Aalto University School of Electrical Engineering ELEC ...
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Aalto UniversitySchool of ElectricalEngineering
ELEC-E4750Radiowave Propagation and ScatteringSession 6: Terrestrial and Satellite Links
ELEC-E475014.10.2020
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Aalto UniversitySchool of ElectricalEngineering
Aalto UniversitySchool of ElectricalEngineering
Schedule
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Wk Date Location Lectures, exercises and deadlines
42Mon. 12 Oct. Online Exercise return session 5Wed. 14 Oct. Lecture 6: terrestrial and satellite links
43Mon. 19 Oct. Exercise return session 6Wed. 21 Oct. Lecture 7: cellular links
44Mon. 26 Oct. Exercise return session 7Wed. 28 Nov. Lecture 8: radio channel characterization
45Mon. 02 Nov. Exercise return session 8Wed. 04 Nov. ELE lab Lecture 9: measurements and analysis
46Mon. 09 Nov. Online Exercise return session 9Wed. 11 Nov. Lecture 10: fading and radio link
performance
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Books, Topics and Exercises Books
Main books S. Saunders, Antennas and Propagation for Wireless Communication Systems, Chapters 3, 5,
6-8, 10, 12 15, Wiley. H. L. Bertoni, Radio propagation for modern wireless systems, Chapters 2-6, Prentice Hall. A. F. Molisch, Wireless Communications, Chapters 1, 5 and 8, Wiley. R. Vaughan and J. B. Andersen, Channels, propagation and antennas for mobile
communications, Chapter 3.2.1, IEE Press. Supplemental book
D. M. Pozar, Microwave Engineering, Chapters 1 and 14, Wiley.
Topic 6: Terrestrial and satellite links (Ch. 5 and 7, Ch. 4) Exercise 1: Two-ray multipath model Exercise 2: Rain attenuation
Topic 7: Cellular links (Ch. 12, Ch. 2) Exercise 1: Physical propagation modeling in microcells Exercise 2: Pathloss and small-scale fading
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Aalto UniversitySchool of ElectricalEngineering
Aalto UniversitySchool of ElectricalEngineering
Cellular Scenarios
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Satellite links(Mega cells)Macrocells
Microcells
Pico cells
Aalto UniversitySchool of ElectricalEngineering
Aalto UniversitySchool of ElectricalEngineering
Two-Ray Model of Radio Propagation
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Aalto UniversitySchool of ElectricalEngineering
Aalto UniversitySchool of ElectricalEngineering
Two-Ray Model of Radio Propagation
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For 𝑑𝑑 ≫ ℎb• Wave propagation distances of
line-of-sight and ground reflection becomes almost the same.
• Ground reflection becomes almost glazing incidence
• Reflection coeff. approaches +1 for “┴” pol and -1 for “||” pol.
𝜃𝜃
𝜃𝜃
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Q1: for a two-ray radio propagation, thereceived power behaves like the figure. Which explanation is incorrect?
A. Constructive and destructive addition of the two rays leads to the fluctuation.
B. A spatial standing wave is seen.C. The variation happens because radio waves are coherent.D. The variation looks exactly the same for horizontal and
vertical polarizations of the transmitted waves.
Figure: normalized received power with respect to the line-of-sight power E0
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Q2: for horizontal polarization where the reflection coefficient of the grazing incidence to the ground is -1, the received field at the RX isstronger than the line-of-sight field when
A. r1 + r2 - r0 = λ/2.B. r1 + r2 - r0 = λ.C. r1 + r2 - r0 = 2λ.D. r1 + r2 - r0 = 300λ.
λ: wavelength
Aalto UniversitySchool of ElectricalEngineering
Aalto UniversitySchool of ElectricalEngineering
Cellular Scenarios
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Satellite links(Mega cells)Macrocells
Microcells
Pico cells
Aalto UniversitySchool of ElectricalEngineering
Aalto UniversitySchool of ElectricalEngineering
Atmosphere Around Earth’s Surface
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Aalto UniversitySchool of ElectricalEngineering
Aalto UniversitySchool of ElectricalEngineering
Excess Losses in Satellite Linksin reference to free-space loss
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Effects of non-ionized atmosphere• Absorption in gases• Absorption, scattering and
depolarization by hydrometeors • Antenna beam-divergence due to
refraction• Scintillation due to time-varying
reflective index• Attenuation due to objects around
earth station, e.g., buildings and trees
• Critical for > 1 GHz RF and low elevation angles
• ITU-R P.618
Effects of ionized atmosphere• Critical frequency due to
change of refractive index• Change of polarization states
due to Faraday rotation• Group delay dispersion• Scintillation due to time-
varying reflective index• Critical for < 1 GHz radio
frequency (RF)• ITU-R P.531
Aalto UniversitySchool of ElectricalEngineering
Aalto UniversitySchool of ElectricalEngineering
Ionosphere
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… is a region of ionized plasma; ions are trapped in the Earth’s magnetic field.
Electromagnetic radiation of the sun makes the ionization.
Aalto UniversitySchool of ElectricalEngineering
Aalto UniversitySchool of ElectricalEngineering
Ionosphere Effects on Radio Propagation
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• Key parameter: electron concentration per cubic meter N
• The electron concentration influences the refractive index:
(Critical frequency)
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A. At the critical frequency,the refractive index is almost 0.
B. Refractive index is smaller at night than in a day inionosphere.
C. Radio waves from the ground do not penetrate the ionosphere below the critical frequency.
D. The densest ionization leads to higher critical frequency.
Q3: Which statement is wrong?
Aalto UniversitySchool of ElectricalEngineering
Aalto UniversitySchool of ElectricalEngineering
Tropospheric Refraction
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Gaseous Absorption
Oxygen atom
Hydrogen atom
Watervapor
Oxygen molecules have quantized rotational energy state (resonances). They have energy corresponding to energy quantum with wavelength of approximately 5 mm.
Oxygen molecule
Aalto UniversitySchool of ElectricalEngineering
Aalto UniversitySchool of ElectricalEngineering
Rain Attenuation• Which level of rain attenuation is most problematic for
satellite links?
17Khan et al., TAP 2003.
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Q4: When discussing the rain attenuation,we usually care a rainfall rate of
A. The smallest 1 % value of a year.B. A mean value of a year.C. A median value of a year.D. The largest 1% value of a year.
Aalto UniversitySchool of ElectricalEngineering
Aalto UniversitySchool of ElectricalEngineering
Outage Probability due to Rain Attenuation
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• Heavy rain fall rate produces the most severe attenuation.
Khan et al., TAP 2003.
Correction factor
1 % most severe rainattenuation
Aalto UniversitySchool of ElectricalEngineering
Aalto UniversitySchool of ElectricalEngineering
Rain Attenuation and Path Length
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… is proportional to total rainy slant path length rR.
The effective rain height hR varies
for latitude.
The length rRdepends on local cloud distribution.
Aalto UniversitySchool of ElectricalEngineering
Aalto UniversitySchool of ElectricalEngineering
Depolarization due to Hydrometeor
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Attenuation depends on the polarization direction with respect to orientation of the hydrometeor.
XPD proportional to rain attenuation loss,(Reasonably accurate above 10GHz)
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Q5: which statement is wrong?A. Rain attenuation depends on the radio frequency.B. Low elevation satellite path is influenced by more
rain attenuation than high elevation satellite path.C. Rain attenuation is polarization-selective.D. Greater link margin is required in the mild climate
areas than in tropical areas.
Aalto UniversitySchool of ElectricalEngineering
Aalto UniversitySchool of ElectricalEngineering
Improving the Outage - Diversity
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Rain cell sizeRain cell size
ff f
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Q6: which one is right as to the diversity in satellite links?
A. Use of multiple radio frequencies in a single ground station is as effective as having multiple ground stations to attain link diversity.
B. A second ground station placed just next to the first ground station leads to low correlation of rain attenuation between the two links.
C. If correlation of rain attenuation between two links is low, there is no improvement of outage.
D. Two ground stations must be separated much greater than the average rain cell size of the site to leverage diversity efficiently.
Aalto UniversitySchool of ElectricalEngineering
Aalto UniversitySchool of ElectricalEngineering
Forthcoming Contact Sessions• Learning outcomes of the exercise problems for topic 7 are to
– Get familiarized with physical propagation modeling in an urban street canyon (problem 1)
– Understand characteristics of pathloss and small-scale fading (problem 2)• During the contact sessions, you
– solve the exercise problems by referring to relevant parts of the course books.• a limited number of course books are available in the room.
– are encouraged to discuss with other students and teachers.– should contact teachers once your solutions are ready.
• if you prepare exercise solutions in an electronic format (recommended), upload the solution to MyCourses first and then contact teachers.
– will propose points for your ready solutions to the teachers.– will not get exercise points without discussing with teachers!
• The discussions MUST happen in the contact sessions.– Are reminded that six exercise problems must be completed in total before the
end of the next Monday session on 19th October.