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Radiotelemetry <br />THEORETICAL CONSIDERATIONS <br />TYPES OF TELEMETRY <br />Radiotelemetry has been used to monitor movements and other behavior of <br />terrestrial animals for many years. Earlier workers did not use radiotelemetry <br />for studying fish movement because it was believed that.radiotransmission <br />through water would be too poor to be effective. Most of this early work <br />involved use of ultrasonics (Stasko and Pincock 1977). The suitability of <br />using both techniques is evaluated below. <br />Ultrasonic Telemetry <br />Ultrasonic transmissions of high frequency sound waves have been success- <br />ful in many aquatic systems. Frequencies employed are usually between 30 and <br />200 kHz, which are not audible to the human ear. Ultrasonics have an advantage <br />over radiotransmissions for tracking fish under certain conditions. For <br />example, ultrasonic transmission range is not greatly affected by dissolved <br />solids. Also, a hydrophone (receiving collector) is generally more directional <br />than a conveniently sized radio antenna due to the shorter acoustic wavelengths <br />and the slower sound velocity. The slower velocity allows the pulse interval <br />to be used in computing the distance travelled from the transmitter to the <br />receiver (Stasko and Pincock 1977). <br />There are, however, several disadvantages of ultrasonic tracking. For <br />example, the detection of ultrasonic signals require that the receiving hydro- <br />phone be immersed in water. This makes tracking difficult with ice cover and <br />also eliminates the use of aircraft. Aircraft use may be essential in a large <br />river system, especially if numerous tagged fish are being tracked. <br />Ultrasonic telemetry is markedly influenced by water temperature, turbu- <br />lence, and sediment load. Temperature affects the velocity of ultrasonic <br />emmissions and a thermal discontinuity may reflect ultrasonic energy away from <br />the hydrophone (Sinning 1979). Entrained air from waves, boat propellers, and <br />turbines in dams may cause enough noise to mask ultrasonic reception, as does <br />the movement of bottom sediments caused by stream currents. The only known <br />use of ultrasonics in the Green River was marginally successful due to water <br />-- --ttrbulertc~- -and---t~ansm-l-ssisn--blacks b <br />ge--- y_sncks- end-__vegQtation __irMcAda_and <br />Wydowski 1980). <br />Radiotelemetry involves the generation (by a transmitter) and propagation <br />of radio waves (electromagnetic radiation) through water. The transmitted <br />energy must then cross the air-water interface and be received by an antenna <br />operating in air. Although radio frequencies of 10 kHz to 50 MHz have been <br />experimented with in water, frequencies between 40 and 160 MHz are usually <br />used. <br />The propagation of radio waves through any medium, in this case water, is <br />inversely proportional to the frequency. Thus, radio waves of high frequency <br />travel a given distance with a greater loss of power than an emission of lower <br />frequency. The nature of the change in propagation with frequency is approxi- <br />mately logarithmic (Lortsdale 1967; Lonsdale and Baxter 1968). Radio signals <br />are attenuated (diluted) more rapidly in water than air, and the amount of <br />attenuation is inversely proportional to the conductivity of the water (Weeks <br />et al. 1977). For this reason, a considerable loss of signal strength is <br />expected when radio waves are propogated through fresh water of high conduc- <br />tivity. Radio transmission in salt water is virtually impossible. <br />The behavior of radio energy at the air-water interface (Fig. 1) is an <br />important consideration for radiotelemetry. Energy contacting the interface <br />is reflected unless the angle of incidence is less than 6° (Weeks et al. <br />1977). Radiation of the energy that passes this interface produces a signal <br />with. the apparent signal source being a circle on the surface of the water <br />(Priede 1980). <br />The preceding explanation does not account for the reflection of radio <br />energy from~the water surface to the bottom and back through the surface, or <br />radiation from anything other than a smooth surface. However, these additional <br />effects result in a signal being emitted from the surface in a pattern dif- <br />ferent from that predicted by theory. Sinning (1979) noted that the U.S. <br />Navy, which experimented with subsurface radio emissions for over 30 years, <br />uses a surface antenna for submarines. This is evidence of the difficulties <br />with long distance underwater radio transmissions yet to be solved. <br />Factors, other than the propagation of radio transmissions through water, <br />must also be considered. The most obvious one is the strength of the emitted <br />radio signal. The range of a signal is directly proportional to the power of <br />the transmitter. Power radiated by the transmitter is a function of the <br />efficiency of both the transmitter and the transmitting antennas. These <br />efficiencies are typically 65 to 70% for underwater applications when the <br />radiated transmitter output is contrasted with battery power ehtering the <br />transmitter (Sinning 1979). <br />Antenna efficiencies (Terman 1955) can be lower (less than 1% to 25%) <br />i;han--transma~te~-P#ficienciES.-~nlhe~-lnss~sf_effisSencies_for_transmitters_ _ _ <br />- ---- <br />and antennas are combined, antenna efficiency may range from less than 1% to <br />18% of the battery power. <br />