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Doug Tougaw
Приєднався 21 сер 2012
Valpo College of Engineering Short Tour Horizontal
A fly-though tour of the Valparaiso University College of Engineering laboratory facilities.
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Відео
Valpo College of Engineering Short Tour Vertical
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A fly-though tour of the Valparaiso University College of Engineering laboratory facilities.
Valpo College of Engineering Full Tour Horizontal
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A fly-though tour of the Valparaiso University College of Engineering laboratory facilities.
Valpo College of Engineering Full Tour Vertical
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A fly-through tour of Valparaiso University's College of Engineering.
Applied Electromagnetic Field Theory Chapter 32 -- Antenna Arrays
Переглядів 3,2 тис.6 років тому
Applied Electromagnetic Field Theory Chapter 32 Antenna Arrays
Applied Electromagnetic Field Theory Four-Element Isotropic Phased Array with Phase Difference
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Applied Electromagnetic Field Theory Four-Element Isotropic Phased Array with Phase Difference
Applied Electromagnetic Field Theory Four-Element Dipole Phased Array
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Applied Electromagnetic Field Theory Four-Element Dipole Phased Array
Applied Electromagnetic Field Theory Two-element Dipole Phased Array
Переглядів 1,2 тис.6 років тому
Applied Electromagnetic Field Theory Two-element Dipole Phased Array
Applied Electromagnetic Field Theory Two-element Isotopic Phased Array
Переглядів 1,3 тис.6 років тому
Applied Electromagnetic Field Theory Two-element Isotopic Phased Array
Applied Electromagnetic Field Theory Chapter 31--Antenna Parameters
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Applied Electromagnetic Field Theory Chapter 31 Antenna Parameters
Applied Electromagnetic Field Theory Chapter 14 -- Magnetic Materials and Magnetic Circuits
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Applied Electromagnetic Field Theory Chapter 14 Magnetic Materials and Magnetic Circuits
Applied Electromagnetic Field Theory Chapter 11-- Magnetic Fields
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Applied Electromagnetic Field Theory Chapter 11 Magnetic Fields
Applied Electromagnetic Field Theory Chapter 30 -- Finite Dipole Antennas and Loop Antennas
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Applied Electromagnetic Field Theory Chapter 30 Finite Dipole Antennas and Loop Antennas
Applied Electromagnetic Field Theory -- Finite Dipole Radiation Pattern
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Applied Electromagnetic Field Theory Finite Dipole Radiation Pattern
Applied Electromagnetic Field Theory Chapter 29 -- Electromagnetic Radiation and Infinitesimal Dipol
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Applied Electromagnetic Field Theory Chapter 29 Electromagnetic Radiation and Infinitesimal Dipol
Applied Electromagnetic Field Theory Chapter 28 -- Lossy Transmission Lines and Dispersion
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Applied Electromagnetic Field Theory Chapter 28 Lossy Transmission Lines and Dispersion
Applied Electromagnetic Field Theory -- Dispersion and Group Velocity
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Applied Electromagnetic Field Theory Dispersion and Group Velocity
Applied Electromagnetic Field Theory Chapter 27 -- Transient Effects and Bounce Diagrams
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Applied Electromagnetic Field Theory Chapter 27 Transient Effects and Bounce Diagrams
Applied Electromagnetic Field Theory Chapter 3--Coulomb's Law
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Applied Electromagnetic Field Theory Chapter 3 Coulomb's Law
Applied Electromagnetic Field Theory Chapter 26 -- Smith Charts
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Applied Electromagnetic Field Theory Chapter 26 Smith Charts
Applied Electromagnetic Field Theory Chapter 25 -- Impedance Matching
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Applied Electromagnetic Field Theory Chapter 25 Impedance Matching
Applied Electromagnetic Field Theory Chapter 24 -- Terminations and Reflections
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Applied Electromagnetic Field Theory Chapter 24 Terminations and Reflections
Applied Electromagnetic Field Theory Chapter 23--Transmission Lines
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Applied Electromagnetic Field Theory Chapter 23 Transmission Lines
Applied Electromagnetic Field Theory Chapter 22--Bounce Diagrams and Standing Waves
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Applied Electromagnetic Field Theory Chapter 22 Bounce Diagrams and Standing Waves
Applied Electromagnetic Field Theory Chapter 21 -- Reflection and Transmission of Electromagnetic Wa
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Applied Electromagnetic Field Theory Chapter 21 Reflection and Transmission of Electromagnetic Wa
Applied Electromagnetic Field Theory Chapter 20 -- Plane Wave Propagation in a Dielectric
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Applied Electromagnetic Field Theory Chapter 20 Plane Wave Propagation in a Dielectric
Applied Electromagnetic Field Theory Chapter 3--Coulomb's Law
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Applied Electromagnetic Field Theory Chapter 3 Coulomb's Law
Applied Electromagnetic Field Theory Chapter 1--Vectors and Vector Arithmetic
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Applied Electromagnetic Field Theory Chapter 1 Vectors and Vector Arithmetic
Applied Electromagnetic Field Theory Chapter 19 -- Plane Wave Propagation in Free Space
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Applied Electromagnetic Field Theory Chapter 19 Plane Wave Propagation in Free Space
Applied Electromagnetic Field Theory Chapter 18 -- Poynting's Theorem and the Wave Equation
Переглядів 2,8 тис.6 років тому
Applied Electromagnetic Field Theory Chapter 18 Poynting's Theorem and the Wave Equation
Wow❤
Thanks sir 🙏🏻
Amazing teaching. Helping me in 2024. Thanks
Solve Y = (A'+ B'C')' A'
Thank you! Very Helpful
Mr T, why didn't you group 1 3 9 11 in 1 group?
This was a great explanation.
The lord sent me here , thank you sir . Could you please share what textbook you use , im currently taking fundamentals of electrical engineering
I'm so glad I could help. I used these notes as a textbook of their own, and I didn't have another textbook for my course. However, there is a playlist of 80 videos in this series that may be helpful to you. Good luck!
great explanation : ))
thanks from france lol
This is 5star explanation🔥
Helpful
Thank you sir , you projected the theorem very well , All my confusions are gone
in you I found a solution. thanks a lot for the great work please!!!
this is awesome
The way i understand it at 27:19 is that Professor Tougaw is taking the magnitude of E to be Etheta times the complex conjugate of Etheta and then taking the squre root: |E| = [(E)*(E*)]ˆ1/2. This is the definition of the magnitude of a vector and this vector E has only one component along the theta direction. When you take the complex conjugate you change i wherever it appears to -i (or j -> -j for electrical engineers).
Thank you so much. Greetings from north Africa (Algerian desert)
Loved the tour. Valparaiso is a dream of a college! 😁
Thanks for this class, really helping me ❤
Again, thanks for this series of videos! :)
Thanks so much for posting these videos 🙏
At example 17.1 at 12:20 it take the charge to dissipate to 10% of its initial value 3.4 * 10 ^ - 19 sec And before that, you calculate that it take the charge to dissipate to 0% of its initial value 0.47 * 10 ^ - 19 sec! This means that it takes more time to dissipate to 10% than to dissipate to 0%! Isn't this a contradiction? It should takes less time to dissipate to 10% than to dissipate to ≈ 0%. Thank you for your efforts in creating this content This is my calculations For ≈ 0% , t= 7.375 × 10^-19 sec t= 5τ For 1% , t= 6.8 × 10^-19 sec For 10% , t= 3.4 × 10^-19 sec For 36.8% , t= τ = 0.47 * 10 ^-19 sec
What happened to C? HELP I DON'T UNDERSTAND
@ 13:52 The field lines of a charged particle moving at constant velocity (incl. v = 0) do not propagate or radiate. There is only radiation during the acceleration of a charged particle. Therefore, during the period t (>>> the period of acceleration dt) there can't be radiation all the time. Read this paragraph: @ 15:10. I don't see why the period t can't be equal to dt? The outcome is the same. But if I'm wrong in this, please correct me.
@ 6:38 In fact, dS = r-hat. dA, with r-hat being the dimensionless unit-vector pointing in the radial direction of the Poynting-vector. The dot-product (in eq. 29.1) is between the Poynting-vector S and this unit-vector, resulting in | S | . | r-hat | . cos(a) = | E | . | H | . cos(a), with 'a' being the angle between the E- and the H-vector; and remember that the length of r-hat = 1. The E- and H-vector are orthogonal and thus, sin(a) = 1. The result of a dot-product is a scalar, that we can take out of the integral. Then, in eq. 29.2 the surface-area A = integral of dA.
Thanks for everything
ESE MAQUINA
Thanks for this series. I have been watching them all. I am just wondering why in the final example squares 7 and 15 are not combined with square 3 to make a line of squares 3,7 and 15. I thought doubling up was right a 'proper' thing to do.
I worked out now the mistake I made in not fully comprehending the rules in this earlier video of yours. I will leave all my ramblings and this link in case it helps another student: ua-cam.com/video/dg_O_bJO9zo/v-deo.html
32:02 great animation, sir tougaw 47:49 another sweet animation of the Yagi-Uda transmission antenna
3:42 correction: the voltages are the same magnitude, just opposite polarities, so it's not quite accurate to describe the dipole ends as "high or low".
𝐆𝐫𝐞𝐚𝐭
Shouldn't A+(B•C) be (A+B)•(A+C)?
So far this playlist seems great for what I need. I took Physics 2 in 2019, but then the pandemic hit and I have 3 kids so my school progress was halted. Now in 2024 im taking Principles of Electrical Engineering as a mechanical engineering student who needs it to prereq into Vibration Analysis in the fall. Im way behind the ball now, and i had a harsh reality check in the first week. Thank you. A lot of the other videos dont seem to be what I need, or have either way too much, or not enough.
Glad it's helpful! Good luck with your course.
shouldn't I2 equal to Ix in the second example since they are in the same loop ?
I was following aong until you got rid of the C in the second equation.
Yes
thanks
thank you so so much
There's a rule that says voltage is same in parallel circuits🙂
What About AD
Thanks
Nice video
This was a useless video
You made two mistakes when solving Ex. 7.3. First of all when you say Vab and you are setting the integral limits from a to b (1 to 3) it means that you are moving in the +ar direction not negative. Second, the integral of 1/r^2 is minus 1/r, not plus.
Hey can someone please tell me where and how I can access the notes?
me as well i need please help us with this🙄
Im assuming you had to have access to this guys college course to get that.
I love this
Thanks!
Sir let me explain something kindly, since we are following the clockwise loop in the circuit, the voltage source on the left is positive since it's following the clockwise from negative to positive, then the 2ohms resistor is a drop voltage from positive to negative not the opposite, becauseit'sa voltage drop from the battery clockwise. The 2A current source is going counter clockwise so it's negative too. So it's +V1-V2-V3=0. I checked it out in my electrical circuits book
I was confused by that part c
i struggled so much with topic and i learned more from this 5 minute video than two years of studying computer science
fantastic