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01 — Noise & Sensitivity

Noise & Sensitivity

Thermal Noise Power
P = kTB (watts)
= −174 dBm/Hz at T=290 K
Noise floor (dBm) = −174 + 10·log(B[Hz])
k=1.381×10⁻²³ J/K · T=290 K · B=bandwidth in Hz
Noise Figure & Noise Temperature
NF = 10·log(F) dB · F = SNR_in/SNR_out
T_e = 290·(F−1) K
F = 1 + T_e/290
NF=3 dB → F=2 → T_e=290 K · NF=0.5 dB → T_e=35 K
Friis Cascaded NF
F_total = F₁ + (F₂−1)/G₁ + (F₃−1)/G₁G₂ + …
All linear (not dB) · First stage dominates
Loss L before LNA: F_sys = L·F_LNA (first stage = attenuator+LNA)
Receiver Sensitivity
S_min = −174 + NF + 10·log(B) + SNR_min
All in dB/dBm · B in Hz
WiFi 20 MHz, NF=5, SNR=10: −174+5+73+10 = −86 dBm
P1dB & IIP3
IIP3 = P_in + ΔIM3/2 (dBm)
OIP3 = IIP3 + G
P1dB_in ≈ IIP3 − 9.6 dB (theoretical)
ΔIM3 = P_fund − P_IM3 (output, dBc) · measured in 2-tone test
Cascaded IIP3 & SFDR
1/IIP3_tot = 1/IIP3₁ + G₁/IIP3₂ + …
SFDR = (2/3)·(IIP3 − P_noise) dB
Last stage dominates IIP3 (opposite of NF) · high gain hurts IIP3
StandardBWNF (typ)SNR_minSensitivity
GSM 900200 kHz8 dB10 dB−103 dBm
LTE 10 MHz9 MHz7 dB−1 dB−98 dBm
WiFi 802.11n 20 MHz20 MHz8 dB4 dB−89 dBm
5G NR 100 MHz100 MHz7 dB1 dB−83 dBm
GPS L12 MHz3 dB−27 dB−135 dBm
Bluetooth LE2 MHz10 dB−3 dB−104 dBm
02 — Path Loss & Link Budget

Path Loss & Link Budget

Free-Space Path Loss (FSPL)
FSPL = 20·log(4πd/λ) dB
= 32.44 + 20·log(f[MHz]) + 20·log(d[km])
= 92.44 + 20·log(f[GHz]) + 20·log(d[km])
×2 distance → +6 dB · ×2 frequency → +6 dB
Friis Link Budget
P_RX = P_TX + G_TX + G_RX − FSPL − L
EIRP = P_TX + G_TX (dBm + dBi)
Link margin = P_RX − S_min (dB)
L = all other losses (cable, atmosphere, polarisation mismatch)
Log-Distance Path Loss
PL(d) = PL(d₀) + 10n·log(d/d₀) + X_σ
n = path loss exponent
X_σ = Gaussian shadowing (std dev σ dB)
Free space n=2 · Urban NLOS n=3–4 · Indoor n=1.6–4
3GPP 5G NR UMi LOS
PL = 32.4 + 21·log(d[m]) + 20·log(f[GHz])
UMa NLOS: 13.54 + 39.08·log(d) + 20·log(f)
InH LOS: 32.4 + 17.3·log(d) + 20·log(f)
3GPP TR 38.901 · f in GHz · d in metres
Rain Attenuation (ITU-R P.838)
3.5 GHz: ~0.03 dB/km at 25 mm/hr
28 GHz: ~4.5 dB/km at 25 mm/hr
60 GHz: ~6 dB/km rain + 15 dB/km O₂
O₂ peak at 60 GHz naturally limits range to ~200 m — used for secure links
Radar Range Equation
R_max = ⁴√(P_T·G²·λ²·σ / ((4π)³·S_min))
P_T=TX power · σ=RCS (m²)
SNR = P_RX / kTBNF
Radar: signal travels 2×range → path loss ∝ R⁴ not R²
ScenarioFreqDistanceFSPL
WiFi 2.4 GHz2.4 GHz50 m80 dB
WiFi 5 GHz5 GHz20 m82 dB
5G NR n783.5 GHz500 m117 dB
5G mmWave28 GHz200 m127 dB
GPS L11.575 GHz20,200 km182 dB
GEO Satellite Ku12 GHz35,786 km205 dB
03 — Transmission Lines

Transmission Lines

Characteristic Impedance
Z₀ = √(L/C) = √((R+jωL)/(G+jωC))
Lossless: Z₀ = √(L/C)  ·  50 Ω standard
Coax: Z₀ = (60/√εr)·ln(D/d)
Microstrip: use Hammerstad-Jensen · Stripline: use Wadell
Reflection & VSWR
Γ = (Z_L − Z₀)/(Z_L + Z₀)
VSWR = (1+|Γ|)/(1−|Γ|)
RL = −20·log|Γ| dB · Mismatch loss = −10·log(1−|Γ|²)
VSWR 2:1 → |Γ|=0.33 → RL=9.5 dB · mismatch loss=0.51 dB
Propagation
v_p = c/√εeff = 1/√(LC)
λ = v_p/f = c/(f·√εeff)
β = 2π/λ · γ = α + jβ
Microstrip FR4: εeff≈3.1 → v_p≈0.57c → λ at 2.4 GHz ≈ 71 mm
Input Impedance
Z_in = Z₀·(Z_L + jZ₀tanβl)/(Z₀ + jZ_Ltanβl)
λ/4 transformer: Z_in = Z₀²/Z_L
λ/2: Z_in = Z_L (repeats)
Open stub: Z_in=−jZ₀cotβl · Short stub: Z_in=jZ₀tanβl
Skin Depth & Conductor Loss
δ_s = 1/√(πfμ₀σ) metres
Copper at 1 GHz: δ_s ≈ 2.1 μm
R_s = 1/(σ·δ_s) = √(πfμ₀/σ) Ω/sq
δ_s ∝ 1/√f · At 10 GHz: 0.66 μm · Trace must be >> δ_s thick
Microstrip Quick Formulas
W/h > 2: Z₀ ≈ 120π/[√εeff·(W/h+1.393+…)]
εeff ≈ (εr+1)/2 + (εr−1)/2·(1+12h/W)^−½
50 Ω on FR4 (εr=4.4, h=1.6mm): W ≈ 3.0 mm
Thinner substrate → narrower trace → higher loss · use Rogers for mm-wave
Substrateεrtan δ50Ω W (h=1.6mm)Best use
FR44.2–4.60.018–0.025~3.0 mm≤3 GHz general
Rogers 4350B3.480.0037~3.5 mm3–20 GHz RF
Rogers 58802.200.0009~5.0 mmmmWave, <0.5 dB/cm
Alumina 96%9.80.0003~0.8 mmMicrowave ICs, hybrids
PTFE (Duroid)2.1–10.50.0002variesMicrowave, radar
04 — Antennas

Antennas & Arrays

Gain, Directivity & Efficiency
G = η·D · G(dBi) = 10·log(η·D)
EIRP = P_TX·G_TX (linear) = P_TX + G_TX (dBm+dBi)
Effective area: A_eff = G·λ²/(4π)
Isotropic = 0 dBi · λ/2 dipole = 2.15 dBi · Patch ≈ 5–8 dBi
Aperture Antennas
Parabolic dish: G = η·(πD/λ)² (η≈0.55–0.65)
Horn: G ≈ 10·log(10·A/λ²) dBi
HPBW ≈ 70·λ/D degrees
1m dish at 12 GHz: G ≈ 44 dBi · 3dB BW ≈ 1.75°
Patch Antenna
Resonant length: L ≈ λ/(2√εeff)
Width: W ≈ c/(2f)·√(2/(εr+1))
Gain ≈ 5–9 dBi · BW ≈ 2–5% (FR4)
2.4 GHz on FR4 (εr=4.4): L ≈ 29 mm · W ≈ 38 mm
Array Gain & Beamwidth
N elements: G_array = G_element + 10·log(N) dB
HPBW ≈ 0.886·λ/(N·d) rad
Grating lobe when d > λ/(1+|sin θ_s|)
64 elements: +18 dB · 128 elements: +21 dB · d=λ/2 is standard
λ/2 Dipole
Z_in ≈ 73 + j42.5 Ω at resonance
Gain = 2.15 dBi
Resonant length: L ≈ 0.475·λ (with end effect)
2.4 GHz dipole: L ≈ 59 mm · match to 50 Ω with balun + L-network
Yagi-Uda
Director: 0.4λ shorter than driven
Reflector: 5% longer than driven
Gain ≈ 10·log(0.5·N) dBi (N elements)
10-element: ≈7 dBi · 20-element: ≈10 dBi · spacing≈0.3λ
05 — S-Parameters

S-Parameters & Network Conversions

S-Parameter Definitions
S11 = b1/a1|a2=0 (input reflection, Z_out=Z₀)
S21 = b2/a1|a2=0 (forward transmission gain)
S12 = b1/a2|a1=0 (reverse isolation)
S22 = b2/a2|a1=0 (output reflection)
a = incident wave · b = reflected wave · all ports terminated in Z₀
Key Relationships
Gain (dB) = 20·log|S21|
RL (dB) = −20·log|S11|
Insertion loss = −20·log|S21|
Isolation = −20·log|S12|
S21=0.707 (−3dB) → 50% power · S21=0.5 → −6 dB · S21=2 → +6 dB
S → ABCD (Z₀=50 Ω)
A = ((1+S11)(1−S22)+S12S21)/(2S21)
B = Z₀·((1+S11)(1+S22)−S12S21)/(2S21)
C = (1/Z₀)·((1−S11)(1−S22)−S12S21)/(2S21)
D = ((1−S11)(1+S22)+S12S21)/(2S21)
S → Z-Parameters
Z11 = Z₀·(1+S11)(1−S22)+S12S21 / Δ
Z12 = Z₀·2S12 / Δ
Z21 = Z₀·2S21 / Δ
Z22 = Z₀·(1−S11)(1+S22)+S12S21 / Δ
Δ = (1−S11)(1−S22)−S12S21
S → Y-Parameters
Y11 = (1/Z₀)·(1−S11)(1+S22)+S12S21 / Δ
Y12 = (1/Z₀)·−2S12 / Δ
Y21 = (1/Z₀)·−2S21 / Δ
Y22 = (1/Z₀)·(1+S11)(1−S22)+S12S21 / Δ
Δ = (1+S11)(1+S22)−S12S21
Stability (Rollett)
K = (1−|S11|²−|S22|²+|Δ|²)/(2|S12S21|)
|Δ| = |S11S22−S12S21|
Unconditionally stable: K>1 AND |Δ|<1
μ = (1−|S11|²)/(|S22−ΔS11*|+|S12S21|) >1
μ > 1 is single-condition stability criterion (preferred)
S11 (dB)|Γ|VSWRMismatch Loss% Power reflected
−6 dB0.503.0:11.25 dB25%
−10 dB0.3161.93:10.46 dB10%
−15 dB0.1781.43:10.14 dB3.2%
−20 dB0.1001.22:10.044 dB1%
−30 dB0.0321.065:10.004 dB0.1%
06 — Filters

RF Filters

Filter Selectivity Comparison
Butterworth: Maximally flat · −3 dB at ωc
Attenuation (dB) = 10·log(1+(ω/ωc)^2n)
Chebyshev: Equiripple · steeper rolloff
Elliptic: Steepest rolloff · has notches
Butterworth: −20n dB/decade · Chebyshev: better by ~6 dB at octave
LC Ladder — Prototype to Scaled
L_scaled = L_proto · Z₀/ωc
C_scaled = C_proto / (Z₀·ωc)
BPF: L_series→L+C · C_shunt→L||C
BW ratio = ω₂/ω₁ = FBW
Element values from tables (Zverev, Matthaei) · Z₀=50 Ω standard
Resonator Q & Insertion Loss
IL_min ≈ 4.34·n·(ωc/BW)·(1/Q_u) dB
Q_loaded = f₀/BW_3dB
Q_external = 1/coupling factor
1/Q_L = 1/Q_u + 1/Q_ext
Higher Q_u → lower IL · Cavity Q≈10000 · LC Q≈50–200 · SAW Q≈1000+
Group Delay
τ_g = −dφ/dω (seconds)
Flat GD → linear phase → no pulse distortion
Bessel filter: maximally flat GD
GD variation: ΔGD = 1/BW (rough estimate)
1 ns GD variation over 1 GHz BW causes ISI · critical for wideband data
Filter TypeRolloffIn-Band RippleGroup DelayBest For
Butterworth−20n dB/dec0 dB (flat)Moderate variationGeneral purpose
Chebyshev ISteeper than BWε dB rippleWorse near band edgeSharp rejection needed
EllipticSteepestε dB rippleWorst near band edgeAdjacent channel rejection
BesselGentlest0 dB (flat)Maximally flatPulse / data fidelity
SAW/BAWVery steep<1 dBModerateMobile, small form factor
07 — Amplifiers & Mixers

Amplifiers & Mixers

Amplifier Gain Types
G_T = |S21|²·(1−|Γ_S|²)/(|1−S11Γ_S|²)·(1−|Γ_L|²)/|1−S22Γ_L|²
G_A = available gain (Γ_L=Γ_out*)
G_P = operating power gain
Maximum available gain: MAG = |S21/S12|·(K−√(K²−1)) when K>1
LNA Design Key Numbers
NF_min ≈ 1+2·(R_n/G_a)·(G_opt²+B_opt²)
Noise match ≠ power match
F = F_min + (R_n/G_s)·|Y_s−Y_opt|²
Match to Γ_opt not Γ_MS for minimum NF · typical LNA NF=0.5–2 dB
Mixer Fundamentals
Products: f_out = |m·f_RF ± n·f_LO|
Conversion loss ≈ 6–8 dB (passive)
SSB NF ≈ Conversion loss (if no 1/f)
Image: f_im = f_LO − f_IF (low-side LO)
Half-IF spur at f_RF ± f_IF/2 — design IF > signal BW × 5 to avoid
Power Amplifier Efficiency
PAE = (P_out − P_in)/P_dc × 100%
Class A: η_max=50% · Class B: 78.5%
Class D/E/F: >85% (switching)
PAPR penalty: back-off = PAPR (dB)
OFDM PAPR≈10dB → PA at 10% average efficiency → DPD restores 3–5 dB
08 — Unit Conversions

Unit Conversions

Power
dBm = 10·log(P[mW])
P[mW] = 10^(dBm/10)
P[W] = 10^((dBm−30)/10)
0 dBm = 1 mW = 224 mV into 50Ω
+10 dBm = 10 mW · +30 dBm = 1 W · +43 dBm = 20 W
Voltage (50 Ω)
V_rms = √(P·R) = √(P·50)
V_pk = V_rms·√2
dBm = 20·log(V_rms) + 13.01
0 dBm → 223.6 mV_rms → 316 mV_pk
dB Ratios
+3 dB = ×2 power = ×1.414 voltage
+6 dB = ×4 power = ×2 voltage
+10 dB = ×10 power = ×3.16 voltage
+20 dB = ×100 power = ×10 voltage
Nepers ↔ dB
1 Np = 8.686 dB
1 dB = 0.1151 Np
α[dB/m] = α[Np/m] × 8.686
Used in attenuation formulas
Noise Temperature ↔ NF
T_e = 290·(10^(NF/10)−1)
NF = 10·log(1+T_e/290)
T_e=0 → NF=0 dB · T_e=290→NF=3 dB
T_e=75 K → NF=1 dB (good LNA)
Frequency ↔ Wavelength
λ[mm] = 300/f[GHz] (free space)
λ_g[mm] = 300/(f[GHz]·√εeff)
1 GHz: λ=300 mm · 2.4 GHz: 125 mm
28 GHz: 10.7 mm · 77 GHz: 3.9 mm
dBmmWV_rms (50Ω)Common reference
−174 dBm/Hz4×10⁻²¹ mW0.45 fV/√HzThermal noise floor (290 K)
−100 dBm0.01 pW707 nVTypical LTE sensitivity
−60 dBm1 nW7.07 μVStrong indoor WiFi
0 dBm1 mW224 mVTest signal reference
+10 dBm10 mW707 mVWiFi TX power
+30 dBm1 W7.07 VFemtocell TX
+43 dBm20 W31.6 VLTE macro base station TX
09 — Constants & Key Numbers

RF Constants

k
1.381×10⁻²³ J/K
Boltzmann constant
T₀
290 K (16.85°C)
Standard noise temperature
kT₀
−174 dBm/Hz
Thermal noise floor @ T₀
c
3×10⁸ m/s
Speed of light (free space)
η₀
377 Ω
Free-space wave impedance
μ₀
4π×10⁻⁷ H/m
Permeability of free space
ε₀
8.854×10⁻¹² F/m
Permittivity of free space
σ_Cu
5.8×10⁷ S/m
Copper conductivity
δ_Cu@1GHz
2.09 μm
Cu skin depth at 1 GHz
Z₀
50 Ω
Standard RF impedance
Z₀_video
75 Ω
Broadcast/cable TV impedance
kT₀B
−101 dBm @ 20 MHz
WiFi noise floor at 290 K
Frequency BandRangeλ (free space)Key Applications
HF3–30 MHz10–100 mShortwave, amateur radio, OTHR radar
VHF30–300 MHz1–10 mFM radio, TV, ATC, TETRA
UHF300 MHz–3 GHz10 cm–1 mGSM, LTE, WiFi, GPS, Bluetooth
SHF / Microwave3–30 GHz1–10 cm5G NR, radar, satellite, microwave links
EHF / mmWave30–300 GHz1–10 mm5G FR2, 77 GHz radar, imaging, WiGig
Sub-THz300 GHz–3 THz0.1–1 mmSecurity imaging, spectroscopy
10 — Master Thumb Rules

Master Thumb Rules

These rules encode decades of RF engineering experience into instantly-usable heuristics. Each one is a mental shortcut that lets you estimate the right answer in seconds — before you even open a calculator. They are not approximations to memorise blindly: the explanation tells you exactly when each rule holds and when it breaks.

01
−174 dBm/Hz — the floor of the universe
Thermal noise at 290 K in 1 Hz. Every receiver sensitivity calculation starts here. Add NF, add 10·log(BW), add SNR_min. If your sensitivity is worse than −174+NF+10·log(BW)+SNR, you have a problem upstream.
02
Every 1 dB before the LNA costs 1 dB of system NF
A lossy cable, filter, or switch before the LNA adds its loss directly to system NF — because a passive attenuator L at T₀ has F=L. This is why LNAs go at the antenna and switches go after them.
03
×2 distance or frequency → +6 dB path loss
FSPL = 20·log(d) + 20·log(f) + constant. Doubling either adds 20·log(2) = 6.02 dB. Every engineer should be able to estimate path loss in their head for any link.
04
28 GHz is 18 dB worse than 3.5 GHz (same distance)
20·log(28/3.5) = 18 dB. This is exactly the gain a 64-element phased array provides. 5G mmWave works because beamforming gain cancels the frequency penalty — but only when the beam is pointing correctly.
05
P1dB ≈ IIP3 − 9.6 dB
Theoretical relationship from Taylor expansion of nonlinearity. In practice P1dB ≈ IIP3 − 8 to −12 dB. If you measure P1dB you can estimate IIP3 immediately — useful when you don't have a second tone source.
06
IM3 power grows at 3:1 slope — IIP3 grows at 2:1
Raise the input 1 dB: fundamental rises 1 dB, IM3 rises 3 dB. The difference ΔIM3 shrinks 2 dB per dB of drive. IIP3 is where the extrapolated lines cross — so IIP3 = P_in + ΔIM3/2.
07
N elements in a phased array → +10·log(N) dB gain
Coherent combining gives N× power gain over a single element. 64 elements = 18 dB. This is the mechanism that allows 5G mmWave to overcome 18 dB of excess path loss vs 3.5 GHz.
08
Skin depth ∝ 1/√f — Cu skin depth at 1 GHz = 2.1 μm
δ = 1/√(πfμ₀σ). At 10 GHz: 0.66 μm. At 100 GHz: 0.21 μm. A 35 μm copper trace is 33 skin depths thick at 1 GHz (full current use), but only 0.21 μm/0.66 μm at 10 GHz matters. Thinner plating means higher conductor loss at higher frequencies.
09
50 Ω on FR4 (h=1.6mm) → trace width ≈ 3.0 mm
The most common microstrip design point. εr=4.4 → εeff≈3.1 → Z₀=50Ω at W/h≈1.88 → W≈3.0mm. Thinner board or higher εr → narrower trace → more conductor loss. Rogers 4350B (εr=3.48) gives wider trace and lower loss at same impedance.
10
VSWR 2:1 → 0.5 dB mismatch loss and 11% reflected power
|Γ|=1/3 → mismatch loss = −10·log(1−1/9) = 0.51 dB. Often ignored but real. For a receive chain with VSWR 2:1 at the LNA input, 0.5 dB of the noise penalty is mismatch before the LNA even operates.
11
Q_L doubles → phase noise drops 6 dB (Leeson)
Leeson's equation: L(f) ∝ 1/Q_L². The single biggest lever in oscillator design. Switching from LC (Q=50) to DRO (Q=5000) improves phase noise 40 dB. Crystal oscillators (Q=10⁵–10⁶) achieve the lowest phase noise for this reason.
12
PLL in-band noise = ref noise + 20·log(N)
Dividing the VCO by N in the feedback loop multiplies the reference phase noise by N at the output. For N=500 (e.g. 5 GHz from 10 MHz reference) that's +54 dB — the main reason fractional-N PLLs exist (smaller effective N).
13
10× wider BW → 10 dB higher noise floor
Noise floor = −174 + 10·log(B). 5G NR at 100 MHz is 10 dB noisier than LTE at 10 MHz. The only way to compensate without better NF is beamforming gain or denser cell deployment — not better LNA, since NF is already near limits.
14
λ/4 line transforms impedance: Z_in = Z₀²/Z_L
Quarter-wave transformer. Open → short. Short → open. 200 Ω load + 100 Ω line → 50 Ω. The most used single-frequency matching technique in microwave design. Works exactly at one frequency and degrades with bandwidth.
15
60 GHz: O₂ absorption = 15 dB/km — 200 m maximum range
Oxygen absorption peak at 60 GHz limits links to ~100–200 m regardless of TX power. This is intentionally exploited for WiGig and secure short-range links. At 77 GHz (automotive radar) absorption drops to 0.4 dB/km — effectively transparent.
16
OFDM PAPR ≈ 10–12 dB — PA back-off costs efficiency
When N subcarriers align in phase, peak power = N × average. Statistical PAPR for LTE/5G NR is 10–12 dB. A 40 W PA running 10 dB back-off delivers 4 W average — 10% efficiency. DPD linearises the PA, allowing 3–5 dB less back-off.
17
Rayleigh fading: 99% coverage needs 20 dB fade margin
For Rayleigh fading (dense urban, no LOS), 1% outage probability requires 20 dB margin above the mean received power. With 2-antenna MRC diversity, the same coverage needs only 10 dB — diversity is far more power-efficient than brute-force margin.
18
Concrete wall: +12–15 dB penetration loss at 3.5 GHz
Building penetration loss is often the biggest single term in indoor coverage planning. One concrete wall = 12–15 dB at 3.5 GHz (worse at mmWave: 20–40 dB). Glass = 2–3 dB. Plasterboard = 3–5 dB. Critical for indoor 5G small cell placement.

RF Engineering Cheat Sheet — How to Use This Page

This cheat sheet is designed for working RF engineers, microwave designers, and students preparing for RF interviews or exams. Every formula is presented with its practical context — not just the equation, but which quantity to solve for, what the typical numerical result looks like in a real system, and when the formula breaks down.

Why Thumb Rules Matter

RF engineering is full of rules of thumb that encode decades of experience into single sentences. "Every 1 dB before the LNA costs 1 dB of system NF" is more useful in a design review than the Friis formula — because it immediately tells you the action to take. The 18 thumb rules in Section 10 are the most important ones in practice: they cover noise, path loss, transmission lines, antennas, oscillators, amplifiers, and propagation. Memorising even half of them will make you significantly faster at RF system design.

Network Parameter Conversions

The S→ABCD, S→Z and S→Y conversion formulas in Section 5 are essential for RF simulation work. S-parameters are the natural measurement domain (VNA), but ABCD parameters are needed for cascading, Z-parameters for circuit analysis, and Y-parameters for parallel admittance synthesis. The conversion formulas assume reference impedance Z₀=50 Ω throughout.