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Transcript

1 Lecture 7: Helmholtz Wave Equations and Plane Waves Instructor: Dr. Gleb V. Tcheslavski Contact: [email protected] Office Hours: Room 2030 Class web site: www.ee.lamar.edu/g leb/em/Index.htm “The ninth wave” by Ivan Aivazovsky (1817-1900) ELEN 3371 Electromagnetics Fall 2008 2 Wave Equation The propagation of EM energy can be described by a wave equation. We assume that the media is homogeneous and may have losses. We also assume there are no free charges in the region of interest; therefore, fields are studied outside the “source region”: v = 0. (7.2.1) Finally, we assume no external currents. Recall that the constitutive relations are: ELEN 3371 Electromagnetics D E B H J E Fall 2008 (7.2.2) (7.2.3) (7.2.4) 3 Wave Equation For the stated assumptions, the Maxwell’s equations can be rewritten as H E t E H E t (7.3.2) E 0 (7.3.3) H 0 (7.3.4) Equations (7.3.1) and (7.3.2) contain both electric and magnetic field terms; therefore, they are coupled equations. When we change either electric or magnetic field, we automatically affect the other field also. ELEN 3371 Electromagnetics (7.3.1) Fall 2008 4 Wave Equation Furthermore, the equations (7.3.1) and (7.3.2) are two first-order PDEs in the two dependent variables E and H. We can combine them into a single secondorder PDE in terms of one of the variables. For the E field, we take curl of (7.3.1) and substitute (7.3.2) into RHS of the result… E E 2 E E H E 2 t t t t t (7.4.1) Using the vector identity: E E 2 E 2 E (7.4.2) We obtain the wave equation: 2 E E 2 E 2 0 t t ELEN 3371 Electromagnetics Fall 2008 (7.4.3) 5 Wave Equation The equation in (7.4.3) is a general homogeneous 3D vector wave equation. It is valid for cases where there are no external sources. We also note that the equation itself does not depend on the coordinate system. Solution of (7.4.3) in general case may be quite complicated… Therefore, we assume that the wave is propagating in free space with no currents and only y component of the electric field exists: i.e. the wave is linearly polarized in the y-direction. Therefore, in the CCS: 2 Ey z Note: ELEN 3371 Electromagnetics 2 0 0 c 1 2 Ey t 2 0 0 Fall 2008 0 (7.5.1) (7.5.2) 6 Wave Equation Example 7.1: Show that the wave equation for the magnetic field intensity H can be derived in a similar way as one for the electric field. By taking curl of the Ampere’s law (7.3.2) and substituting the Faraday’s law (7.3.1) to the result, we arrive at H E H E t t H t t (7.6.1) Using the vector identity: H H 2 H 2 H (7.6.2) We obtain the new wave equation: 2 H H 2 H 2 0 t t (7.6.3) Note: this wave equation has exactly the same form as one for the electric field. ELEN 3371 Electromagnetics Fall 2008 7 Wave Equation Example 7.2: Compute an approximate numerical value for the velocity of light c. Using the numerical values for the electric and magnetic constants in free space, we write: c 1 0 0 1 1 4 10 109 36 3 108 m / s 7 Note: the more accurate value for the dielectric constant will slightly reduce this estimate. ELEN 3371 Electromagnetics Fall 2008 8 One-dimensional Wave equation 1. Wave experiments in other disciplines (mechanics) A plunger (wave-maker) in a water tank can move up and down. The repetition frequency of the plunger’s motion is slow enough to excite waves not interfering with each other. The water (mechanical) waves propagate slowly compared to EM. ELEN 3371 Electromagnetics Fall 2008 9 One-dimensional Wave equation These waves are transversal We can evaluate the velocity of wave propagation (the speed at which wave crest is traveling) and the trajectory of wave propagation. is perpendicular to the direction of propagation. The velocity of propagation depends on the surface tension and mass density of water. ELEN 3371 Electromagnetics Fall 2008 10 One-dimensional Wave equation A string is stretched between two points. A small perturbation is launched at one end of it and it propagates to the other end. We neglect any reflections. The velocity of propagation depends on the tension on the string and its mass density. These waves are transversal: is perpendicular to the direction of propagation ELEN 3371 Electromagnetics Fall 2008 11 One-dimensional Wave equation A spring is stretched between two walls. If one of the walls is suddenly moved, a perturbation in the spring compression propagates to the other end of the spring. We can find the trajectory of the propagation and the velocity of propagation. The velocity of propagation depends on the elasticity and the mass density of the spring. The wave in this experiment is longitudinal : is in the direction of propagation (parallel to it). Longitudinal EM waves do not exist! ELEN 3371 Electromagnetics Fall 2008 12 One-dimensional Wave equation 2. Analytical solution of a 1D equation – traveling waves. Recall that in 1D the wave equation is: 2 Ey z or 2 0 0 2 Ey z 2 2 Ey t 2 0 2 1 Ey 2 0 2 c t (7.12.1) (7.12.2) The most general solution for this equation is: E y ( z, t ) F ( z ct ) G ( z ct ) (7.12.3) Here F and G are arbitrary functions determined by the generator exciting the wave. ELEN 3371 Electromagnetics Fall 2008 13 One-dimensional Wave equation E y ( z, t ) F ( z ct ) G ( z ct ) The solution F(z – ct) is a wave traveling in the +z direction. The solution G(z + ct) is a wave traveling in the -z direction. Two possible ways to create both waves simultaneously: 1) Two generators (sources) at z = - and at z = +; 2) A source at z = - and a reflecting boundary, say, at z = 0: an incident and a reflected waves! Let us verify the validity of the general solution… ELEN 3371 Electromagnetics Fall 2008 14 One-dimensional Wave equation First, we introduce two new variables: z ct z ct (7.14.1) (7.14.2) And use the chain rule of differentiation: E y dG t d t E y dF dG z d z d z ELEN 3371 Electromagnetics dF d t Fall 2008 dG dF c c d d dG dF 1 1 d d (7.14.3) (7.14.4) 15 One-dimensional Wave equation The second derivatives are: 2 1 Ey 1 d 2F d 2G d 2 F d 2G 2 2 2 2 2 c c 2 2 2 c t c d d d d 2 2 E y d 2 F 2 d 2G 2 d 2 F d 2G 1 1 2 2 2 2 z d d d d 2 Therefore: 2 Ey z 2 2 1 Ey 2 c t 2 Which proves that (7.12.3) is a general form of a solution for (7.12.2). ELEN 3371 Electromagnetics Fall 2008 (7.15.1) (7.15.2) (7.15.3) 16 One-dimensional Wave equation Let us find a particular solution for the following assumptions: 1. The solution is a known function P(z) at the time t = 0; 2. The derivative of the solution is a known function Q(z) at the time t = 0. E y ( z, 0) P( z ) E y ( z, 0) Q( z ) t (7.16.1) A particular solution of (7.12.2) that satisfies (7.16.1) is z ct 1 1 E y ( z , t ) P( z ct ) P ( z ct ) Q ( z ')dz ' 2 2c z ct 1 1 P( z ct ) P( z ct ) R( z ct ) R( z ct ) 2 2 z Were 1 R ( z ) Q( z ')dz ' is an auxiliary function. c0 ELEN 3371 Electromagnetics Fall 2008 (7.16.2) 17 One-dimensional Wave equation F ( z ct ) F0e ( z ct ) 2 Example 7.3: Show that the function is a solution of the wave equation. That’s a Gaussian-pulse traveling wave. Let z’ = z – ct; therefore F ( z ct ) F0e z '2 and G(z + ct) = 0. The chain rule: F dF z ' z '2 F0 2 z ' e (1) z dz ' z F dF z ' z '2 F0 2 z ' e ( c) t dz ' t and ELEN 3371 Electromagnetics 2 F 2 z '2 2 F 2 4 z ' e (1) 0 z 2 1 2 F 1 2 z '2 2 2 2 F0 2 4 z ' e ( c ) 2 c t c Fall 2008 (7.17.1) (7.17.2) (7.17.3) (7.17.4) 18 One-dimensional Wave equation Combining the second derivatives, we arrive at: 1 2 z '2 2 2 z '2 F0 2 4 z ' e (1) 2 F0 2 4 z ' e ( c) 2 0 c A sequence of pulses taken at successive times illustrates the propagation of the pulses. The velocity of propagation is c. ELEN 3371 Electromagnetics Fall 2008 (7.18.1) 19 One-dimensional Wave equation We can also define the propagation of Gaussian pulse as an initial value problem: P( z ) F ( z ') t 0 F0e z2 (7.19.1) F dF z ' z '2 2 F0 c z ' e t dz ' t (7.19.2) F z2 Q( z ) ( z ') t 0 2 F0cze t (7.19.3) The auxiliary function will be: z z 1 1 z '2 z2 R( z ) Q( z ')dz ' 2cF0 z ' e dz ' F0 1 e F0 F ( z ) c0 c 0 ELEN 3371 Electromagnetics Fall 2008 (7.19.4) 20 One-dimensional Wave equation Therefore, the particular solution will be: 1 1 1 1 E y ( z, t ) F ( z ct ) F ( z ct ) F0 F ( z ct ) F0 F ( z ct ) 2 2 2 2 F ( z ct ) Which is a Gaussian wave traveling in the +z direction. ELEN 3371 Electromagnetics Fall 2008 (7.20.1) 21 Matlab solution of a 1D wave eqn. The main weakness of numerical solutions is that they do not really give any inside to the underlying physics of the problem as theoretical solutions do. However, Matlab allows to plot the numerical solutions, which, to some extend, overcomes this limitation… Recall that a 1D WE: 2 Ey z 2 2 1 Ey 2 0 2 c t (7.21.1) To develop a numerical solution to (7.21.1), we first need to solve a first-order PDE sometimes called the advection equation: 1 0 z c t (7.21.2) (7.21.2) describes the transport of a conserved scalar quantity in a vector field: for instance, a pollutant spreading through a flowing stream. It’s hard to solve numerically in the general case. ELEN 3371 Electromagnetics Fall 2008 22 Matlab solution of a 1D wave eqn. For the initial condition ( z, t 0) F ( z ) (7.22.1) The analytical solution of the advection equation is given by ( z, t ) F ( z ct ) (7.22.2) Which is also a solution of the wave equation… Remark: the wave equation and the advection equation are hyperbolic equations, the diffusion equations are parabolic equations, and Laplace’s and Poisson’s equations are elliptic equations. ELEN 3371 Electromagnetics Fall 2008 23 Matlab solution of a 1D wave eqn. We assume that the space z and time t can be represented in a 3D figure. The amplitude of the wave is specified by the third coordinate. Next, we set up a numerical grid: we divide the region L, in which the wave propagates, into N sections (N = 4 in the figure). Therefore, the step in space: h L N (7.23.1) Assuming that the velocity of the propagation is c and it takes time for the wave to cover h: ELEN 3371 Electromagnetics h c Fall 2008 (7.23.2) 24 Matlab solution of a 1D wave eqn. We assume the solution to be stable and use the periodic boundary conditions: once a numerically calculated wave reaches the boundary at z = +L/2, it reappears at the same time at the boundary z = -L/2 and continues to propagate in the region –L/2 z +L/2. However, instead of evaluating the wave at the edges, it is estimated at ½ of a spatial increment from them. Using the forward difference method: ( zi , tn ) ( zi , tn ) t where ELEN 3371 Electromagnetics L 1 zi i h 2 2 tn (n 1) Fall 2008 (7.24.1) (7.24.2) (7.24.3) 25 Matlab solution of a 1D wave eqn. Using the central difference method: ( zi h, tn ) ( zi h, tn ) z 2h (7.25.1) Therefore, the advection equation will be: ( zi h, tn ) ( zi h, tn ) 1 ( zi , tn ) ( zi , tn ) 0 2h c (7.25.2) In (7.25.2), all terms except for one are given for the present time, and one term specifies the future value of the wave: c ( zi ,tn ) ( zi ,tn ) ( zi h,tn ) ( zi h,tn ) 2h That’s a Finite Difference Time Domain (FDTD) method. ELEN 3371 Electromagnetics Fall 2008 (7.25.3) 26 Matlab solution of a 1D wave eqn. The expression in (7.25.3) is valid in the interior range: 2 n N-1. At the edges employing the periodic boundary conditions: c ( z2 tn ) ( z N ,tn ) 2h c ( z N ,tn ) ( z N ,tn ) ( z1 tn ) ( z N 1 ,tn ) 2h ( z1 ,tn ) ( z1 ,tn ) (7.26.1) (7.26.2) For unstable problems, the Lax method is used: ( zi ,tn ) 1 c ( zi h,tn ) ( zi h,tn ) ( zi h,tn ) ( zi h,tn ) 2 2h 1 c ( z1 ,tn ) ( z2 ,tn ) ( z N ,tn ) ( z2 tn ) ( z N ,tn ) 2 2h 1 c ( z N ,tn ) ( z1 ,tn ) ( z N 1 ,tn ) ( z1tn ) ( z N 1 ,tn ) 2 2h ELEN 3371 Electromagnetics Fall 2008 (7.26.3) (7.26.4) (7.26.5) 27 Time-harmonic plane waves 1. Plane waves in vacuum. Assuming that a time-harmonic propagating wave is polarized in the y-direction. E( z, t ) Ey ( z, t ) Ey ( z)e jt (7.27.1) a phasor In a vacuum, the phase velocity of the wave equals to the velocity of light c. Therefore, the 1D wave equation is: 2 Ey ( z) z 2 2 2 2 jt E ( z ) d E ( z ) j 1 y y 2 0 2 Ey ( z) e 0 2 2 c t c dz ELEN 3371 Electromagnetics Fall 2008 (7.27.2) 28 Time-harmonic plane waves or d 2 E y ( z ) 2 Ey ( z) 0 2 dz c (7.28.1) We introduce a new quantity called a wave number: k c 2 f 2 c (7.28.2) Therefore, the 1D wave equation (the Helmholtz equation) is: ELEN 3371 Electromagnetics d 2 Ey ( z) dz 2 k 2 Ey ( z) 0 Fall 2008 (7.28.3) 29 Time-harmonic plane waves A solution of the second-order ODE (7.28.3) is in a form: Ey ( z) ae jkz be jkz (7.29.1) where a and b are the integration constants. Incorporating (7.27.1), we obtain: Ey ae j (t kz ) be j (t kz ) (7.29.2) The real part of the solution will be: E y acos(t kz ) bcos(t kz ) Note: instead of the real, we could use the imaginary part – sin function. The first term in (7.29.3) is a wave moving in a +z direction; the second term is a wave moving in the –z direction (incident and reflected waves). ELEN 3371 Electromagnetics Fall 2008 (7.29.3) 30 Time-harmonic plane waves Since the waves are propagating in vacuum, the phase velocities for these traveling waves are: v k c (7.30.1) In general, the phase velocity is a vector since it has both a magnitude and a direction. It can have a value greater than the light speed! However, there is no energy (or particles) transferred at that speed. The wave number may also be a vector and, therefore, indicate the direction, in which the wave is traveling. In this case, it is frequently called a wave vector and the quantity kz can be replaced by k r kr kˆ rˆ ELEN 3371 Electromagnetics Fall 2008 (7.30.2) 31 Time-harmonic plane waves Example 7.4: A polarized in the y direction electric field that propagates in vacuum was simultaneously measured at z = 0 and one wavelength away at z = 2 cm. The amplitude is 2 V/m. Find the frequency of excitation, and write an expression that describes the wave if it’s moving in the +z direction. The wavelength is = 0.02 m, therefore: 2 f 2 c 3 108 k f 1.5 1010 Hz15GHz c 0.02 The wave number: The wave is: ELEN 3371 Electromagnetics 2 2 k 100 0.02 E ( z, t ) 2 106 cos 2 15 109 t 50 z u y Fall 2008 (7.31.1) (7.31.2) (7.31.3) 32 Time-harmonic plane waves Example 7.5: Show that a linearly polarized plane wave can be resolved into two equal amplitude circularly polarized waves: i.e. waves that rotate about the z axis. The linearly polarized wave E y ( z, t ) E0u y e j t kz can be written as a sum of two components: where E y ( z, t ) Since We obtain: Ey ( z, t ) Ey ( z, t ) Ey ( z, t ) E0 E0 j t kz j t kz u ju e ; E ( z , t ) u ju e y x y y x 2 2 u x u sin ;u y u cos u y jux u e j ;u y jux u e j (7.32.1) (7.32.2) (7.32.3) (7.32.4) (7.32.5) Which demonstrates that the first and second waves rotate in opposite directions. ELEN 3371 Electromagnetics Fall 2008 33 Time-harmonic plane waves 2. Magnetic field intensity and characteristic impedance. The magnetic field intensity can be found via the Faraday’s law: E ( z, t ) j B( z, t ) j0 H ( z, t ) u x 1 H ( z, t ) j0 x 0 Since: Therefore: ELEN 3371 Electromagnetics H ( z, t ) 1 E0 e j (t kz ) j0 z Fall 2008 uy y E0 e j t kz uz z 0 k j (t kz ) (u x ) ux E0e 0 (7.33.1) (7.33.2) (7.33.3) 34 Time-harmonic plane waves We introduce a new quantity called a characteristic impedance of the medium: Zc For a free space: Therefore: k Z0 H x ( z, t ) The Poynting vector: kc c k 0 E ( z, t ) 120 376.73 H ( z, t ) 0 1 1 E0e j (t kz )u x u z E y ( z , t ) A m] Zc Zc S E ( z, t ) H ( z, t ) Suz If we know the value of one of the field components and the characteristic impedance, we can find the value of the other field component. ELEN 3371 Electromagnetics Fall 2008 (7.34.1) (7.34.2) (7.34.3) (7.34.4) 35 Time-harmonic plane waves Example 7.6: Find the magnetic field intensity for the following electric field in vacuum: E ( z, t ) 2 106 cos 2 15 109 t 50 z u y E ( z, t ) 2 106 ( z, t ) cos 2 15 109 t 50 z u z u y Z0 120 ( z, t ) 5.3 109 cos 2 15 109 t 50 z ux A m This direction of the magnetic field intensity is required so the power will flow in the +z direction: S EH uz ELEN 3371 Electromagnetics uy ? Fall 2008 36 Time-harmonic plane waves Example 7.7: Find the average power in a circular area in a plane defined by z = constant, whose radius is 3 m if the electric field in a vacuum is: E( z, t ) 10cos t kz ux In a complex form: E( z, t ) 10e jt kz ux Since the field is in a vacuum, Z0 = 120 . 10 j t kz H ( z, t ) e uy 120 The average power: 1 1 10 * Pav Re E ( z, t ) H ( z, t ) ds 10 32 3.75W 2 s 120 2 ELEN 3371 Electromagnetics Fall 2008 37 Plane wave propagation in a dielectric medium 1. Plane wave in a lossless homogeneous dielectric. The wave number for the wave propagating in a vacuum is a function of permittivity and permeability of free space: k0 2 f 0 0 (7.37.1) Naturally, for a dielectric medium that may have different constants, the wave number will be k 2 f 0 r 0 r ELEN 3371 Electromagnetics Fall 2008 (7.37.2) 38 Plane wave propagation in a dielectric medium If a plane wave generated by a signal generator propagates through two different dielectrics… Say, with the same magnetic constants but different permittivities, the wave numbers will be for these two media: k1 2 f 10 k2 2 f 2 0 (7.38.1) Both signals travel the same distance z but will have different phase velocities: v1 k1 ;v2 k2 ELEN 3371 Electromagnetics Fall 2008 (7.38.2) 39 Plane wave propagation in a dielectric medium This difference in velocities delays the arrival of one signal with respect to the other and causes a phase difference that can be detected: k1z k2 z 2 f 10 2 0 z (7.39.1) If the total phase change in the signal passing through one of the paths is known: 1 2 f 10 z The relative phase difference is 2 f 10 2 0 z 1 2 1 1 2 f 10 z Therefore, if the properties of one of the regions are known and the phase difference is measured, we can identify the other material. ELEN 3371 Electromagnetics Fall 2008 (7.39.2) (7.39.3) 40 Plane wave propagation in a dielectric medium The ratio of the phase velocity in a vacuum to the phase velocity in a dielectric is called the index of refraction for the material: n Optical materials are usually characterized by their index of refraction. ELEN 3371 Electromagnetics c v p ,diel r Material Vacuum Air at STP Ice Water at 20 C Acetone Ethyl alcohol Sugar solution(30%) Fluorite Fused quartz Glycerine Sugar solution (80%) Typical crown glass Crown glasses Fall 2008 (7.40.1) Index 1.00000 1.00029 1.31 1.33 1.36 1.36 1.38 1.433 1.46 1.473 1.49 1.52 1.52-1.62 Material Spectacle crown, C-1 Sodium chloride Polystyrene Carbon disulfide Flint glasses Heavy flint glass Extra dense flint, EDF-3 Methylene iodide Sapphire Rare earth flint Lanthanum flint Arsenic trisulfide glass Diamond Index 1.523 1.54 1.55-1.59 1.63 1.57-1.75 1.65 1.7200 1.74 1.77 1.7-1.84 1.82-1.98 2.04 2.417 41 Plane wave propagation in a dielectric medium Example 7.7: Find the phase difference if one region is filled with a gas with r = 1.0005 and the other region is a vacuum. The frequency of oscillation is 10 GHz and the length is z = 1m. The phase difference is 2 f 0 0 0 r 0 z 2 f 0 0 1 r z 2 1010 0 1 1.0005 1 0.052 radians 3 3 108 This difference is small but can be detected. Also, if the travel distance is increased, the resolution (i.e. detectable phase difference) will be higher. ELEN 3371 Electromagnetics Fall 2008 42 Plane wave propagation in a dielectric medium 2. Plane wave in a lossy homogeneous dielectric. A dielectric material can be lossy, i.e. exhibit a nonzero conductivity . In this situation, a conduction current must be added to the displacement current when considering the Ampere’s law. E (r ) j H (r ) (7.42.1) H (r ) J (r ) j E(r ) j E(r ) (7.42.2) Assuming, as before, no free charges (v = 0) and following the same procedure: 2 E(r ) j j E(r ) 0 ELEN 3371 Electromagnetics Fall 2008 (7.42.3) 43 Plane wave propagation in a dielectric medium Assuming, as previously, that the electric field is linearly polarized in the y direction and the wave propagates in the z direction, we arrive to: d 2 Ey ( z) dz 2 j j E y ( z ) 0 d 2 Ey ( z) or dz 2 2 Ey ( z) 0 (7.43.1) (7.43.2) Where the propagation constant: j j j 1 j 2 2 ELEN 3371 Electromagnetics Fall 2008 (7.43.3) 44 Plane wave propagation in a dielectric medium The propagation constant is complex: j (7.44.1) In a vacuum, = 0 and = k. In a general case, the real and imaginary parts are nonlinear functions of the frequency: ( ) ( ) ELEN 3371 Electromagnetics 2 2 1 1 1 1 2 Fall 2008 2 (7.44.2) (7.44.3) 45 Plane wave propagation in a dielectric medium As a result, the phase velocity may depend on the wave’s frequency. This phenomena is called dispersion and the medium in which wave is propagating, is called a dispersive medium (every lossy medium). v p ( ) 1 (7.45.1) 2 1 1 2 Another quantity we recall here is the group velocity: vg ( ) ELEN 3371 Electromagnetics 1 1 2 1 2 2 2 2 2 1 1 1 1 2 Fall 2008 (7.45.2) 46 Plane wave propagation in a dielectric medium The component of the electric field propagating in the +z direction is: Ey ( z, t ) Ey 0e jt z E y 0e z e j t z (7.46.1) Wave propagates with a phase constant but the amplitude decreases with an attenuation constant . Units of are radians/m. Units of are nepers/m [Np/m]. If = 1 Np/m, the amplitude of the wave will decrease e times at a distance 1 m. 1 Np/m 8.686 dB/m. The characteristic impedance is: Z c ( ) ELEN 3371 Electromagnetics Ey ( z) H x ( z) j ( ) j ( ) Fall 2008 (7.46.2) 47 Plane wave propagation in a dielectric medium Example 7.8: A 10 V/m wave at the frequency 300 MHz propagates in the +z direction in an infinite medium. The electric field is polarized in the x direction. The parameters of medium are r = 9, r = 1, and = 10 S/m. Write the complete time domain expression for the electric field. We can find the attenuation constant as 2 1 1 2 10 4 107 1 36 10 36 2 9 10 1 1 6 9 2 300 10 9 10 9 2 108.01Np / m The phase constant is: 2 2 7 9 4 10 1 9 10 10 36 rad 8 1 1 2 3 10 1 1 109.65 2 2 36 2 3 108 9 109 m ELEN 3371 Electromagnetics Fall 2008 48 Plane wave propagation in a dielectric medium The complex propagation constant is 108 + j110 and the electric field is E ( z, t )10e108 z cos 2 3 108 t 110 z ux V m Example 7.9: Plot the phase velocity and the group velocity for the medium with r = 9, r = 1, and = 10 S/m The velocities can be described by (7.45.1) and (7.45.2). Both velocities increase with the frequency. The limit is the same: v c r ELEN 3371 Electromagnetics 108 m s Fall 2008 49 Plane wave propagation in a dielectric medium Two approximations are frequently used: A) A dielectric with small losses ( << ) with a high-frequency approximation: 1 1 2 2 (7.49.1) The approximate values for attenuation and propagation constants are: 2 ELEN 3371 Electromagnetics Fall 2008 (7.49.2) (7.49.3) 50 Plane wave propagation in a dielectric medium v vg 1 (7.50.1) In this situation, the phase and the group velocities are the same. Also, some attenuation is introduced. “A pizza in a microwave oven”: water in the pizza acts as a conductor turning pizza into a complex impedance. The wave passing through it decays, therefore, the energy is absorbed and must be converted into heat. B) A dielectric with large losses ( >> ) with a low-frequency approximation: The conduction current is much greater than the displacement current, therefore: H (r ) J (r ) j E (r ) E (r ) ELEN 3371 Electromagnetics Fall 2008 (7.50.2) 51 Plane wave propagation in a dielectric medium In this situation: 1 1 2 Therefore: (7.51.1) (7.51.2) 2 We introduce a skin depth of the material: 1 2 1 [m] f (7.51.3) The skin depth decreases with the increasing frequency – skin effect. ELEN 3371 Electromagnetics Fall 2008 52 Plane wave propagation in a dielectric medium Example 7.10: Estimate the skin depth of copper at a frequency of 3 GHz. The conductivity of copper is = 5.8 107 S/m; r = 1, and r = 1. 1 1 1.21106 m f 3 109 4 107 5.8 107 Plot the magnitude of the electric field of a plane wave for t = 0 and Ey0 = 10 V/m. 10 Check the validity of the lowfrequency approximation first: y E (z), V/m 0.1667 8 We can use the approximation. 6 4 2 0 ELEN 3371 Electromagnetics 0 Fall 2008 1 2 3 4 5 z, m 6 7 8 9 10 53 Plane wave propagation in a dielectric medium Imagine: if the “pizza in a microwave oven” was covered by a good conductor… The skin effect would lead to all energy being absorbed by a tiny layer of the conductor and the pizza would be cold. Finally, the characteristic impedance for an imperfect conductor is: Zcond (1 j ) 2 If the conductivity is large, Z approaches zero. ??QUESTIONS?? ELEN 3371 Electromagnetics Fall 2008 (7.53.1) 54 Polarization Polarization is the property of electromagnetic waves, such as light, that describes the direction of the transverse electric field. More generally, the polarization of a transverse wave describes the direction of oscillation in the plane perpendicular to the direction of travel. Longitudinal waves such as sound waves do not exhibit polarization, because for these waves the direction of oscillation is along the direction of travel. ELEN 3371 Electromagnetics Fall 2008 55 Polarization types Linear ELEN 3371 Electromagnetics Circular Fall 2008 Elliptical 56 Linear polarization In such arrangement with two parallel infinite plates, when applying a sinusoidal input to the system, the phase difference between voltages on the top and bottom plates will be 1800. The resulting electric field between the plates appears to have only one non-zero component and, therefore, said to be linearly polarized in the uy direction. Back ELEN 3371 Electromagnetics Fall 2008 57 Types of waves A transverse EM wave is a wave whose E and H vectors are perpendicular to the direction of wave’s propagation: light, radiowaves. A longitudinal EM wave would be a wave whose E and H vectors are parallel to the direction of wave’s propagation: sound. ELEN 3371 Electromagnetics Fall 2008 58 Types of transversal waves A plane wave is a constant-frequency wave whose wavefronts (surfaces of constant phase) are infinite parallel planes of constant amplitude normal to the phase velocity vector. By extension, the term is also used to describe waves that are approximately plane waves in a localized region of space. For example, a localized source such as an antenna produces a field that is approximately a plane wave in its far-field region. A wavefront ELEN 3371 Electromagnetics Fall 2008 59 Types of transversal waves A spherical wave is a constant-frequency wave whose wavefronts (surfaces of constant phase) are parallel concentric spheres of constant amplitude normal to the phase velocity vector. When the distance from the source is very large, a spherical wave can be locally approximated as a plane wave. Back ELEN 3371 Electromagnetics Fall 2008 60 Phase and group velocities The phase velocity of a wave is the rate at which the phase of the wave propagates in space. This is the velocity at which the phase of any single frequency component of the wave will propagate. We can pick one particular phase of the wave (for example the crest) and it would appear to travel at the phase velocity. Vp k Here, is a radial frequency and k is the wave number. The group velocity of a wave is the velocity with which the variations in the shape of the wave's amplitude (modulation or envelope of the wave) propagate through space. Vg k ELEN 3371 Electromagnetics Fall 2008 61 Phase and group velocities In the simple case of a pure traveling sinusoidal wave we can imagine a "rigid" profile being physically moved in the positive x direction with speed v. Clearly, the wave function depends on both time and position. At any fixed instant of time, the function varies sinusoidally along x, whereas at any fixed location on the x axis the function varies sinusoidally with time. If the wave profile is a solid entity sliding to the right, then obviously the phase velocity is the ordinary speed with which the actual physical parts are moving. However, we could also imagine the “magnitude" as the position along a transverse space axis, and a sequence of tiny massive particles along the x axis, each oscillating vertically. In this case the wave pattern propagates to the right with phase velocity vp, just as before, and yet no material particle has any motion at all. This illustrates that the phase of a traveling wave may or may not correspond to a particular physical entity. Back ELEN 3371 Electromagnetics Fall 2008