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Basic Radio Wave Propagation Theory
basic radio wave propagation theory
















Radio waves can get to the Moon and back in 2 ½ seconds or circle the Earth in 1/7 second. It also deals with features.Radio waves are just another form of light that travels at the same speed 186,000 miles per second. Radio Waves Propagation Radio propagation is a term used to explain how radio waves behave when they are transmitted, or are propagated from one point on the Earth to another.Large fires have an effect of suppressing Very or Ultra High FrequencyPDF This paper provides a survey of the basic mechanisms which influence the propagation of electromagnetic waves at most. RADIO WAVES PROPAGATION Definition Radio waves propagation is a term used to explain how radio waves behave when they are transmitted, or are propagated from one point on the Earth to another.

High annual rainfall, which is over a 1000 mm and high soil fertility, makes it suitable for sugar cane farming. The radio wave interferometer measured signalAttenuation of 0.43 dB through the fire with maximum temperature and flame depthReceived 20 January 2016 accepted 18 July 2016 published 21 July 2016The Burdekin Delta is known for its high sugar cane (Saccharum spp.) crop yield in Australia. As atmospheric pressure ionized medium (combustion plasma),Sugarcane fire has momentum transfer electron-neutral collision frequency muchHigher than plasma frequency, hence propagation of VHF/UHF radio waves throughSuch a medium is predicted to suffer a significant attenuation and phase shift.Radiowave propagation measurements were carried out in a moderate intensityPrescribed sugarcane fire at 151 MHz frequency over a 590 m path using aRadiowave interferometer. Plume species which include graphitic carbon,Alkalis and thermally excited radicals such as methyl are responsible forIonization. One of the causes of signal attenuation in fireEnvironment is plume ionization. MobileHand-held radio operating at the frequency ranges is a major communication toolDuring fire suppression therefore inefficient radio communication systems putLives of fire fighters at risk.

basic radio wave propagation theory

Moist combustion conditions prevail in the cane fires. Cool night air quenches the heat in the flame to temperatures lower than 1000˚C. The fires move rapidly and turbulently mix with convected surrounding air. Potassium, which exists in cane foliage, is volatilized by the intense heat and drawn by convective currents into the flame where it is thermally ionized to give electrons. In instances where cane fires get out of control, radio wave communication systems which are commonly used in fire suppression should be able to function effectively under such environment.Sugarcane fire flame temperatures are in the range of 600˚C - 1000˚C.

Phase change measurement involves running a reference signal from a transmitter to receiver circuits for phase comparison. The measurements were performed using a radio wave interferometer, an instrument specifically designed to measure attenuation or phase change of a radio wave signal after passing through a fire plume. Potassium contributes significantly to ionization in the fires provided flame temperatures are higher than 900˚C.The paper reports on radio wave propagation measurements carried out in a prescribed agricultural fire in a sugarcane field at Australian Tropical Agriculture College (ATAC) in Clare, Lower Burdekin.

Equation (1) can therefore be expressed as:Figure 1. According to Akthar , propagation constant (γ) is related to attenuation (a) and shift (b) coefficients in a medium by the relation γ = a + i(b). However in this experiment, phase measurements were not possible because the sides of the sugarcane paddock were very long to consider running a reference signal cable.If a plane polarized electromagnetic wave is considered to travel in the positive x-direction, its signal strength (E) at any given time can be given as Where γ is propagation constant, ω is cyclic propagation frequency (=2pf) and E 0 is initial electric field strength of the radio signal.

Clare is 90 km south of Townsville in the Burdekin Delta (19˚35'S and 147˚24'E) ( Figure 2). Attenuation (Attn) of the signal that traverses canefire expressed in dB is The sugarcane paddock where the prescribed burn was carried out was at the Burdekin Agricultural College in Clare. Amplitude of a radio signal that propagates through a sugarcane fire is attenuated and is given by Without a canefire intercepting the propagation path, the amplitude of the signal that traversed air is not attenuated, and is given by As attenuation coefficient (a f) is zero (0). The two effects in a lossy medium are measurable and can be related to those in free space. Dielectric permittivity of vacuum is equal to unity. The induced phase shift and loss in signal are due to electric dielectric permittivity which is not equal to unity (1).

Its leaves in the bottom 3 m were fully dried while those in the rest of height of straw were half dried. This fertile soils and the high rainfall in the regions makes it suitable for sugar cane farming.The sugarcane considered for harvesting was a year old (mature) and nearly 6 m tall. The soils are fertile alluvial with variable layering. Average rainfall in the region is 1032 mm. The climate in the area is monsoonal with hot wet summers and warm dry winters. The paddock is one of the 400ha of sugar cane paddocks owned by the Agricultural College.

The crops were closely packed and almost impossible for one to walk across the rows. 2002).In the paddock was 1 m. The location of the study area (adapted from: Charles worth et al.

The distance of Be to B f was 556 m. Tx was 30 m from BC such that Tx was 570 m from B 2. Rx was set 20 m from AB such that from B 1 to the Rx was 115 m. The units were set some distance away from the paddock so that they are not affected by heat from the burning sugarcane. The distance separating the units (Tx − Rx) was 581.5 m. The length of the paddock was roughly 1000 m and 100 m wide (see Figure 3).Receiver (Rx) and transmitters (Tx) units of a Radio Wave Interferometer were set up on adjacent sides of the sugar cane paddock (sides AB and BC in Figure 3).

The radio wave interferometer was switched on at 6.20 pm while the HOBO data logger was switched on at 6.24pm to allow the instrument to stabilize.The sugarcane fire was ignited along the side AB ( Figure 3) with liquid flame. Signal strength readings at Rx were then logged into HOBO â data logger for continuous monitoring.The Tx and Rx units were enclosed in polystyrene boxes wrapped with aluminum foil to reflect heat from cane fire. The antennas were tuned such that the maximum strength received at Rx was 689 mV.

To the steel pipe stem, six steel pipes of diameter 20 cm were screwed to the stem forming “branches” at every 1.0 m of the stem height. The tower was erected inside the paddock, a few meters from its edge. The wind forced the fire to propagate along the length of the paddock thus intercepting the propagation path (shown in Figure 3) at an angle of approximately 79˚.A thermocouple tower of height 6.1 m was constructed from a steel pipe (stem) of diameter 0.15 m.

The thermocouples wires were buried in a trench 20 cm deep and connected to the SPECTRUM â data logger 50 cm away from the tower.The thermocouples were wired to a SPECTRUM â SP 1700 - 51 W thermocouple data logger to read in temperatures throughout the experiment. The thermocouples were then fixed to branches by means of muffler tape and the electro-fused junctions were left protruding 2.5 cm beyond the branch length into the flame. The type K thermocouple wires were electro-fused at one end to make perfect junctions and tested with a hot air gun and a multimeter. Set up for the transmitter and receiver units at the study site.The thermocouples were cut from a 100 m roll of double braided fiberglass insulated chromel-alumel (24-G/G) thermocouple wire 50 mm in diameter.

The error is mainly due to the convection and radiation heat transfer to and from thermocouple bead. SP 1700-51w logger has the capability to read temperatures up to 1370˚C, therefore is ideal for measuring cane fire flame temperatures.There is a discrepancy between the actual combustion gas temperature and that measured by a bare bead thermocouple. The data logger was dug 75 cm into ground and wrapped around with an insulating material (Fiberflex â) to protect it from heat that may the produced in the grassfire.

basic radio wave propagation theory