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Maxwell's Equations; Polarization; Poynting's Vector (PDF) Maxwell’s Equations (free space) Integral form Differential form MIT 2.71/2.710 03/18/09 wk7-b- 8 Wave Equation for electromagnetic waves MIT 2.71/2.710 03/18/09 wk7-b- 9 Electric fields in matter atom under electric field: • charge neutrality is preserved • spatial distribution of charges becomes assymetric Dipole moment Polarization Spatially variant polarization induces local charge imbalances (bound charges) Fig. 3.38 in Hecht, Eugene. Optics. Reading, MA: Addison-Wesley, 2001. ISBN: 9780805385663. (c) Addison-Wesley. All rights reserved. This content MIT 2.71/2.710 is excluded from our Creative Commons license. For more information, 03/18/09 wk7-b-10 see http://ocw.mit.edu/fairuse. Constitutive relationships E: electric field D: electric displacement polarization “Spring” binding the electron to the nucleus is linear: i.e., electron displacement as function of electric force is given by Hooke’s law with spring constant B: magnetic induction H: magnetic field magnetization Most optical materials are non magnetic at optical frequencies, i.e. M=0; therefore, B=μ0 Fig. 3.38 in Hecht, Eugene. Optics. Reading, MA: Addison-Wesley, 2001. ISBN: 9780805385663. (c) Addison-Wesley. All rights reserved. This content MIT 2.71/2.710 is excluded from our Creative Commons license. For more information, 03/18/09 wk7-b-11 see http://ocw.mit.edu/fairuse. Maxwell’s equations in constitutive form Vacuum Matter with free Matter without free charges and currents charges or currents Wave equation in matter but without free charges or currents becomes: MIT 2.71/2.710 03/18/09 wk7-b-12 k, E, B form a right-handed triad . In free space or isotropic media, the vectors k, E, B form a right-handed triad. Fig. 3.13, 3.14 in Hecht, Eugene. Optics. Reading, MA: Addison-Wesley, 2001. ISBN: 9780805385663. (c) Addison-Wesley. All rights reserved. This content is excluded from ourCreative Commons license. For more information, MIT 2.71/2.710 see http://ocw.mit.edu/fairuse. 03/18/09 wk7-b-13 The Poynting vector E S 㱻 In the case of harmonic waves, B E k 㱺 B MIT 2.71/2.710 03/18/09 wk7-b-14 Irradiance (aka Intensity) From the definition of the Poynting vector and the k, E, B relationship, For a harmonic (sinusoidal) wave propagating along z Recall at optical frequencies, the field oscillates very rapidly, ~10141015 Hz. Therefore, opto-electronic detectors only register the average energy flux This referred to as irradiance or intensity of the optical field, and is measured in units of W/m2 (more commonly W/cm2) (T=2/ or integral multiples) Since for the harmonic wave the intensity is MIT 2.71/2.710 03/18/09 wk7-b-15 Calculation of the intensity from phasors Recall the phasor representation of a harmonic wave We cannot quite represent the Poynting vector as a phasor, because the Poynting vector is obtained as a product of the E, B fields (recall we may only add or subtract phasors; we are not allowed to do nonlinear operations with them.) Nevertheless, we can obtain the intensity (time-averaged Poynting vector) from the phasor as follows: Consider the time-averaged superposition of Now consider the corresponding two fields at the same frequency: phasors: and form the quantity Clearly, MIT 2.71/2.710 03/18/09 wk7-b-16 MIT OpenCourseWare http://ocw.mit.edu 2.71 / 2.710 Optics Spring 2009 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms..
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