![]() ![]() When Phillip Smith was working at Bell Labs, he have to match one antenna and he was looked for a way to solve the design graphically. In this post, I will try to show the handling of the three-dimensional Smith Chart and its application for a low-noise amplifier design. Advances in 3D rendering software make it easy to use for design. Last years, three-dimensional Smith Chart has become popular. However, the 2D format has some restrictions when the active impedances (oscillators) or stability circles (amplifiers) are represented, since these ones usually leave the polar chart. Traditionally, the Smith Chart has been used as 2-D polar form, centered at an unit radius circle. Developed by Phillip Smith in 1939, it has become the most popular graphic method for representing impedances and solving operations with complex numbers. The mathematical theory of the 3D Smith chart 1 unifies active and passive microwave circuit design on the surface of a Riemann sphere.ġ Representation of the 2D (a) and 3D (b) Smith charts.The Smith Chart is a standard tool in RF design. The reflection coefficient plane is mapped stereographically through the South Pole on the surface of a unit sphere. As a result, the classical 2D Smith chart including the passive loads 2 is mapped stereographically into the North hemisphere, while the circuits with negative resistance (that are outside the classical planar Smith chart) are mapped into the South one. The East hemisphere is the place of inductive circuits, whereas the West hemisphere hosts the capacitive circuits. ![]() Meantime, the Greenwich meridian is the locus of pure resistive circuits (see Figure 1, where the constant resistance r and reactance x circles are drawn in blue and red, respectively). The 3D Smith chart differs from previous attempts 4 to generalize the planar 2D Smith chart in a fundamental way: the way in which infinity is treated. The preceding theories fail to merge the active and passive worlds in a simple and rigorous manner, since they propose an empirical solution to map an infinite region into a finite surface. These approaches turned into complicated transforming equations, making the visual and intuitive interpretation of microwave problems very difficult. In this article, how the 2D and 3D Smith charts deal with the infinite regions are first described. Next, the advantages of using the 3D Smith chart to represent both active and passive loads are illustrated with two examples: the stability circles of an amplifier and the impedance of a microwave oscillator. The infinite region of the normalized impedance or z-plane is due to the open circuit, because the magnitude of the input impedance grows to infinity as the load tends to an open circuit. Since in practical applications, impedances can be found close to the open circuit, it is rather uncommon to use the z-plane to perform a visual representation of loads.įor the reflection coefficient plane (ρ-plane), the infinite region corresponds to the load with the same magnitude and opposite sign to the characteristic impedance of the line (that is the infinite mismatch or z = –1 in normalized impedance terms). Although it denotes a particular active load, this input impedance is important in some practical applications such as oscillator design.
0 Comments
Leave a Reply. |