Doug Tougaw
Doug Tougaw
  • Видео 245
  • Просмотров 851 513

Видео

Valpo College of Engineering Short Tour Vertical
Просмотров 1143 года назад
A fly-though tour of the Valparaiso University College of Engineering laboratory facilities.
Valpo College of Engineering Full Tour Horizontal
Просмотров 3813 года назад
A fly-though tour of the Valparaiso University College of Engineering laboratory facilities.
Valpo College of Engineering Full Tour Vertical
Просмотров 1123 года назад
A fly-through tour of Valparaiso University's College of Engineering.
Applied Electromagnetic Field Theory Chapter 32 -- Antenna Arrays
Просмотров 3,2 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 32 Antenna Arrays
Applied Electromagnetic Field Theory Four-Element Isotropic Phased Array with Phase Difference
Просмотров 6376 лет назад
Applied Electromagnetic Field Theory Four-Element Isotropic Phased Array with Phase Difference
Applied Electromagnetic Field Theory Four-Element Dipole Phased Array
Просмотров 6096 лет назад
Applied Electromagnetic Field Theory Four-Element Dipole Phased Array
Applied Electromagnetic Field Theory Two-element Dipole Phased Array
Просмотров 1,2 тыс.6 лет назад
Applied Electromagnetic Field Theory Two-element Dipole Phased Array
Applied Electromagnetic Field Theory Two-element Isotopic Phased Array
Просмотров 1,3 тыс.6 лет назад
Applied Electromagnetic Field Theory Two-element Isotopic Phased Array
Applied Electromagnetic Field Theory Chapter 31--Antenna Parameters
Просмотров 1,3 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 31 Antenna Parameters
Applied Electromagnetic Field Theory Chapter 14 -- Magnetic Materials and Magnetic Circuits
Просмотров 2,5 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 14 Magnetic Materials and Magnetic Circuits
Applied Electromagnetic Field Theory Chapter 11-- Magnetic Fields
Просмотров 2,8 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 11 Magnetic Fields
Applied Electromagnetic Field Theory Chapter 30 -- Finite Dipole Antennas and Loop Antennas
Просмотров 28 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 30 Finite Dipole Antennas and Loop Antennas
Applied Electromagnetic Field Theory -- Finite Dipole Radiation Pattern
Просмотров 6346 лет назад
Applied Electromagnetic Field Theory Finite Dipole Radiation Pattern
Applied Electromagnetic Field Theory Chapter 29 -- Electromagnetic Radiation and Infinitesimal Dipol
Просмотров 1,9 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 29 Electromagnetic Radiation and Infinitesimal Dipol
Applied Electromagnetic Field Theory Chapter 28 -- Lossy Transmission Lines and Dispersion
Просмотров 1,6 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 28 Lossy Transmission Lines and Dispersion
Applied Electromagnetic Field Theory -- Dispersion and Group Velocity
Просмотров 6126 лет назад
Applied Electromagnetic Field Theory Dispersion and Group Velocity
Applied Electromagnetic Field Theory Chapter 27 -- Transient Effects and Bounce Diagrams
Просмотров 1,8 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 27 Transient Effects and Bounce Diagrams
Applied Electromagnetic Field Theory Chapter 3--Coulomb's Law
Просмотров 5446 лет назад
Applied Electromagnetic Field Theory Chapter 3 Coulomb's Law
Applied Electromagnetic Field Theory Chapter 26 -- Smith Charts
Просмотров 1,1 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 26 Smith Charts
Applied Electromagnetic Field Theory Chapter 25 -- Impedance Matching
Просмотров 1,1 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 25 Impedance Matching
Applied Electromagnetic Field Theory Chapter 24 -- Terminations and Reflections
Просмотров 1 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 24 Terminations and Reflections
Applied Electromagnetic Field Theory Chapter 23--Transmission Lines
Просмотров 3,2 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 23 Transmission Lines
Applied Electromagnetic Field Theory Chapter 22--Bounce Diagrams and Standing Waves
Просмотров 1,7 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 22 Bounce Diagrams and Standing Waves
Applied Electromagnetic Field Theory Chapter 21 -- Reflection and Transmission of Electromagnetic Wa
Просмотров 1,2 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 21 Reflection and Transmission of Electromagnetic Wa
Applied Electromagnetic Field Theory Chapter 20 -- Plane Wave Propagation in a Dielectric
Просмотров 1,9 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 20 Plane Wave Propagation in a Dielectric
Applied Electromagnetic Field Theory Chapter 3--Coulomb's Law
Просмотров 4,6 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 3 Coulomb's Law
Applied Electromagnetic Field Theory Chapter 1--Vectors and Vector Arithmetic
Просмотров 14 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 1 Vectors and Vector Arithmetic
Applied Electromagnetic Field Theory Chapter 19 -- Plane Wave Propagation in Free Space
Просмотров 2,9 тыс.6 лет назад
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
Просмотров 2,8 тыс.6 лет назад
Applied Electromagnetic Field Theory Chapter 18 Poynting's Theorem and the Wave Equation

Комментарии

  • @subeersulub
    @subeersulub 10 часов назад

    bravo

  • @Chutkiji69
    @Chutkiji69 13 дней назад

    Wow❤

  • @gamehub2904
    @gamehub2904 Месяц назад

    Thanks sir 🙏🏻

  • @AK47_414
    @AK47_414 Месяц назад

    Amazing teaching. Helping me in 2024. Thanks

  • @bananafish9105
    @bananafish9105 Месяц назад

    Solve Y = (A'+ B'C')' A'

  • @kazuarcus7847
    @kazuarcus7847 Месяц назад

    Thank you! Very Helpful

  • @MrThePhotoshopper
    @MrThePhotoshopper 2 месяца назад

    Mr T, why didn't you group 1 3 9 11 in 1 group?

  • @CHR1ST1AN444
    @CHR1ST1AN444 2 месяца назад

    This was a great explanation.

  • @BenBuchane
    @BenBuchane 2 месяца назад

    The lord sent me here , thank you sir . Could you please share what textbook you use , im currently taking fundamentals of electrical engineering

    • @dougtougaw7681
      @dougtougaw7681 2 месяца назад

      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!

  • @shenakatesencil6732
    @shenakatesencil6732 3 месяца назад

    great explanation : ))

  • @YungNaysen
    @YungNaysen 3 месяца назад

    thanks from france lol

  • @JamesHlanguyo
    @JamesHlanguyo 3 месяца назад

    This is 5star explanation🔥

  • @IshaNegi18
    @IshaNegi18 3 месяца назад

    Helpful

  • @kamyabratadebnath9389
    @kamyabratadebnath9389 3 месяца назад

    Thank you sir , you projected the theorem very well , All my confusions are gone

  • @NabumboFarida
    @NabumboFarida 3 месяца назад

    in you I found a solution. thanks a lot for the great work please!!!

  • @johnpaulrayco1366
    @johnpaulrayco1366 3 месяца назад

    this is awesome

  • @quantumradio
    @quantumradio 4 месяца назад

    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).

  • @baghdadiabdellatif1581
    @baghdadiabdellatif1581 5 месяцев назад

    Thank you so much. Greetings from north Africa (Algerian desert)

  • @igorrocha1845
    @igorrocha1845 5 месяцев назад

    Loved the tour. Valparaiso is a dream of a college! 😁

  • @igorrocha1845
    @igorrocha1845 5 месяцев назад

    Thanks for this class, really helping me ❤

  • @igorrocha1845
    @igorrocha1845 5 месяцев назад

    Again, thanks for this series of videos! :)

  • @igorrocha1845
    @igorrocha1845 5 месяцев назад

    Thanks so much for posting these videos 🙏

  • @baghdadiabdellatif1581
    @baghdadiabdellatif1581 5 месяцев назад

    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

  • @Devi--Devi
    @Devi--Devi 6 месяцев назад

    What happened to C? HELP I DON'T UNDERSTAND

  • @jacobvandijk6525
    @jacobvandijk6525 6 месяцев назад

    @ 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.

  • @jacobvandijk6525
    @jacobvandijk6525 6 месяцев назад

    @ 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.

  • @ahmetsasa5644
    @ahmetsasa5644 6 месяцев назад

    Thanks for everything

  • @r3dx936
    @r3dx936 7 месяцев назад

    ESE MAQUINA

  • @RoyBolinggoing
    @RoyBolinggoing 7 месяцев назад

    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.

    • @RoyBolinggoing
      @RoyBolinggoing 7 месяцев назад

      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: ruclips.net/video/dg_O_bJO9zo/видео.html

  • @h7opolo
    @h7opolo 7 месяцев назад

    32:02 great animation, sir tougaw 47:49 another sweet animation of the Yagi-Uda transmission antenna

  • @h7opolo
    @h7opolo 7 месяцев назад

    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".

  • @mariasultana4615
    @mariasultana4615 7 месяцев назад

    𝐆𝐫𝐞𝐚𝐭

  • @pierregiuseppegilles9135
    @pierregiuseppegilles9135 7 месяцев назад

    Shouldn't A+(B•C) be (A+B)•(A+C)?

  • @LyleH-13
    @LyleH-13 7 месяцев назад

    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.

    • @dougtougaw7681
      @dougtougaw7681 7 месяцев назад

      Glad it's helpful! Good luck with your course.

  • @OceanDreams-xs1ii
    @OceanDreams-xs1ii 8 месяцев назад

    shouldn't I2 equal to Ix in the second example since they are in the same loop ?

  • @nathaniell.1886
    @nathaniell.1886 8 месяцев назад

    I was following aong until you got rid of the C in the second equation.

  • @AichatouOmor
    @AichatouOmor 8 месяцев назад

    Yes

  • @ameeryasen7107
    @ameeryasen7107 8 месяцев назад

    thanks

  • @sciekoszczur
    @sciekoszczur 9 месяцев назад

    thank you so so much

  • @johannes.50
    @johannes.50 9 месяцев назад

    There's a rule that says voltage is same in parallel circuits🙂

  • @divyatandon2389
    @divyatandon2389 9 месяцев назад

    What About AD

  • @donorofeverything9641
    @donorofeverything9641 9 месяцев назад

    Thanks

  • @TacoDaddy-mr8ig
    @TacoDaddy-mr8ig 10 месяцев назад

    Nice video

  • @TacoDaddy-mr8ig
    @TacoDaddy-mr8ig 10 месяцев назад

    This was a useless video

  • @amirkard
    @amirkard 10 месяцев назад

    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.

  • @noor-ul-islamkashif7070
    @noor-ul-islamkashif7070 10 месяцев назад

    Hey can someone please tell me where and how I can access the notes?

    • @Info-MZ24h
      @Info-MZ24h 8 месяцев назад

      me as well i need please help us with this🙄

    • @LyleH-13
      @LyleH-13 7 месяцев назад

      Im assuming you had to have access to this guys college course to get that.

  • @lechip3765
    @lechip3765 10 месяцев назад

    I love this

  • @thechrisricci
    @thechrisricci 10 месяцев назад

    Thanks!

  • @innovbrain
    @innovbrain 11 месяцев назад

    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

  • @jakeday5224
    @jakeday5224 11 месяцев назад

    i struggled so much with topic and i learned more from this 5 minute video than two years of studying computer science