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- https://eng.libretexts.org/Bookshelves/Electrical_Engineering/Electronics/Microwave_and_RF_Design_III_-_Networks_(Steer)/00%3A_Front_Matter/01%3A_TitlePageDefault Text
- https://eng.libretexts.org/Bookshelves/Electrical_Engineering/Electronics/Microwave_and_RF_Design_II_-_Transmission_Lines_(Steer)/05%3A_Coupled_Lines_and_Applications/5.03%3A_Coupled_Transmission_Line_TheoryThus the coupled pair of conductors supports two unique families of modes (each family comprising forward- and backward-traveling waves) with each family relating to a particular field configuration o...Thus the coupled pair of conductors supports two unique families of modes (each family comprising forward- and backward-traveling waves) with each family relating to a particular field configuration on the coupled line system.2 That is, S1 and S2 are each single numbers and, just considering the forward-traveling waves, ωS1 is the propagation constant of one mode and ωS2 is the propagation constant of the second mode.
- https://eng.libretexts.org/Bookshelves/Electrical_Engineering/Electronics/Book%3A_Fundamentals_of_Microwave_and_RF_Design_(Steer)/10%3A_Impedance_Matching/10.02%3A_Matching_Networks\[\begin{align}\Gamma_{\text{in}}^{\ast}&=\frac{Z_{\text{in}}-Z_{\text{REF}}}{Z_{\text{in}}+Z_{\text{REF}}}=\left(\frac{Z_{S}^{\ast}-Z_{\text{REF}}}{Z_{S}^{\ast}+Z_{\text{REF}}}\right)^{\ast} =\frac{(...Γ∗in=Zin−ZREFZin+ZREF=(Z∗S−ZREFZ∗S+ZREF)∗=(Z∗S−Z0)∗(Z∗S+Z0)∗=(Z∗S)∗−Z∗REF(Z∗S)∗+Z∗REF=ZS−Z∗REFZS+Z∗REF=ΓS
- https://eng.libretexts.org/Bookshelves/Electrical_Engineering/Electronics/Book%3A_Fundamentals_of_Microwave_and_RF_Design_(Steer)/07%3A_Microwave_Network_Analysis/7.06%3A_SummaryWhich is used depends on which makes the task of visualizing circuit operation more clear, which makes analyzing circuits more convenient, and which enables different circuits to be made electrically ...Which is used depends on which makes the task of visualizing circuit operation more clear, which makes analyzing circuits more convenient, and which enables different circuits to be made electrically equivalent. RF and microwave design is characterized by conceptual insight and it is essential to use parameters and graphical representations that are close to the physical world.
- https://eng.libretexts.org/Bookshelves/Electrical_Engineering/Electronics/Book%3A_Fundamentals_of_Microwave_and_RF_Design_(Steer)/04%3A_Planar_Transmission_Lines/4.02%3A_SubstratesThe characteristics of the line are then more or less the same as for the same structure with a uniform dielectric of permittivity, εeff=εeε0. So th...The characteristics of the line are then more or less the same as for the same structure with a uniform dielectric of permittivity, εeff=εeε0. So the energy lost in the dielectric is proportional to ωε″ and the energy stored in the electric field is proportional to \omega\varepsilon '.
- https://eng.libretexts.org/Bookshelves/Electrical_Engineering/Electronics/Microwave_and_RF_Design_I_-_Radio_Systems_(Steer)/05%3A_RF_Systems/5.07%3A_4G_Fourth_Generation_RadioIf the time duration of a symbol is short, which is the case if wideband modulation is used, then the components of a signal, corresponding to one symbol, following longer paths could arrive at the sa...If the time duration of a symbol is short, which is the case if wideband modulation is used, then the components of a signal, corresponding to one symbol, following longer paths could arrive at the same time as the components of the next symbol following shorter paths.
- https://eng.libretexts.org/Bookshelves/Electrical_Engineering/Electronics/Microwave_and_RF_Design_II_-_Transmission_Lines_(Steer)/04%3A_Extraordinary_Transmission_Line_Effects/4.10%3A_Lines_on_Semiconductor_Substrates\[\begin{align}\label{eq:1}C_{1}&=\varepsilon_{1}\frac{A}{d_{1}},\: R_{1}=\frac{1}{\sigma_{1}}\frac{d_{1}}{A},\:C_{2}=\varepsilon_{2}\frac{A}{d_{2}},\:R_{2}=\frac{1}{\sigma_{2}}\frac{d_{2}}{A} \\ \lab...\begin{align}\label{eq:1}C_{1}&=\varepsilon_{1}\frac{A}{d_{1}},\: R_{1}=\frac{1}{\sigma_{1}}\frac{d_{1}}{A},\:C_{2}=\varepsilon_{2}\frac{A}{d_{2}},\:R_{2}=\frac{1}{\sigma_{2}}\frac{d_{2}}{A} \\ \label{eq:2}\tau_{1}&=R_{1}C_{1}=\frac{\varepsilon_{1}}{\sigma_{1}},\:\tau_{2}=R_{2}C_{2}=\frac{\varepsilon_{2}}{\sigma_{2}}\end{align}
- https://eng.libretexts.org/Bookshelves/Electrical_Engineering/Electronics/Book%3A_Fundamentals_of_Microwave_and_RF_Design_(Steer)The book series Microwave and RF Design is a comprehensive treatment of radio frequency (RF) and microwave design with a modern “systems-first” approach. Design is oriented towards cellular communicat...The book series Microwave and RF Design is a comprehensive treatment of radio frequency (RF) and microwave design with a modern “systems-first” approach. Design is oriented towards cellular communications and microstrip design so that lessons learned can be applied to real-world design tasks. The books in the Microwave and RF Design series are: Radio Systems (Volume 1), Transmission Lines (Volume 2), Networks (Volume 3), Modules (Volume 4), and Amplifiers and Oscillators (Volume 5).
- https://eng.libretexts.org/Bookshelves/Electrical_Engineering/Electronics/Book%3A_Fundamentals_of_Microwave_and_RF_Design_(Steer)/01%3A_Introduction_to_Microwave_Engineering/1.02%3A_Radio_ArchitectureThe discrete channels are capable of being reused within the service area.” The key attributes here are (a) the concept of cells arranged in clusters and the total number of channels available is divi...The discrete channels are capable of being reused within the service area.” The key attributes here are (a) the concept of cells arranged in clusters and the total number of channels available is divided among the cells in
- https://eng.libretexts.org/Bookshelves/Electrical_Engineering/Electronics/Book%3A_Fundamentals_of_Microwave_and_RF_Design_(Steer)/03%3A_Transmission_Lines/3.04%3A_Special_Cases_of_Lossless_Terminated_Lines\label{eq:29} Z_{\text{in}}=Z_{0}\frac{Z_{01}+\jmath Z_{0}\tan (\beta\ell)}{Z_{0}+\jmath Z_{01}\tan (\beta\ell)}=Z_{0}\frac{Z_{01}+\jmath Z_{0}∞}{Z_{0}+\jmath Z_{01}∞}=\frac{Z_{0}^{2}}{Z_{01}} Th...\label{eq:29} Z_{\text{in}}=Z_{0}\frac{Z_{01}+\jmath Z_{0}\tan (\beta\ell)}{Z_{0}+\jmath Z_{01}\tan (\beta\ell)}=Z_{0}\frac{Z_{01}+\jmath Z_{0}∞}{Z_{0}+\jmath Z_{01}∞}=\frac{Z_{0}^{2}}{Z_{01}} The layout of a microstrip quarter-wave transformer is shown in Figure \PageIndex{13}, where \ell = \lambda_{g}/4 and the characteristic impedance of the transformer, Z_{0}, is the geometric mean of the impedances on either side, that is, Z_{0} =\sqrt{Z_{01}Z_{02}}.
- https://eng.libretexts.org/Bookshelves/Electrical_Engineering/Electronics/Microwave_and_RF_Design_V%3A_Amplifiers_and_Oscillators_(Steer)/zz%3A_Back_Matter/01%3A_Index