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เข้าร่วมเมื่อ 24 ก.พ. 2020
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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// STAY IN THE LOOP
Follow our Ansys Academic LinkedIn showcase page for updates on learning resources, events, job opportunities, cutting-edge simulation content and more!
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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.ly/32eEcuR
// QUESTIONS ABOUT THIS VIDEO OR USING ANSYS?
Get help from Ansys experts and peers through the Ansys Learning Forum. Search for answers to common questions, browse discussion categories or ask your own question.
Visit today → bit.ly/3qsytK2
// STAY IN THE LOOP
Follow our Ansys Academic LinkedIn showcase page for updates on learning resources, events, job opportunities, cutting-edge simulation content and more!
Follow today → bit.ly/3Bbaaow
มุมมอง: 5 247
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Calculating S-Parameters - Lesson 3
มุมมอง 28K2 ปีที่แล้ว
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
มุมมอง 14K2 ปีที่แล้ว
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
มุมมอง 13K2 ปีที่แล้ว
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
มุมมอง 5K2 ปีที่แล้ว
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
มุมมอง 3.1K2 ปีที่แล้ว
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
มุมมอง 2.3K2 ปีที่แล้ว
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
มุมมอง 5K3 ปีที่แล้ว
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
มุมมอง 12K3 ปีที่แล้ว
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
มุมมอง 3.9K3 ปีที่แล้ว
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
มุมมอง 8K3 ปีที่แล้ว
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
มุมมอง 10K3 ปีที่แล้ว
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
มุมมอง 12K3 ปีที่แล้ว
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
มุมมอง 12K3 ปีที่แล้ว
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
มุมมอง 4.3K3 ปีที่แล้ว
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
มุมมอง 6K3 ปีที่แล้ว
Dipole Input Impedance Over Frequency - Lesson 2
Intro to Frequency Characteristics of The Half-Wave Dipole - Lesson 1
มุมมอง 3.5K3 ปีที่แล้ว
Intro to Frequency Characteristics of The Half-Wave Dipole - Lesson 1
The Theoretical Radiation Pattern of a Half-wave Dipole - Lesson 3
มุมมอง 13K3 ปีที่แล้ว
The Theoretical Radiation Pattern of a Half-wave Dipole - Lesson 3
The Current Structure on a Half-wave Dipole - Lesson 2
มุมมอง 20K3 ปีที่แล้ว
The Current Structure on a Half-wave Dipole - Lesson 2
Intro to Design of the Half-wave Dipole - Lesson 1
มุมมอง 6K3 ปีที่แล้ว
Intro to Design of the Half-wave Dipole - Lesson 1
Design of the Half-Wave Dipole - Overview
มุมมอง 8813 ปีที่แล้ว
Design of the Half-Wave Dipole - Overview
The Cylindrical Coordinate System - Lesson 8
มุมมอง 3.2K3 ปีที่แล้ว
The Cylindrical Coordinate System - Lesson 8
The Rectangular Patch Antenna - Lesson 5
มุมมอง 27K3 ปีที่แล้ว
The Rectangular Patch Antenna - Lesson 5
Intro to Example Antenna Types - Lesson 1
มุมมอง 4.9K3 ปีที่แล้ว
Intro to Example Antenna Types - Lesson 1
Example Antenna Types - Course Overview
มุมมอง 1.2K3 ปีที่แล้ว
Example Antenna Types - Course Overview
Very concise explanation. What a great video, thank you a lot. from an undergrad studying finals
evliymişşin yaaa , gene de seviyorum
Hello Kathryn I would like to ask if it would be feasible and at all beneficial to have multiple Yagi antennas all equally tuned and at the same hight but in a circular array. For example having six Yagi antennas forming a star pattern so as to push the +dB signal out in more of a wabbley circular pattern (Non collinear). Thank you kindly for sharing your knowledge
This is FANTASTIC !
Thanks!!!
In my understanding T=(Zo-Zin)/(Zo+Zin) Or am I wrong?
You are so smart ... My wish to love you
Tq❤
Perfect
Beautifully developed concept of the Lorenz gauge especially. I'm surprised you so readily dismissed the vector potential as a purely mathematical artifact rather than as something pertaining to a physical reality. There is an argument for the reality of the vector potential based on quantum phenomena such as the Aharonov-Bohm effect. Although he termed it as the electro-tonic function (i.e. Faraday's electro-tonic state), Maxwell was clearly convinced of its physical significance with respect to electromagnetic induction. He seemed to prefer its relevance in that situation over the commonly agreed causal relationship between flux linking and electromagnetic induction.
Superb ❤
She is good !
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.
Speaking as a retired RF Systems engineer, I agree 100 % with your assessment of her teaching abilities
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