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A transmitter and receiver operate at \(100 \mathrm{MHz}\) are at the same level, and are separated by \(4 \mathrm{~km}\). The signal must diffract over a building half way between the antennas that is \(20 \mathrm{~m}\) higher than the direct path between the antennas. What is the attenuation (in decibels) due to diffraction?

Short Answer

Expert verified
The attenuation due to diffraction is approximately 89.3 dB.

Step by step solution

01

Calculate the wavelength

First, find the wavelength (\textlambda\text) using the speed of light (\text c\text) and the frequency (\text f\text): \[ \textlambda = \frac{c}{f} \] where \[ \text c = 3 \times 10^8 \text{ m/s}, \ f = 100 \text{ MHz} = 100 \times 10^6 \text{ Hz} \] So, \[ \textlambda = \frac{3 \times 10^8 \text{ m/s}}{100 \times 10^6 \text{ Hz}} = 3 \text{ m} \]
02

Calculate the Fresnel Zone parameter (F)

The Fresnel Zone parameter (\text F\text) is given by: \[ \text F = \frac{\text h \times \text d_1 \times \text d_2}{\textlambda (\text d_1 + \text d_2)} \] where \[ \text h = 20 \text{ m}, \ d_1 = \frac{4 \text{ km}}{2} = 2 \text{ km} = 2000 \text{ m}, \ d_2 = 2000 \text{ m}, \ \textlambda = 3 \text{ m} \] Substitute these values: \[ \text F = \frac{20 \times 2000 \times 2000}{3 \times (2000 + 2000)} = \frac{80,000,000}{6000} = 13333.33 \text{ m}^{-1} \]
03

Calculate the Fresnel-Kirchhoff Diffraction parameter (v)

The Fresnel-Kirchhoff diffraction parameter (\text v\text) is calculated by: \[ \text v = \text F^{1/2} \] Substitute \text F\text from the previous step: \[ \text v = (13333.33)^{1/2} \] Using a calculator, you get: \[ \text v \text ≈ 115.42 \]
04

Calculate the diffraction loss (L)

The attenuation due to diffraction (\text L\text) in decibels is given by: \[ \text L = 6.9 + 20 \text{log} (\text v - 0.1)^2 +1 \] Substituting \text v ≈ 115.42 \: \[ \text v - 0.1 = 115.32, \ \text (115.32)^2 = 13300 \] So, \[ L = 6.9 + 20 \text{log} \frac{13300}{1} \] Using a calculator for the log: \[ \text{log} 13300 ≈ 4.12 \] Substitute back: \[ L = 6.9 + 20 \times 4.12 \] \[ L ≈ 6.9 + 82.4 \] \[ L ≈ 89.3 \text{ dB} \]

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Wavelength Calculation
The wavelength of a wave (\textlambda) is an essential component in understanding various electromagnetic principles. For radio waves at a given frequency, this is calculated using the formula: \textlambda = \frac{c}{f}. Here, \text c\text is the speed of light, which equals 300,000,000 meters per second (\text m/s\text), and \text f\text is the frequency of the wave. For a frequency of 100 MHz (100 million Hertz), the wavelength is: \[ \text\textlambda = \frac{3 \times 10^8 \text{ m/s}}{100 \times 10^6 \text{ Hz}} = 3 \text{ m} \]. Recognizing how to compute wavelength is vital for calculating other parameters, such as the Fresnel Zone.
Fresnel Zone Parameter
The Fresnel Zone is a key concept when studying wave propagation and diffraction. It helps to understand the regions around the direct line of sight between the transmitter and receiver where constructive and destructive interference occurs. The first Fresnel Zone radius at a given point between the transmitter and receiver is defined, calculated as: \[ \text F = \frac{\text h \times \text d_1 \times \text d_2}{\textlambda (\text d_1 + \text d_2)} \]. For our example: \text h = 20 meters, \text d_1 = 2000 meters, \text d_2 = 2000 meters, and \textlambda = 3 meters, it calculates to: \[ \text F = \frac{20 \times 2000 \times 2000}{3 \times (2000 + 2000)} = \frac{80,000,000}{6000} = 13333.33 \text{ m}^{-1} \]. This parameter helps in defining how much the signal is obstructed by an object.
Fresnel-Kirchhoff Diffraction Parameter
The Fresnel-Kirchhoff diffraction parameter (\text v\text) indicates the level of diffraction that occurs when a wave encounters an obstacle. It is derived from the square root of the Fresnel Zone parameter, \text F: \[ \text v = \text F^{1/2} \], which in our calculation is: \[ \text v = (13333.33)^{1/2} \text ≈ 115.42 \]. Higher values of \text v\text correspond to larger obstacles in the path of the wave, leading to stronger diffraction effects. Understanding this parameter lets you predict how much the wave will bend around objects and potentially reach the receiver beyond direct line-of-sight.
Diffraction Loss
Diffraction loss (\text L), measured in decibels (dB), quantifies the reduction in signal strength due to wave diffraction. It’s computed using: \[ \text L = 6.9 + 20 \text{log} [( \text v - 0.1)]^2 +1 \]. Using our parameter \text v ≈ 115.42: \[ \text v - 0.1 = 115.32,\text (115.32)^2 = 13300 \]. Thus: \[ L = 6.9 + 20 \text{log} \frac{13300}{1} \], leading to: \[ L ≈ 89.3 \text{ dB} \]. Knowing diffraction loss is essential for designing communications systems that account for potential signal obstructions and ensuring reliable transmission quality.

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Most popular questions from this chapter

A communication system operating at \(2.5 \mathrm{GHz}\) includes a transmit antenna with an antenna gain of \(12 \mathrm{dBi}\) and a receive antenna with an effective aperture area of \(20 \mathrm{~cm}^{2}\). The distance between the two antennas is \(100 \mathrm{~m}\). (a) What is the antenna gain of the receive antenna? (b) If the input to the transmit antenna is \(1 \mathrm{~W}\), what is the power density at the receive antenna if the power falls off as \(1 / d^{2},\) where \(d\) is the distance from the transmit antenna? (c) Thus what is the power delivered at the output of the receive antenna?

On a resonant antenna a large current is established by creating a standing wave. The current peaking that thus results establishes a strong electric field (and hence magnetic field) that radiates away from the antenna. A typical dipole loses \(15 \%\) of the power input to it as resistive \(\left(I^{2} R\right)\) losses and has an antenna gain of \(10 \mathrm{dBi}\) measured at \(50 \mathrm{~m}\). Consider a base station dipole antenna that has \(100 \mathrm{~W}\) input to it. Also consider that the transmitted power density falls off with distance \(d\) as \(1 / d^{3}\). Hint, calculate the power density at \(50 \mathrm{~m}\). [Parallels Example 4.2\(]\) (a) What is the input power in \(\mathrm{dBm} ?\) (b) What is the power transmitted in \(\mathrm{dBm} ?\) (c) What is the power density at \(1 \mathrm{~km} ?\) Express your answer as \(\mathrm{W} / \mathrm{m}^{2}\). (d) What is the power captured by a receive antenna (at \(1 \mathrm{~km}\) ) that has an effective antenna aperture of \(6 \mathrm{~cm}^{2} ?\) Express your answer in first \(\mathrm{dBm}\) and then watts. (e) If the background noise level captured by the antenna is \(1 \mathrm{pW}\), what is the SNR in decibels? Ignore interference that comes from other transmitters.

A transmit antenna and a receive antenna are separated by \(1 \mathrm{~km}\) and operate at \(1 \mathrm{GHz}\). What is the radius of the first Fresnel zone at \(0.5 \mathrm{~km}\) from each antenna?

Two identical antennas are used in a pointto-point communication system, each having a gain of \(50 \mathrm{dBi}\). The system has an operating frequency of \(28 \mathrm{GHz}\) and the antennas are at the top of masts \(100 \mathrm{~m}\) tall. The RF link between the antennas consists only of the direct line-of- sight path. (a) What is the effective aperture area of each antenna? (b) How does the power density of the propagating signal rolloff with distance. (c) If the separation of the transmit and receive antennas is \(10 \mathrm{~km},\) what is the path loss in decibels? (d) If the separation of the transmit and receive antennas is \(10 \mathrm{~km},\) what is the link loss in decibels?

An antenna operating at \(28 \mathrm{GHz}\) has an antenna gain of \(50 \mathrm{dBi}\). What is the effective aperture area of the antenna?

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