 Km) due to the earth curve )
    35. Fresnel Z F l Zone
    36. Fresnel Z F l Zone cont. t
    37. Improving F I i Fresnel Effect l Eff t Raise the antenna New structure Existing structure Different mounting point Remove trees
    38. Site to Sit F Sit t Site Fresnel Zone lZ Antenna Height Fresnel zone consideration Line-of-Sight over 25 miles (40 Km) hard to implement Antenna Height (Value (V l “H”) Total Distance Fresnel @ 60% (Value “F”) Earth Curvature (Value “C”)
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