Presentation on theme: "Waveguides Rectangular Waveguides TEM, TE and TM waves"— Presentation transcript:
1Waveguides Rectangular Waveguides TEM, TE and TM waves Cutoff FrequencyWave PropagationWave Velocity,
2WaveguidesCircular waveguideRectangularwaveguideIn the previous chapters, a pair of conductors was used to guide electromagnetic wave propagation. This propagation was via the transverse electromagnetic (TEM) mode, meaning both the electric and magnetic field components were transverse, or perpendicular, to the direction of propagation.In this chapter we investigate wave-guiding structures that support propagation in non-TEM modes, namely in the transverse electric (TE) and transverse magnetic (TM) modes.In general, the term waveguide refers to constructs that only support non-TEM mode propagation. Such constructs share an important trait: they are unable to support wave propagation below a certain frequency, termed the cutoff frequency.Optical FiberDielectric Waveguide
3Rectangular Waveguide Let us consider a rectangular waveguide with interior dimensions are a x b,Waveguide can support TE and TM modes.In TE modes, the electric field is transverse to the direction of propagation.In TM modes, the magnetic field that is transverse and an electric field component is in the propagation direction.The order of the mode refers to the field configuration in the guide, and is given by m and n integer subscripts, TEmn and TMmn.The m subscript corresponds to the number of half-wave variations of the field in the x direction, andThe n subscript is the number of half-wave variations in the y direction.A particular mode is only supported above its cutoff frequency. The cutoff frequency is given byLocation of modes
4Rectangular Waveguide The cutoff frequency is given byRectangular WaveguideLocation of modesTable 7.1: Some Standard Rectangular WaveguideWaveguideDesignationa(in)btfc10(GHz)freq rangeWR9759.7504.875.125.605.75 – 1.12WR6506.5003.250.080.9081.12 – 1.70WR4304.3002.1501.3751.70 – 2.60WR2842.841.342.082.60 – 3.95WR1871.872.872.0643.163.95 – 5.85WR1371.372.6224.295.85 – 8.20WR90.900.450.0506.568.2 – 12.4WR62.311.0409.49
5To understand the concept of cutoff frequency, you can use the analogy of a road system with lanes having different speed limits.
6Rectangular Waveguide Let us take a look at the field pattern for two modes, TE10 and TE20In both cases, E only varies in the x direction; since n = 0, it is constant in the y direction.For TE10, the electric field has a half sine wave pattern, while for TE20 a full sine wave pattern is observed.
7Rectangular Waveguide ExampleLet us calculate the cutoff frequency for the first four modes of WR284 waveguide. From Table 7.1 the guide dimensions are a = mils and b = mils. Converting to metric units we have a = cm and b = cm.TM11TE10:TE10TE20TE01TE11TE01:TE20:TE11:
9Rectangular Waveguide - Wave Propagation We can achieve a qualitative understanding of wave propagation in waveguide by considering the wave to be a superposition of a pair of TEM waves.Let us consider a TEM wave propagating in the z direction. Figure shows the wave fronts; bold lines indicating constant phase at the maximum value of the field (+Eo), and lighter lines indicating constant phase at the minimum value (-Eo).The waves propagate at a velocity uu, where the u subscript indicates media unbounded by guide walls. In air, uu = c.
10Rectangular Waveguide - Wave Propagation Now consider a pair of identical TEM waves, labeled as u+ and u- in Figure (a). The u+ wave is propagating at an angle + to the z axis, while the u- wave propagates at an angle –.These waves are combined in Figure (b). Notice that horizontal lines can be drawn on the superposed waves that correspond to zero field. Along these lines the u+ wave is always 180 out of phase with the u- wave.
11Rectangular Waveguide - Wave Propagation Since we know E = 0 on a perfect conductor, we can replace the horizontal lines of zero field with perfect conducting walls. Now, u+ and u- are reflected off the walls as they propagate along the guide.The distance separating adjacent zero-field lines in Figure (b), or separating the conducting walls in Figure (a), is given as the dimension a in Figure (b).The distance a is determined by the angle and by the distance between wavefront peaks, or the wavelength . For a given wave velocity uu, the frequency is f = uu/.If we fix the wall separation at a, and change the frequency, we must then also change the angle if we are to maintain a propagating wave. Figure (b) shows wave fronts for the u+ wave.The edge of a +Eo wave front (point A) will line up with the edge of a –Eo front (point B), and the two fronts must be /2 apart for the m = 1 mode.(a)a(b)
12Rectangular Waveguide - Wave Propagation For any value of m, we can write by simple trigonometryThe waveguide can support propagation as long as the wavelength is smaller than a critical value, c, that occurs at = 90, orWhere fc is the cutoff frequency for the propagating mode.We can relate the angle to the operating frequency and the cutoff frequency by
13Rectangular Waveguide - Wave Propagation The time tAC it takes for the wavefront to move from A to C (a distance lAC) isA constant phase point moves along the wall from A to D. Calling this phase velocity up, and given the distance lAD isThen the time tAD to travel from A to D isSince the times tAD and tAC must be equal, we have
14Rectangular Waveguide - Wave Propagation The Wave velocity is given byPhase velocityWave velocityGroup velocityThe Phase velocity is given byAnalogy!usingBeachPoint of contactPhase velocityWave velocityThe Group velocity is given byGroup velocityOcean
15Rectangular Waveguide - Wave Propagation The phase constant is given byThe guide wavelength is given byThe ratio of the transverse electric field to the transverse magnetic field for a propagating mode at a particular frequency is the waveguide impedance.For a TE mode, the wave impedance isFor a TM mode, the wave impedance is
17Rectangular Waveguide ExampleLet’s determine the TE mode impedance looking into a 20 cm long section of shorted WR90 waveguide operating at 10 GHz.From the Waveguide Table 7.1, a = 0.9 inch (or) cm and b = inch (or) cm.ModeCutoff FrequencyModeCutoff FrequencyTE106.56 GHzTE106.56 GHzTE0113.12 GHzRearrangeTE0113.12 GHzTE2013.13 GHzTE1114.67 GHzTE1114.67 GHzTE2013.13 GHzTE0226.25 GHzTE0226.25 GHzTM11TE10TE01TE20TE11TE026.56 GHz13.12 GHz14.67 GHz26.25 GHz13.13 GHzAt 10 GHz, only the TE10 mode is supported!
18Rectangular Waveguide ExampleThe impedance looking into a short circuit is given byThe TE10 mode impedanceThe TE10 mode propagation constant is given by