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No energy is transferred through the media boundary and the fields in envelope nodes have values equal to 0. 0000000016 00000 n 2.5: Plane wave incident normally on a plane conducting boundary, Consider the situation in Fig. Get step-by-step explanations, verified by experts. 0000009392 00000 n • Reflection & Transmission (Normal Incidence) • Reflected & Transmitted Power • Optical Materials, Perfect Conductors, Metals TRUE or FALSE . 0000010657 00000 n 0000004790 00000 n -���;k�~ R ` ��@� endstream endobj 49 0 obj 222 endobj 34 0 obj << /Type /Page /Parent 30 0 R /Resources << /Font << /F6 45 0 R /F5 44 0 R /F7 46 0 R /F4 41 0 R /F3 35 0 R >> /ExtGState << /R4 47 0 R >> /ProcSet [ /PDF /Text ] >> /Contents 36 0 R /MediaBox [ 0 0 612 792 ] /CropBox [ 0 0 612 792 ] /Rotate 0 >> endobj 35 0 obj << /Type /Font /Subtype /Type1 /Name /F3 /BaseFont /Helvetica-Bold >> endobj 36 0 obj << /Filter /FlateDecode /Length 37 0 R >> stream v�Ѳ\uj���~��u�k����a+�h��&31 g��׃r].w�stT� GvDH3\S�˭�{$�ڪ��O����H�� ��]��X[ BJ��M/Ok��-��[)C9S�>���MN��_���M�j`����5!u�Fg�h)��,�>��+������o��f�נ=�d�E:mq���0��O��q�ʱ�z� U�=��K���& MWntt�̨,!W�nE>�S%����Zc��wy ���p�3�`�[Q 0000005785 00000 n intrinsic impedance respectively, of medium 1. By using the previous formulas, we have: Why did we study polarization in the previous post and now we study the incidence? What is the value of the wave impedance in the conductor? 0000000813 00000 n The conductor may be considered to be a perfect conductor. 0000006804 00000 n Figure 57 shows the coefficients of reflection (solid curves) and transmission (dashed curves) for oblique incidence from air to glass (). In this case an envelope of a standing wave will be demonstrated. H�b```f``������[��À �@����ș���Qmp���!v%����kgT�X"��D��-8#�M55���o�ޥb;�&m:s�&?m�Np��#{r�ZrkEf�i7�i��cu"��II�ص�c 0q 1.2.2      Normal incidence of a plane wave on a perfect conductor surface. =�'Z���e�M�DR�*D 1.2.2 Normal incidence of a plane wave on a perfect conductor surface. 2.5 where the incident wave travels in the, . x��Y[�G�!0����m�ӜH;��� !�k%ON@{,�-���W=]U=��-8^�:U�]]������j�l���������nr����9��V�`҆�o'r=y���������X�WO����͋��?#�1s2���ߦ�a����72ik�P��=�β�{��a!����L��S�^v$J��1>5ߚB�3_�L��S�~ 0000000762 00000 n In this case an envelope of a standing wave will be demonstrated. Its name refers to the shape of a wave front (constant phase surfaces, perpendicular to the direction of propagation) of … endstream endobj 893 0 obj<>/Size 870/Type/XRef>>stream )j�1S�ZZ��Y��'я�X, k�UJCQ1�R�WPP �Ȩi�`Za��F�d0Pߛ���vmߥY��Z"3�E���H{5��i�&�ɐf>�4Oʮ&�s��w��Y�۪m:*�KCu�l+^��mj��������[���#�O �Nhc��e��j�93��N�)�L�mt� Thus, we obtained the correct answer because we were able to independently determine that η 2 = 0 in a perfect conductor. Course Hero is not sponsored or endorsed by any college or university. Reflection Coefficient and its Dependency on Angle of Incidence. Save my name, email, and website in this browser for the next time I comment. 0000004975 00000 n There are important applications where these two concepts are developed: And these are just some of the simplest applications. Incident wave reflected wave . ���4G�z��L�0�������Z�{Ǥgݮ�Rhe�g�ˡƱp�v�����O;��ZH��7���}����#��X�U�*� �������.a����sT偍��H`��*�0��Ĝ�V�CG ���T�vת;�L��A���F��lKQbCl�*)RIc% �T�D L��9xU�� R�@���$��� "��^��>d�P��DҺ ˤ��)sTI�Ux)EY[s H�|��n�0E��/[U�� $Ģ�E�(i�7�Y For this incompletely defined example, the initial part of Step 2 of the method involves refinement of the problem definition by describing more explicitly the incident wave, for example: E (z,t )= xˆEo cos (ωt − kz) ⎣⎡Vm-1⎤⎦ (9.1.1) The field inside a perfect conductor is zero. stream %PDF-1.4 %���� Normal Incidence Plane Wave Reflection at Perfect Conductor At the boundary, since and are both 0, then: Solution exists for Then, This is our old friend, the standing wave! Fig. 1. When Region 2 is a perfect conductor, the reflection coefficient Γ 12 = − 1 and the solution described in Equations 5.1.18 and 5.1.19 applies. 6.2 Plane wave reflection from media interface at normal incidence The reflection coefficient is defined as the ratio of amplitude of the reflected electric field divided by amplitude of the incident electric field as follows: Γ = Er 20 Electromagnetic Field Theory by R. S. Kshetrimayum 3/20/2018 The reflected magnetic field can be obtained from the %�쏢 We regularly blog in our spare time. CHECK YOUR UNDERSTANDING-2 (FETs)-Review of basics and examples.pdf, Design of Educational programs by the healthcare providers.docx, Korea Advanced Institute of Science and Technology, Chapter10-Electromagnetic wave propagation-2015-V2 (1), University of California, San Diego • ECE 107, Korea Advanced Institute of Science and Technology • EE 204. 0000002247 00000 n This preview shows page 1 - 4 out of 39 pages. 0000088418 00000 n endstream endobj 871 0 obj<>/Metadata 252 0 R/Pages 242 0 R/StructTreeRoot 254 0 R/Type/Catalog/Lang(EN)>> endobj 872 0 obj<>/ProcSet[/PDF/Text]/ExtGState<>>>/Type/Page>> endobj 873 0 obj<> endobj 874 0 obj<> endobj 875 0 obj<> endobj 876 0 obj<> endobj 877 0 obj<>stream �c���x2��A_'���8Ǵ*1��2�I�����zj�����/֔}ղܷ�F�s �g endstream endobj 878 0 obj<> endobj 879 0 obj<> endobj 880 0 obj<>stream Notify me of follow-up comments by email. 0000006893 00000 n boundary is an interface with a perfect conductor (medium 2: considered: normal incidence and oblique incidence. Introducing Textbook Solutions. The left-hand panel shows the wave polarization for which the electric field is parallel to the boundary, whereas the right-hand panel shows the wave polarization for which the magnetic field is parallel to the boundary. 0000010220 00000 n 0000005911 00000 n C5 Switch to excisting field component i.g. Plane Wave Reflections at a Conductor Power and reflection coefficient at dielctric boundary. 0000000707 00000 n ��ɷ��5�n� tP2Gp*J4�(Lp��������+��X�Iz��"K/���I�i�t�l�C&������0�_c�h�\�4Ĕ�Bbz���!�Q��3Z�?�*`�o��{��(�Ķ��'r6�CX�ٳ�ʙ�*jJ��*�{�|�K�`y����y�L���P:��1�X� �2cđδ�ްN��$�riɵ܀��k�ڙP�\J厌��W֏�a�#c]�>w�ʭ��t�L��.���F�r�x���h��],Ér�F8����-C}������F�M�¸U.�ٸ�3?��A���+�9��9�Ѕ���$㤱9�����ާ7�K@�oL�(�W���U�@�" rC�����є��C�G� > endobj 39 0 obj << /Type /Encoding /Differences [ 0 /NUL 9 /HT 10 /LF 13 /CR 127 /DEL 128 /Adieresis ] >> endobj 40 0 obj << /Filter /FlateDecode /Length 1237 /Subtype /Type1C >> stream -         Change the medium of section 2 to metal by editing Medium parameter of the section2 object (see Fig. Reflection and Refraction of Plane Waves NORMAL INCIDENCE AT A PLANE … leZ჏_}�/h:�6�܂�e&��;�^���������� YQ-7��N��'i}jJe�S�CLA9���)(���2�x���[tՐf�-���Э�^�$�JP��a�ʻ h��y�/�CM�.��y�-��g��q˯��͸Т�W_���P�_�{?�YZ��&o�#J���Qo�6>�J]h��������Fm8�=�n}p�h�M�˧t�Z. Hy. 1 + 21 12. cos sin cos sin kd j kd kd j kd. 6.2 Plane wave reflection from media interface at normal incidence 6.2.2 Lossless medium If the regions are lossless dielectric, then, σ = 0 and µ and ε are real quantities The propagation constant for this case is purely imaginary and can be written as 25 Electromagnetic Field Theory by …

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