1. CSE5807 Wireless and Personal Area Networks Lecture 2 Radio Communications Principles Chapters 2,5 and 11 Stallings

2. Communications Channel Capacity Channel capacity is the maximum rate at which data can be transmitted over a given communication path or channel, under given conditions of: –Bandwidth –Noise –Error rate

3. Communications Channel Capacity Data Rate – the rate, in bits per second (bps), at which data can be transmitted Bandwidth – the bandwidth of the transmitted signal as constrained by the transmitter and the nature of the transmission medium, in cycles per second, hertz Noise – the average white/thermal level of noise over the communications path Error Rate – the rate at which errors occurs eg 10 -6

4. Bandwidth Telephone Channel Frequency range is 300Hz to 3400Hz Bandwidth is 3400-300 = 3100Hz Transmitter/Receiver Telephone hand set Cable Two pair of wires

5. Nyquist Bandwidth Noise Free channel The rate of signal transmission is at least twice the bandwidth of a channel. C = 2*B (assumes 2-level signaling two states) Eg Bandwidth of 3100 Hz, C= 6200 bps

6. Nyquist Bandwidth Multi-level signaling (M, more than two states) C = 2Blog 2 M Eg Bandwidth of 3100 Hz and M = 64, C= 6200*log 2 64 = 37200 bps

7. Nyquist Bandwidth + More signaling levels = more data carried each signal interval - Noise and transmission system effects become more serious as M increases

8. Shannon Noise is an ever-present phenomenon in communications Need a way of representing the interaction of noise and data rate The amount of signal level compared to the noise is important in considering the possible data rates

9. Shannon A higher signal to noise ratio is equivalent to a high quality signal Measured in deciBels (1/10 th of a Bel) SNR dB = 10 log10 * (signal power/noise power)

10. Shannon Maximum channel capacity (taking signal to noise ratio into account): C = Blog 2 (1+SNR)

11. Gain/Loss Measurement power out Gain dB = 10 log 10 power in If the measured power out is less than the power in, then we have a loss and the formula will give a negative result. Often, the negative gain result is written as a Loss without the sign.

12. Gain/Loss Measurement power out Gain dBm = 10 log 10 1mW

13. Antenna Systems An antenna is a device that is used for radiating and/or collecting electromagnetic energy A receiving antenna may be one or more conductors that have electrical energy induced in them by the passage of Electro Magnetic Radiation A transmitting antenna causes EMR due to the electrical energy in the antennas conductor(s)

14. Antenna Systems An antenna will radiate power in all directions but, typically, does not performance equally well in all directions A common way to characterize the performance of an antenna is the radiation pattern

15. Isotropic Antenna (Idealised) Omnidirectional - A point source that radiates power in all directions equally – fig 5.1(a) Directional - preferred direction of radiation along one axis – fig 5.1(b)

16. Relative Power To determine relative power in a given direction a line is drawn from the antenna position at the appropriate angle, and the point of intercept with the radiation pattern is determined

17. Relative Power Fig 5.1 shows a comparison of two transmission angles, A and B. Fig 5.1(a) vectors A and B of equal length Fig 5.1(b) vector B is longer then vector A Comments ?

18. Beam Width When we measure the directivity of an antenna, we often describe this as the beam width. It is the angle within which the power radiated by the antenna is focused This is usually found by measuring the power in the preferred direction and then discovering where this power level drops to half the value of the preferred direction

19. Reception Pattern When an antenna is used for reception the radiation pattern becomes a reception pattern

20. Antenna Wavelength We usually measure the antenna by its wavelength λ This is calculated using the following formula λ = where v is the speed of light 3 x 10 8 m/s f v

21. Antenna Wavelength Frequency of transmission f = 12 GHz V = 3 x 10 8 metres/second Wavelength λ = 3 x 10 8 /12 x 10 9 =- 0.025 metres

22. Antenna Types - Dipoles Half-wave dipole Consists of two straight collinear conductors of equal length, separated by a small gap The length of the antenna is one half the wavelength of the signal that can be transmitted most efficiently

23. Antenna Types Half-wave Dipole

24. Antenna Types - Dipoles Quarter-wave dipole A vertical quarter wave antenna is the type commonly used for car and portable radios

25. Antenna Types Quarter-wave antenna

26. Radiation Patterns

27. Antenna Types Parabolic Antenna

28. Radiation Pattern – Parabolic Antenna

29. Antenna Gain Is a measure of the directionality of an antenna. Antenna gain is defined as the power output, in a particular direction compared to that produced in any direction by a perfect isotropic omnidirectional antenna If an antenna has a gain of 3dB, that antenna improves on the isotropic antenna in that direction by 3dB, or a factor of 2 (10 0.3 ) The increased power radiated in a given direction is at the expense of other directions

30. Propagation Modes – Ground Wave Follows contour of the earth, can propagate considerable distances The electromagnetic wave induces a current in the earth’s surface, the result of which is to slow the wave front near the earth, causing the wave front to tilt downward and hence follow the earth’s curvature AM Radio Below 2MHz

31. Propagation Modes Ground Wave

32. Propagation Modes – Sky Wave A signal from an earth based antenna is reflected from the ionized layer of the upper atmosphere back down to earth Signal can travel through a number of hops, bouncing back and forth Signal can be picked up thousands of kms from transmitter CB radio, BBC 2 to 30MHz

33. Propagation Modes Sky Wave

34. Propagation Modes – Line of Sight Above 30MHz neither ground nor sky wave propagation operate Signal can be transmitted between earth station and satellite overhead that is not beyond the horizon For ground based communication transmitting and receiving antennas must be within an effective line of sight of each other

35. Propagation Modes – Line of Sight Maximum distance d between two antennas of height h 1 and h 2 for LOS propagation is: d = 3.57(√Kh 1 + √Kh 2 ) Where K=1 for optical LOS and K= 1.33 for radio LOS What is maximum d between two antennas for LOS if h 1 = 100m and the other antenna is at ground level?

36. Propagation Modes Line-of-Sight

37. Propagation Modes Refraction

38. Polarization The polarization of an antenna is the orientation of the electric field of the radio wave with respect to the Earth's surface and is determined by the physical structure of the antenna and by its orientation. A simple straight wire antenna will have one polarization when mounted vertically, and a different polarization when mounted horizontally

39. Polarization For line-of-sight communications for which polarization can be relied upon, it can make a large difference in signal quality to have the transmitter and receiver using the same polarization Many tens of dB difference are commonly seen and this is more than enough to make the difference between reasonable communication and a broken link.

40. Diversity Antenna Systems Using two antennas located a distance apart can counteract the effect of signal loss due to propagation problems.

41. Transmission Problems Attenuation and Attenuation Distortion Free Space Loss Noise Atmospheric Absorption Multipath Refraction

42. Transmission Problems - LOS Fresnel Zone The higher the frequency of the transmission, the more it may be affected by obstructing objects. The possible interference is determined by computing the Fresnel Zone

43. Transmission Problems Fresnel Zone TransmitterReceiver radius S kmD km

44. Antenna Types Yagi A Yagi antenna consists of a driven element (1/2 –wave dipole) and one or more director elements (in the forward direction) and a reflector element (behind the driven element)