
Design a dielectric resonator oscillator in HFSS using boxes, cylinders, and two microstrip lines around a Rogers substrate. Set dimensions in millimeters, assign materials, and configure vacuum and ground planes.
Learn to simulate a dielectric resonator oscillator in hfss by creating lump ports, assigning excitations, configuring a solution setup and frequency sweep, and optimizing for a 10 ghz resonance.
Simulate an inverted L antenna in HFSS, including FR-4 substrate, airbox, ground plane, and a parametric port, then validate results and observe resonance near 2.45 GHz.
Discover how to simulate the inverted F antenna with HFSS, configuring the ground plane, substrate height, vias, and top-layer geometry. Analyze resonance around 2.4 GHz, noting real and imaginary parts.
Simulate mila meander inverted-L antenna in hfss, configure substrate, airbox, ground plane, and terminal port excitation, and analyze resonance at 2.45 ghz with return loss and radiation patterns.
Learn to design and simulate a meander-line inverted-F antenna (MIFA) in HFSS, focusing on excitation, vias, ground plane, and substrate for a 2.45 GHz resonance with 50-ohm impedance and VSWR.
Learn to simulate a monopole PCB antenna in HFSS, connecting a meander-line F antenna to a board with a 50-ohm excitation, observing resonance, gain, and radiation pattern.
Simulate a meander inverted antenna with lumped RLC components, incorporating capacitor and inductor values connected to the SoC, for 50 ohm excitation and 0.86GHz matching.
Learn to simulate a 13.56 MHz NFC RFID antenna in HFSS software, configure excitation and a parametric inductance value, and connect top and bottom layers with vias for accurate results.
Simulate the NFC RFID antenna with lumped RLC in HFSS, define 50-ohm ports, and tune resonance near 13.56 MHz by adjusting inductance and capacitance.
Learn to simulate and optimize a 13.56 MHz NFC RFID antenna in HFSS by setting parametric variables, adjusting width and inductance, and evaluating radiation boundaries and port excitations.
Explore how to measure and analyze the coupling between two 13.56 MHz NFC RFID antennas in HFSS, sweeping distance from 5 to 50 mm and examining S11 and S21.
Simulate a six-cell dipole antenna array in HFSS by duplicating a single cell, setting the excitation port, and sweeping 2.5–3.5 GHz to analyze the resonance.
Simulate a free array dipole antenna in HFSS software, with three ports and three excitations, achieving a resonance frequency of 2.95 and a 3D model.
In this course, different type of Antennas such as ILA (Inverted L Antenna), IFA (Inverted F Antenna), MILA (Meandered L Antenna), MIFA (Meandered F Antenna), 13.56 MHz NFC, 3 Array & 6 Array Dipole Antenna and DRO (Dielectric Resonator Oscillators) is simulated with HFSS Software. HFSS file of designs are available for download. HFSS software is common software for microwave and RF applications. You will have a priority in the industry, if you have knowledge and experience in HFSS in order to participate in projects related to radar system, communication systems, wireless technology, GSM, GPS and defense industry, satellite communication, aircraft radars and space applications.
In this course, we start with short overview about DRO(Dielectric Resonator Oscillators) and then we will simulate 10 GHz DRO with HFSS Software. then we will continue to simulate diffrent types of PCB Antennas with HFSS software. PCB antenna refers to the antenna printed on the PCB circuit board, which has the advantages of simple manufacturing and low cost, and is widely used Applications such as Bluetooth (Bluetooth), WiFi, Wireless mouse, Zigbee and other shortdistance wireless devices. then we will simulate 13.56 MHz NFC antenna which has huge application in RFID industry. we will discuss about optimizing the NFC antenna and how to match it with RLC components. at the end, we will simulate 3 Array and 6 Array Dipole Antenna at HFSS software. an antenna Array is a radiating system, which consists of individual radiators and elements. Each of this radiator, while functioning has its own induction field. The elements are placed so closely that each one lies in the neighbouring one’s induction field. Therefore, the radiation pattern produced by them, would be the vector sum of the individual ones.