Back
ExamFull examSolution only

EMSP 27jun2022 with solutions

Full exam for ELECTROMAGNETICS AND SIGNAL PROCESSING FOR SPACEBORNE APPLICATIONS in the Aerospace Engineering degree programme at Politecnico di Milano. The document covers: Electromagnetics and Signal Processing for Spaceborne Applications June 27th, 2022 1 2 3 4 do not write above Problem 1 A plane sinusoidal EM wave (f = 9 GHz) propagates from a medium with electric permittivity r1 = 3 into free space (assume r = 1 for both media). The

ELECTROMAGNETICS AND SIGNAL PROCESSING FOR SPACEBORNE APPLICATIONSFull exam

Document information

What's included in this study material

Full exam for ELECTROMAGNETICS AND SIGNAL PROCESSING FOR SPACEBORNE APPLICATIONS in the Aerospace Engineering degree programme at Politecnico di Milano. The document covers: Electromagnetics and Signal Processing for Spaceborne Applications June 27th, 2022 1 2 3 4 do not write above Problem 1 A plane sinusoidal EM wave (f = 9 GHz) propagates from a medium with electric permittivity r1 = 3 into free space (assume r = 1 for both media). The

Import quality: text was extracted directly from the original document.

Extracted content from the document

Representative passages recognised in different parts of the material. The full extracted text remains available to search, while this compact preview makes the page easier to read.

Page 1

Electromagnetics and Signal Processing for Spaceborne Applications June 27th, 2022 1 2 3 4 do not write above Problem 1 A plane sinusoidal EM wave (f = 9 GHz) propagates from a medium with electric permittivity r1 = 3 into free space (assume r = 1 for both media). The expression of the incident electric field is: 𝐸⃗ 𝑖(𝑧,𝑦)= 𝐸0 (√3 2 𝜇 𝑦 + 1 2𝜇 𝑧 + 𝑗 2𝜇 𝑥)𝑒−𝑗𝛽√3 2 𝑧𝑒𝑗𝛽 2𝑦 V/m 1) 1 Determine the incidence angle . 2) 2 Determine the polarization of the incident field 𝐸⃗ 𝑖 (it is sufficient to state whether the polarization is elliptical, circular or linear; additional details, such as rotation direction or tilt angle, are not required). 3) 3 Determine the polarization of the reflected field 𝐸⃗ 𝑟. 4) 4 Calculate the absolute value of E0 by knowing that the power density of the electric field in A(x = -1 m, y = -1 m, z = -1 m) is ST = 0.5 W/m 2 (consider only the contribution of the reflected field). Solution 1) The incidence angle can be derived, for example, from the y component of : 𝛽𝑦 = 𝛽sin(𝜃)= 𝛽/2  sin(𝜃)= 1/2  𝜃 = 30° SURNAME AND NAME ____________________________________________________ ID NUMBER ___________________________________________________________ SIGNATURE ___________________________________________________________ y z 2 1  A 2) The wave has two components: a TE one, along x, and a TM one, given by the combinations of the two fields along y and z. The absolute value of the components is E0 V/m (TM) and E0/2 V/m (TE), and the differential phase shift is /2 3) Considering that the wave also has a TM component, it is worth checking the Brewster angle: 𝜃𝐵 = tg−1 (√ 𝜀𝑟2 𝜀𝑟1 ) = 30° As  = B  the TM component is totally transmitted into the second medium. As a result, the polarization of the reflected wave will be linear (along x). 4) To determine E0, it…

Preview

First page of the document.

First page: EMSP 27jun2022 with solutions