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Intro to Multiport Analysis — Course Overview
In this course we will introduce multiport network analysis methods, which describe a network purely through its externally observable behavior at a finite number of ports. This course was created for Ansys Innovation Courses by Dr. Kathryn Leigh Smith, assistant professor, UNC-Charlotte, in partnership with Ansys.
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// INTERESTED IN MORE?
Visit Ansys Innovation Courses for free courses that include videos, handouts, simulation examples with starting files, homework problems and quizzes.
Visit today → bit.ly/3Eo8esU
// DOWNLOAD FREE ANSYS SOFTWARE
Ansys offers free student product downloads for homework, capstone projects, student competitions, online learning and more!
Download today → bit....
Просмотров: 5 124
Видео
Calculating S-Parameters - Lesson 3
Просмотров 28 тыс.2 года назад
In this lesson we will work through the calculation of S-parameters for a simple example two-port network. This course was created for Ansys Innovation Courses by Dr. Kathryn Leigh Smith, assistant professor, UNC-Charlotte, in partnership with Ansys. // INTERESTED IN MORE? Visit Ansys Innovation Courses for free courses that include videos, handouts, simulation examples with starting files, hom...
What are S-parameters? - Lesson 2
Просмотров 14 тыс.2 года назад
This lesson will define the scattering parameters (S-parameters) of a network, which describe the reflections and transmissions of voltage waves impinging on the network ports. This course was created for Ansys Innovation Courses by Dr. Kathryn Leigh Smith, assistant professor, UNC-Charlotte, in partnership with Ansys. // INTERESTED IN MORE? Visit Ansys Innovation Courses for free courses that ...
Intro to Basics of S-parameters - Lesson 1
Просмотров 13 тыс.2 года назад
In this lesson we will discuss scattering parameters, or S-parameters. We will first talk through the definition of the S-parameters, then we will work through an example. This course was created for Ansys Innovation Courses by Dr. Kathryn Leigh Smith, assistant professor, UNC-Charlotte, in partnership with Ansys. // INTERESTED IN MORE? Visit Ansys Innovation Courses for free courses that inclu...
Multiport Parameters ([S], [Z], [Y], and [ABCD] Parameters) - Lesson 3
Просмотров 5 тыс.2 года назад
This lesson will briefly introduce four commonly used multiport parameters: Z-parameters, Y-parameters, S-parameters, and [ABCD] parameters. This course was created for Ansys Innovation Courses by Dr. Kathryn Leigh Smith, assistant professor, UNC-Charlotte, in partnership with Ansys. // INTERESTED IN MORE? Visit Ansys Innovation Courses for free courses that include videos, handouts, simulation...
The Black Box Model - Lesson 2
Просмотров 3 тыс.2 года назад
This lesson introduces black box models, which characterize a system by focusing entirely on externally observable characteristics while ignoring all the internal mechanisms by which those characteristics are achieved. This course was created for Ansys Innovation Courses by Dr. Kathryn Leigh Smith, assistant professor, UNC-Charlotte, in partnership with Ansys. // INTERESTED IN MORE? Visit Ansys...
Intro to Multiport Analysis - Lesson 1
Просмотров 2,3 тыс.2 года назад
In this lesson we will introduce multiport analysis methods. We will begin by introducing the black box model and then look specifically at four examples of multiport analysis methods. This course was created for Ansys Innovation Courses by Dr. Kathryn Leigh Smith, assistant professor, UNC-Charlotte, in partnership with Ansys. // INTERESTED IN MORE? Visit Ansys Innovation Courses for free cours...
Viewing Simulation Results In HFSS - Lesson 3
Просмотров 5 тыс.3 года назад
Once your dipole antenna array has finished simulating in HFSS, you are ready to view the results of your simulation. There are many different options for viewing various aspects of this simulation. This lesson will look at the method for generating a few of the most important plots. This lesson is part of the Ansys Innovation Course: Simulating a Dipole Array in HFSS. To access this and all of...
Setting Up an Antenna Array in Ansys HFSS - Lesson 2
Просмотров 12 тыс.3 года назад
In this lesson, we will discuss the process for building a simulation model for an antenna array consisting of five half-wave dipole elements arranged linearly along the x-axis, with an inter-elemental spacing of one wavelength and with the feed phase constant along the length of the array. This course was created for Ansys Innovation Courses by Dr. Kathryn Leigh Smith, assistant professor, Uni...
Intro to Simulating a Dipole Array in Ansys HFSS - Lesson 1
Просмотров 3,8 тыс.3 года назад
In this lesson, we will do a walkthrough for simulating an array of antennas in Ansys HFSS. We will specifically be building an array of five half-wave dipole elements arranged linearly along the x-axis, with an inter-elemental spacing of one wavelength and with the feed phase constant along the length of the array. This course was created for Ansys Innovation Courses by Dr. Kathryn Leigh Smith...
Manipulating the Array Factor - Lesson 4
Просмотров 8 тыс.3 года назад
This lesson takes a graphical look at the effect of varying the array components of a uniform array that can be used to manipulate the array factor. Specifically, it looks at the effect of varying the distance between array elements, the number of array elements, and the phase difference between neighboring elements. This course was created for Ansys Innovation Courses by Dr. Kathryn Leigh Smit...
Uniform Antenna Arrays - Lesson 3
Просмотров 10 тыс.3 года назад
This lesson introduces uniform antenna arrays, which are arrays comprised of a collection of identical elements all driven with the same signal amplitude, having equal spacing between neighboring elements, and a progressively stepped phase shift along the length of the array. This course was created for Ansys Innovation Courses by Dr. Kathryn Leigh Smith, assistant professor, University of Nort...
Defining the Array Factor - Lesson 2
Просмотров 11 тыс.3 года назад
This lesson introduces the antenna array factor. Antenna arrays consisting of a collection of identical elements are usually characterized in terms of their array factor. The array factor of any given array of identical antenna elements is a product of the number of elements, the relative input signals (magnitude and phase) of the various elements, and the geometric arrangement of the elements....
Intro to Basics of Antenna Arrays - Lesson 1
Просмотров 12 тыс.3 года назад
When two or more radiating elements are operated in close proximity to one another, the interference of their radiated fields can become a major factor in determining their collective radiation pattern. Antenna engineers leverage this fact to their advantage by creating antenna arrays - collections of proximate antennas that are designed to operate cohesively to produce a desired pattern of rad...
Dipole Radiation Pattern Over Frequency - Lesson 3
Просмотров 4,2 тыс.3 года назад
This lesson introduces the variation seen in the far-field radiation pattern of a dipole antenna as the driving frequency changes. At the frequency where the length of the antenna is equal to half a wavelength, the antenna radiates a single-lobed pattern focused broadside to the length of the antenna, but the number of lobes and strength of the radiation varies greatly with frequency. We will l...
Dipole Input Impedance Over Frequency - Lesson 2
Просмотров 6 тыс.3 года назад
Dipole Input Impedance Over Frequency - Lesson 2
Intro to Frequency Characteristics of The Half-Wave Dipole - Lesson 1
Просмотров 3,4 тыс.3 года назад
Intro to Frequency Characteristics of The Half-Wave Dipole - Lesson 1
The Theoretical Radiation Pattern of a Half-wave Dipole - Lesson 3
Просмотров 13 тыс.3 года назад
The Theoretical Radiation Pattern of a Half-wave Dipole - Lesson 3
The Current Structure on a Half-wave Dipole - Lesson 2
Просмотров 20 тыс.3 года назад
The Current Structure on a Half-wave Dipole - Lesson 2
Intro to Design of the Half-wave Dipole - Lesson 1
Просмотров 6 тыс.3 года назад
Intro to Design of the Half-wave Dipole - Lesson 1
Design of the Half-Wave Dipole - Overview
Просмотров 8763 года назад
Design of the Half-Wave Dipole - Overview
The Cylindrical Coordinate System - Lesson 8
Просмотров 3 тыс.3 года назад
The Cylindrical Coordinate System - Lesson 8
The Rectangular Patch Antenna - Lesson 5
Просмотров 27 тыс.3 года назад
The Rectangular Patch Antenna - Lesson 5
Intro to Example Antenna Types - Lesson 1
Просмотров 4,7 тыс.3 года назад
Intro to Example Antenna Types - Lesson 1
Example Antenna Types - Course Overview
Просмотров 1,1 тыс.3 года назад
Example Antenna Types - Course Overview
thank you
Wow 😍amazingly explained Thank you
Greetings! I am an engineering manager at a major company running an RF group. My company is paying for me to do my second master's degree at Johns Hopkins online (I am on the west coast). I will be 60 in 2025 but do not want to stop learning. That said, I am taking a course at JHU in computational electromagnetics and on my final project we are implementing a simple telegrapher's equation in finite difference. This does not mean it's easy. PS: My first master's degree is in music - organ performance and sacred music from the Jacobs School of Music at Indiana University Bloomington. Thank you for these helpful videos!
Now it makes sense when you brought up Helmholtz theorem.... Thanks
Very nice 👍😊 I am from India nice clerifa tions
All of your videos are excellent. I don't know if you are listening still to replies, and I hate to impose if you are, but a fascinating question I have been trying to answer is that the length to diameter of a dipole antenna determines its bandwidth, and adding d with a fixed l increases the bandwidth while decreasing its resonant frequency. Do you know why this is? I have done many searches and found nothing, except that increasing d reduces the inductance, which contradicts the lowering of the resonant frequency, unless fringe fields counteract the reduction in inductance. Thank you, whether you see this or not. Edited to add: I found the answer in ARRL Handbook on page 20.3. “If the diameter of the conductor is increased, the capacitance per unit length increases and the inductance per unit length decreases. Since the radiation resistance is affected relatively little, the decreased L/C ratio causes the Q of the antenna to decrease so that the resonance curve becomes less sharp with change in frequency. This effect is greater as the diameter is increased, and is a property of some importance at the very high frequencies where the wavelength is small.”
best!
THANK YOU!
patch antenna was my final year project in 2010 at Houari Boumedien University in Algeria (Modeling of a patch antenna network using the iterative method)
Good 👍
Good 👍
Extremely oraganised and simple. Straight to the point. Thanks for posting
Thank you.
thank you
so beautiful so amazing crystal clear🎉🎉🎉🎉❤❤❤❤
Great video! I have one question: Since we matched Z0 and Zin, what about Z1 and Zload? I mean we secured no reflections at the beginning of the quarter wave transformer but did we secure no reflections between the quarter wave transformer and the antenna?
huh
2:19 - H field should be pointing either in +x or -x direction, right? (+ or - x directions are not defined in the shown example, that's why I am saying +x or -x, depending on the right-handed rule) So equation should be with a hat x and a hat x.
Hi, I would like to ask why do we bother to create the concept of A which in the end is a formula related to the current and then we take the curl of it to get B, when we can use Ampere's Law which is the curl of B = mu0*J in statics and vacuum? If we want the vector B, can't we just use integration on the curl of B instead of doing the Magnetic Vector Potential approach?
please what is the radius of the second circle you draw to to have the intersection
Hi professor, thank u. But I have a question. Why didn't you consider dD/dt for ampere's law
wow, that's so useful, love it
Hey there, does ZL means the Impedance or the Admittance? Thanks.
@@Meltonsix Hi! In general, Z is used to symbolize impedance, while Y is used for admittance.
Thank you so much!!!! I admire you and your lecture
wow these lectures are insanely good
White Karen Hernandez Betty Thomas Brenda
I would move to the awful state of NC to continue with my Ph.D. if I could learn from her! Throughout my entire BSEE and MSEE curriculums and 6 years in the RF Engineering industry, never have I ever met anyone who could explain these topics as clearly as she does. If these playlists existed back when I first began my graduate coursework with an emphasis in applied EM and antenna theory and design, I’d of progressed significantly faster. If you’re studying RF/Microwave Engineering and you’re NOT watching her videos, you’re either unaware they exist, or a glutton for punishment doomed to exist in complex exponential HELL as a means to make sense of antenna design through abstract mathematics (as is the conventional method) given what I believe to be a lack of professors with her level of comprehension in academia.
this was really helpful, thanks
Thank you very much.
Thanks a lot Doc
❤
Well in the Poisson equation for A we have a scalar on the left by definition,but a vector of J on the right,how come?
The animation on 1:14 is very confusing. When I point the thumb of my right hand in the direction of the X-axis (arrow, top left of the monitor), my right-hand fingers do not curl in the direction of rotation as shown. They curl in the clockwise direction and not the anti-clockwise direction.
Thank you so much!! Thanks to you I finally understand this material :)
If you wanna understand the imaginary numbers, the complex plane and the Euler's formula, read the book "Engineering mathematics" by Steinmetz where he brilliantly explains all this stuff from the ground up
High quality content. Thanks!
0:57,Hr is having gamma in power , how(gamma with k)?
can you please clarify the expansion in 0:22 . in Hr term ' - ' was missing and also e^+jkr. Please help me out
Directors should connected with each other?
no, directors and the reflector are straight conductive elements that aren't connected electrically to anything. the dipole should be split down the center, but not the others.
Very helpful videos!
Ohm's law always apply, even before reaching the load, ohm's law applies to the local instantaneous impedance seen, the characteristic impedance!
Thank you❤
Makes so much more sense when you condense pages of math identities into a few sentences. Like I don’t really need to reinvent the wheel, final solution is what matters and the basic set up
Thanks
Thank u sir
Thank you for your brief and clear explanation
These are great videos. Very clearly presented and everything is derived from first principles. I'm not sure why they don't have more views. Thanks
As you explain it is to describe LTI systems but we use this notation in time harmonic quantity, With the time harmonic quantity how phasor makes assumptions, pls explain
Mum help, am about to run mad
@ 3:29 So the yellow line on the circle is an area of the sphere! Hmm, why do I keep staring at these three buttons?