EduKG
← Back

radio communication television and radar principles

Learning objectives

  • Outcome

    Label a block diagram of a radio link with the roles of the carrier oscillator, modulator, transmitting and receiving antennas, and demodulator, and describe message transfer at each stage in one sentence.

  • Outcome

    Compute the wavelength from λ=c/f0\lambda = c/f_0 and choose an antenna length within a factor of 2 of λ/2\lambda/2 for a given frequency.

  • Outcome

    Determine target range from the echo delay d=cΔt/2d = c\Delta t/2 and find the maximum unambiguous range of a radar from the pulse repetition period.

  • Outcome

    Convert a measured Doppler shift into the radial speed of a target using Δf=2vf0/c\Delta f = 2vf_0/c and state from the sign of the shift whether the target approaches or recedes.

Understand the idea

Principles of Radio Communication, Television, and Radar

Text

Radio communication rests on the emission and reception of electromagnetic waves. A harmonic carrier s0(t)=A0cos⁡(2πf0t)s_0(t)=A_0\cos(2\pi f_0 t) is radiated by an antenna, and the message is imposed on it by amplitude, frequency, or phase modulation: s(t)=A(t)cos⁡(2πf0t+φ(t))s(t)=A(t)\cos(2\pi f_0 t+\varphi(t)). An antenna radiates efficiently when its size is comparable with the wavelength λ=c/f0\lambda=c/f_0, which is why long-wave stations need tall masts while mobile links use centimetre waves. Television transmits picture and sound in one channel: the video signal amplitude-modulates the carrier (in practice with a partly suppressed sideband to save spectrum), while line and frame sync pulses let the receiver rebuild the raster. Radar sends a short pulse, receives the echo, and converts the delay Δt\Delta t into range by d=cΔt/2d=c\Delta t/2, the factor 2 accounting for the round trip. A moving target shifts the echo frequency by the Doppler amount Δf=2vf0/c\Delta f=2vf_0/c, which yields its radial speed.

Worked examples

Direct

Problem

A radio station transmits at f0=100f_0 = 100 MHz. Find the wavelength λ\lambda and estimate the length of a half-wave dipole receiving antenna.

Solution

Radio waves travel at c=3.0⋅108c = 3{.}0\cdot10^{8} m/s, so

λ=cf0=3.0⋅1081.00⋅108=3.0 m.\lambda = \frac{c}{f_0} = \frac{3{.}0\cdot10^{8}}{1{.}00\cdot10^{8}} = 3{.}0\ \text{m}.

A half-wave dipole has length

l=λ2=1.5 m.l = \frac{\lambda}{2} = 1{.}5\ \text{m}.

This corresponds to the VHF (FM) band, where such stations operate.

Application

Problem

A pulsed radar sends a probing pulse, and the echo from a target returns after Δt=40\Delta t = 40 $\mu$s. The pulse repetition period is T=1.0T = 1{.}0 ms. Find the target range dd and the maximum unambiguous range dmaxd_{max} of the radar.

Solution

The echo travels to the target and back, so 2d=cΔt2d = c\Delta t and

d=cΔt2=3.0⋅108⋅40⋅10−62=6.0⋅103 m=6.0 km.d = \frac{c\Delta t}{2} = \frac{3{.}0\cdot10^{8}\cdot 40\cdot10^{-6}}{2} = 6{.}0\cdot10^{3}\ \text{m} = 6{.}0\ \text{km}.

For the echo to return before the next pulse we need T≥2d/cT \ge 2d/c, hence

dmax=cT2=3.0⋅108⋅1.0⋅10−32=1.5⋅105 m=150 km.d_{max} = \frac{cT}{2} = \frac{3{.}0\cdot10^{8}\cdot1{.}0\cdot10^{-3}}{2} = 1{.}5\cdot10^{5}\ \text{m} = 150\ \text{km}.

A target at 6 km lies inside that interval, so its range is measured unambiguously.

Transfer

Problem

A speed-control radar operates at f0=10f_0 = 10 GHz. Mixing the transmitted and reflected signals gives a difference (Doppler) frequency Δf=1.0\Delta f = 1{.}0 kHz. Find the radial speed of the car in m/s and km/h, and explain how the sign of the shift shows whether it is approaching or receding.

Solution

For a radar that transmits and receives at the same frequency the Doppler shift is Δf=2vf0/c\Delta f = 2vf_0/c, hence

v=Δf c2f0=1.0⋅103⋅3.0⋅1082⋅1.0⋅1010=15 m/s≈54 km/h.v = \frac{\Delta f\, c}{2f_0} = \frac{1{.}0\cdot10^{3}\cdot3{.}0\cdot10^{8}}{2\cdot1{.}0\cdot10^{10}} = 15\ \text{m/s} \approx 54\ \text{km/h}.

Sign of the shift: if the echo arrives with a higher frequency (Δf>0\Delta f > 0), the distance is shrinking — the car is approaching; if with a lower one (Δf<0\Delta f < 0), it is receding. Note also that the radar measures only the radial component of velocity: if the car moves at an angle to the beam, vv will be smaller than the true speed.

Practice

Text

An at-home modelling lab (entirely safe, no transmission required).

  1. In a spreadsheet, tabulate λ=c/f0\lambda = c/f_0 for carriers at 88, 100, 108 MHz (FM), 600 MHz (television) and 3 GHz (radar). For each row compute λ/2\lambda/2 and note which antenna size is realistic.
  2. Model a pulsed radar: repetition period T=1T = 1 ms, target at 15 km. Compute the echo delay Δt=2d/c\Delta t = 2d/c (it should be 100 $\mu$s) and sketch a 'transmitted pulse — echo' timing diagram.
  3. Place the target at 200 km with the same TT and show that the echo arrives only after the next pulse: range ambiguity appears, and the instrument may report a false close target.
  4. In a free simulator (e.g. Falstad 'Amplitude Modulation' or a similar online oscilloscope) observe the carrier and envelope for AM while changing the modulation depth; compare with FM, where the amplitude stays constant.

Safety. Do not use real transmitters in service or amateur bands without a licence; all measurements and observations are done in a simulator or offline.

Visual reference

Purpose

Show that radio communication, television and radar share one and the same chain 'carrier → modulation → antenna → propagation → reception → demodulation', and link the echo time delay to the target range.

Representation

Block diagram of a radio link: carrier oscillator → modulator (message input) → transmitting antenna → propagation medium → receiving antenna → demodulator. Beside it, two graphs: above, an oscillogram of an AM signal with envelope A(t)A(t) on the carrier cos⁡(2πf0t)\cos(2\pi f_0 t); below, a timing diagram of transmitter pulses (period TT) and the received echo delayed by Δt\Delta t, together with the formula d=cΔt/2d = c\Delta t/2.

Real-world examples

Mobile phone call

Scenario

You call a friend on a mobile phone. The phone emits radio waves at a frequency of 1,8 GHz1{,}8\ \text{GHz} (1,8×109 Hz1{,}8\times 10^9\ \text{Hz}). The transmitter power is about 0,2 W0{,}2\ \text{W}, and the nearest base station is 500 m500\ \text{m} away. The wavelength is: λ=cf=3,0×108 m/s1,8×109 Hz≈0,17 m.\lambda = \frac{c}{f} = \frac{3{,}0\times 10^8\ \text{m/s}}{1{,}8\times 10^9\ \text{Hz}} \approx 0{,}17\ \text{m}. The signal reaches the station in about t=d/c=500/3,0×108≈1,7×10−6 s=1,7 μst = d/c = 500/3{,}0\times 10^8 \approx 1{,}7\times 10^{-6}\ \text{s} = 1{,}7\ \mu\text{s}.

Connection

The scenario uses emission of electromagnetic waves by the phone antenna and modulation: sound is converted into an electrical signal that is superimposed on the 1,8 GHz1{,}8\ \text{GHz} carrier. The receiving antenna extracts this signal. The frequency choice relies on the spectrum: in the microwave band, compact antennas work and many channels are available.

Radar speed gun

Scenario

An officer points a radar at a car. The radar emits pulses at a frequency f0=24,15 GHzf_0 = 24{,}15\ \text{GHz}. The car moves at speed v=30 m/sv = 30\ \text{m/s} (108 km/h108\ \text{km/h}). The reflected signal returns with a Doppler frequency shift: Δf=2vf0c=2⋅30⋅24,15×1093,0×108≈4,8×103 Hz=4,8 kHz.\Delta f = \frac{2 v f_0}{c} = \frac{2 \cdot 30 \cdot 24{,}15\times 10^9}{3{,}0\times 10^8} \approx 4{,}8\times 10^3\ \text{Hz} = 4{,}8\ \text{kHz}. For a distance d=150 md = 150\ \text{m}, the echo delay is: t=2dc=2⋅1503,0×108=1,0×10−6 s=1,0 μs.t = \frac{2d}{c} = \frac{2\cdot150}{3{,}0\times10^8} = 1{,}0\times10^{-6}\ \text{s} = 1{,}0\ \mu\text{s}.

Connection

The radar principles work here: directed emission of radio waves, reflection from the car, and reception of the echo. The Doppler shift Δf=2vf0/c\Delta f = 2 v f_0/c gives speed, while the delay t=2d/ct = 2d/c gives distance. The frequency 24,15 GHz24{,}15\ \text{GHz} is chosen from the spectrum: the wavelength λ=c/f0≈0,012 m\lambda = c/f_0 \approx 0{,}012\ \text{m} allows a narrow beam.

Television tower and reception

Scenario

A city receives a television signal from a tower of height h=300 mh = 300\ \text{m} operating at a frequency f=600 MHzf = 600\ \text{MHz} (6,0×108 Hz6{,}0\times10^8\ \text{Hz}). The wavelength is: λ=cf=3,0×1086,0×108=0,50 m.\lambda = \frac{c}{f} = \frac{3{,}0\times10^8}{6{,}0\times10^8} = 0{,}50\ \text{m}. The line-of-sight distance to the horizon from the tower height is: d≈2Rh=2⋅6,37×106⋅300≈6,2×104 m=62 km.d \approx \sqrt{2 R h} = \sqrt{2\cdot 6{,}37\times10^6\cdot 300} \approx 6{,}2\times10^4\ \text{m} = 62\ \text{km}. Therefore reliable reception is possible within a radius of several tens of kilometers.

Connection

The example shows television transmission: the video signal modulates the 600 MHz600\ \text{MHz} carrier (UHF band), and the receiving antenna extracts it. Propagation is almost line-of-sight, so the tower height determines the coverage area; this follows from the properties of electromagnetic waves in the UHF part of the spectrum.