22-Elec-B3 Digital Communications Systems · December 2019
Question 3 of 5: Link Budgeting
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. National Examinations — December 2019, 16-Elec-B3 Digital Communication Systems. Three hours, closed book; an approved Casio or Sharp calculator is permitted. Five questions of 25 marks each are printed; any four constitute a complete paper worth 100 marks, and only the first four appearing in the answer book are marked. All five questions are solved here, because this set is a study resource rather than a marked script. Note 1 of the cover page invites the candidate to submit a clear statement of any assumption made where a question is open to interpretation — that licence is used explicitly in Question 3(a).
Reference texts.
S. Haykin, Communication Systems, 5th ed. — matched filtering and optimum detection, noise power spectral density, sampling and quantisation.
B. P. Lathi and Z. Ding, Modern Digital and Analog Communication Systems, 4th ed. — PCM, aliasing, spread spectrum, link power budgets.
B. Sklar, Digital Communications: Fundamentals and Applications, 2nd ed. — convolutional coding and the Viterbi algorithm, communications link analysis, spread-spectrum techniques.
J. G. Proakis and M. Salehi, Digital Communications, 5th ed. — correlation receivers, error probability in AWGN, trellis decoding.
$30\log_{10}(4\pi d f/c)$, $f = 5$ GHz, $c = 3.0\times10^8$ m/s
Find. (a) the maximum path loss the link can tolerate while still meeting the SNR requirement with the stated margin; (b) the range at which that loss is reached; (c) the path-loss exponent implied by the model; (d) −30 dBm converted to watts.
Check: two readings of the source, both answered. The paper prints “antenna gains of 3 dB” — plural noun, single value. The natural engineering reading, and the one used for the boxed answers below, is 3 dB at each end, i.e. $G_t + G_r = 6$ dB of antenna gain in the budget. A reader who instead takes the 3 dB as the combined figure obtains a maximum path loss of 134.03 dB and a range of 140.2 m; both variants are carried through the working so either marking scheme can be followed. Note also that the quantity labelled “receiver noise figure of −174 dBm/Hz” is dimensionally a noise power spectral density, not a noise figure — −174 dBm/Hz is exactly $kT_0$ at $T_0 = 290$ K — so it is integrated over the bandwidth rather than added as a dB penalty. Cover-page Note 1 invites exactly this kind of stated assumption.
Approach. Convert everything to dB units referred to 1 mW, form the noise power in the 10 MHz bandwidth, add the SNR requirement and the fading margin to obtain the minimum acceptable received power, and take the difference between transmitted and required received power after gains and losses. Then invert the given path-loss law for distance, read the exponent off its coefficient, and convert dBm to watts from the definition.
Part (a) — put the transmit power in dBm. The dBm scale is referred to 1 mW, so $P_t = 8$ W $= 8000$ mW gives
$$P_t\,[\text{dBm}] = 10\log_{10}(8000) = \boxed{39.03\ \text{dBm}}$$
A useful mental check: 1 W is $+30$ dBm and a factor of 8 is $3 \times 3 = 9$ dB, so 8 W is about 39 dBm.
Compute the receiver noise floor. The noise power in a bandwidth $B$ follows from the power spectral density by integration, which on a logarithmic scale is an addition:
$$N\,[\text{dBm}] = N_0\,[\text{dBm/Hz}] + 10\log_{10} B = -174 + 10\log_{10}(10\times10^{6}) = -174 + 70 = -104\ \text{dBm}.$$
This is the thermal noise floor of a 10 MHz channel at room temperature, and it is the reference against which the SNR requirement is measured.
Set the minimum acceptable received power. The receiver must sit at least $\mathrm{SNR}_{\text{req}}$ above the noise floor, and the fading margin is extra headroom held in reserve for the deepest fades the link must survive:
$$P_{rx,\min} = N + \mathrm{SNR}_{\text{req}} + M = -104 + 3 + 3 = -98\ \text{dBm}.$$
Close the budget and solve for the allowed path loss. Following the signal from the transmitter to the detector, every gain adds and every loss subtracts:
$$P_{rx} = P_t + G_t + G_r - L_{rx} - L_{\text{path}} \;\ge\; P_{rx,\min}.$$
Rearranging for the largest loss the link can absorb and substituting the primary reading $G_t = G_r = 3$ dB,
$$L_{\text{path,max}} = P_t + G_t + G_r - L_{rx} - P_{rx,\min} = 39.03 + 3 + 3 - 6 - (-98)$$
$$\boxed{L_{\text{path,max}} = 137.03\ \text{dB}}$$
Under the alternative reading (3 dB of antenna gain in total) the same arithmetic gives 134.03 dB.
Part (b) — invert the path-loss law for distance. Setting the model equal to the allowance,
$$30\log_{10}\!\left(\frac{4\pi d f}{c}\right) = 137.03 \quad\Longrightarrow\quad \frac{4\pi d f}{c} = 10^{137.03/30} = 10^{4.5677} = 3.696\times10^{4}.$$
The frequency-dependent factor is
$$\frac{4\pi f}{c} = \frac{4\pi (5\times10^{9})}{3.0\times10^{8}} = 209.44\ \text{m}^{-1},$$
so the maximum range is
$$d_{\max} = \frac{3.696\times10^{4}}{209.44} = \boxed{176.5\ \text{m}}$$
Substituting back, $30\log_{10}(209.44 \times 176.46) = 137.03$ dB, which closes the loop. Under the 3-dB-total reading the range falls to 140.2 m — a 20 % reduction from a 3 dB change, which is the practical point of the exercise: at an exponent of 3 the range is only weakly sensitive to link-budget errors.
Part (c) — read the path-loss exponent from the coefficient. The general empirical path-loss law is written
$$L_{\text{path}}\,[\text{dB}] = 10\,n\log_{10} d + \text{constant},$$
where $n$ is the path-loss exponent. Expanding the given expression separates the distance dependence from the frequency dependence:
$$30\log_{10}\!\left(\frac{4\pi d f}{c}\right) = 30\log_{10} d + 30\log_{10}\!\left(\frac{4\pi f}{c}\right),$$
so matching coefficients gives $10n = 30$ and
$$\boxed{n = 3}$$
Equivalently, doubling the range costs $10n\log_{10} 2 = 9.03$ dB, against 6.02 dB for free space. An exponent of 3 sits between ideal free space ($n=2$) and a cluttered urban or indoor environment ($n \approx 3.5$–4), and describes a link with partial obstruction and ground reflection.
Part (d) — convert −30 dBm to watts. By the definition of the dBm scale, $P\,[\text{dBm}] = 10\log_{10}(P/1\,\text{mW})$, so inverting,
$$P = 10^{-30/10}\ \text{mW} = 10^{-3}\ \text{mW} = 10^{-3} \times 10^{-3}\ \text{W}$$
$$\boxed{P = 1\times10^{-6}\ \text{W} = 1\ \mu\text{W}}$$
The anchors make this a mental calculation: 0 dBm is 1 mW and every $-10$ dB is one decade, so $-30$ dBm is three decades below 1 mW, i.e. 1 µW.