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YAGI ANTENNA DESIGN

3 CHAPTER DESIGN AND IMPLEMENTATION

3.5 YAGI ANTENNA DESIGN

The antenna parameters element lengths and spacing are given in terms of wavelength, so an antenna for a given frequency can be easily designed. The lengths of various antenna

elements are related to the frequency (f=106 MHz) is as follows:

Planned frequency of transmission f = 100MHz

The following equations will be used to derive the appropriate length of the elements that will make up the yagi antenna and the spacing between them. Fig 3.7 will be used as the

reference.

The equations for length of the elements are: [24]

First Director Length = 

4(BCD) --- (I)

22 Second Director Length = 

4(BCD) --- (II) Third Director Length = &

4(BCD) --- (III) Fourth Director Length = &6

4(BCD) --- (IV)

Dipole Length = $&

4(BCD) --- (V)

Reflector Length = 

4(BCD) --- (VI)

The Spacing between the elements can be found from the following equations: [24]

A = " Fourth Director Length = &6

 = 1.38 meters

23 C = &

 = 0.3 meters D = &

 = 0.3 meters E = $6

 = 0.48 meters

Figure 3.6 YAGI ANTENNA STRUCTURE [24]

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4 CHAPTER 4 TEST AND RESULTS

4.1 INTRODUCTION

This section will discuss tests carried out on the final circuit and the results obtained. Measured waveforms from the oscilloscope will be used to illustrate the performance at each stage of the circuit and the method used to evaluate the obtained result will be described.

4.2 TEST EQUIPMENT

At various stages of the circuit different test were required to confirm the performance of the stages. The following test tools were used:

a) Digital Multimeter: This is an electronic device used to measure continuity, voltage and current. The multimeter was particularly useful for measuring the base-emitter voltage of each transistor in order to verify if it was within the voltage range (i.e 0.6V to 0.7V) of the transistor active region.

b) Oscilloscope: This is a type of electronic test instrument that allows observation of constantly varying signal voltages with respect to time. It allows the observation of signal amplitude and the period of the signal. The oscilloscope was used to check if the oscillator part of the circuit was oscillating as desired. Also the performance of the audio amplifier and the output of the electret microphone was evaluated with the oscilloscope.

c) Analogue FM Radio Receiver: An analog FM receiver was required to tune to the transmitting frequency of the transmitter. The FM receiver will intercept the transmitted FM signal and demodulate it to reproduce the original sound input. With the FM radio receiver it was possible to determine the range of the FM transmitter and also its sound quality.

4.3 CONSTRUCTION AND ASSEMBLY TOOLS a) Cutting Plier

b) Flat Nose Plier c) Digital Multimeter

25 d) Soldering Iron and Lead

e) Small flat screw driver f) Drill Bit

4.4 CONSTRUCTION AND ASSEMBLY

The FM transmitter was built using discrete electronic components (such as resistors, capacitors, transistors) soldered on a vero board. The vero board was made up several vertical conducting strips, on which components were soldered. A drill bit was used to etch out sections of the strips where an electrical bridge was not wanted. The inductor was fabricated by winding 4 turns of a 2mm gauge copper wire on a threaded bolt; while the yagi antenna was constructed by cutting the elements of a ready-made yagi antenna to fit the design specification.

The circuit assembled on the vero board is placed into a handheld instrumentation case 90 × 65 × 25 cm in dimension. A hole is drilled at the top to accommodate the electret microphone, another hole is drilled by its side with an audio jack fitted for the purpose of accepting an external audio signal source. An output for the yagi antenna connection is made on the right side of the case while the power switch is mounted on the reverse side.

4.5 COMPONENT LIST a) Electret Microphone b) Resistor

Table 4.1 RESISTORS

Component Type Quantity Use

68 KΩ Carbon Film 1 Bias for electret

microphone

4.7 KΩ Carbon Film 4 Voltage divider DC-Bias

for carrier Oscillator

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10 KΩ Carbon Film 1 Provide Modulating

voltage

c) Capacitors

Table 4.2 CAPACITORS

Component Value Type Quantity Use

47 nF Ceramic 2 For stabilising D-C input

voltage

22 pF Ceramic 2 Feedback Capacitor to

enhance voltage swing of Oscillator

22 µF Ceramic 1 Audio Coupling Capacitor

2 – 10 pF Variable

capacitor

1 Capacitance for tank

circuit

1 Inductance for tank circuit

e) Transistor

Table 4.4 TRANSISTORS

Component Value Type Quantity Use

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Component Value Type Quantity Use

BB204 Variable Capacitance

The following tests were carried out to evaluate the performance of the circuit.

I. Waveform Measurement

II. Voltage and current measurement III. Transmission Range

4.6.1 WAVEFORM MEASUREMENT

Fig 4.1 shows the combined waveform of the audio signal before amplification and after amplification. The upper waveform is the waveform measured at the collector of the first stage transistor, which is the output of the audio amplifier circuit. The bottom waveform is the waveform measured at the output of the electret microphone. The time per division setting was 1 milli-second; while the volts per division was 50 milli-volts.

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Figure 4.1 PRE-AMPLIFIED VS AMPLIFIED AUDIO WAVEFORM

Volts / Div

Time / Div 50

mV

1 ms

A comparison of the waveform shows a significant amplification of the audio signal, which is very important to achieve a better modulation index.

4.6.2 VOLTAGE AND CURRENT MEASUREMENT

The voltage and current at key parts of the circuit was measured in order to derive the actual power consumption of the circuit and also the amount of power generated in the tank circuit.

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Table 4.6 VOLTAGE AND CURRENT MEASUREMENT Operational

From the measurements in table 4.6, we can calculate the following:

Power Consumption = Vbattery × Icurrent = 9 × 165mA = 1485 mW Power in Tank circuit = 2 × Ic2 × Rinductor

Power in Tank circuit = 2 × (97 × 10-3)2 × 1 = 18.8 mW

4.6.3 TRANSMISSION RANGE MEASUREMENT

A FM receiver was used to demodulate the transmitted FM signal; a good quality audible message was received within a 30 meters radius of the FM transmitter. However the transistor’s performance degraded significantly as the collector’s current rises; this

significantly limited the transmission power and consequently the distance covered was also limited.

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5 CHAPTER 5 CONCLUSION AND RECOMMENDATION

5.1 CONCLUSION

A direct FM transmitter with a range up to 10 meters can be built using the varactor diode modulator approach to generate frequency modulated signal. Within the 10 meters range the quality of the sound produced was very good and the bandwidth of the generated FM signal appeared to be within the ±75KHz. This was crucial in producing a good quality sound output.

The addition of a Yagi antenna to boost the transmitting distance did not yield a significantly better result; it is suspected that the power generated by the circuit was insufficient to drive a yagi antenna, as the transistor became excessively hot with the addition of a yagi antenna and the FM signal produced degenerated.

5.2 LIMITATION

It was difficult to evaluate the generated frequency modulated signal, which is about 80MHz.

Measurement of the modulated waveform was not possible due to non-availability of an oscilloscope capable of measuring up to the 80 MHz frequency range.

5.3 RECOMMENDATION

The FM transmitter is highly susceptible to frequency drift when touched or moved from one place to another. It is recommended that the components on the circuit are closely put together, as it was discovered that frequency drifting was reduced in this way.

The performance of the circuit can also be improved by building it on a Printed Circuit Board (PCB) or a well etched out vero board. It was found that the audio sound produced was clearer when the unused conducting rails on the vero board were etched out or cut out. Vero boards have relatively high parasitic capacitance between their conducting rails; these parasitic capacitance do affect the general performance of the circuit.

It is believed that the performance of this circuit can also be improved, if a D-C power source was used instead of a battery to power the circuit; however this would increase the power

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dissipated by the transistors and a cooling fan will be required to prevent the transistors from getting damaged.

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REFERENCES

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http://radio.meteor.free.fr/us/antenna.html. [Accessed: 30-Jan-2016].

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6 APPENDIX

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