![Randall Manteufel](/img/default-banner.jpg)
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Randall Manteufel
Registrace 18. 01. 2013
Videos to help students learn engineering statics, thermodynamics, fluid mechanics and heat transfer. Based on EGR 2103 Statics, ME 3293 Thermodynamics I, ME 3663 Fluid Mechanics, ME 4313 Heat Transfer, and ME 4293 Thermodynamics II.
I don't have time to answer all of the questions submitted. I hope you understand. Thanks.
Thermodynamics textbook: M.J. Moran, H.N. Shapiro, D.D. Boettner, M.B. Bailey, Fundamentals of Engineering Thermodynamics, 7th Edition, Wiley, 2011.
Fluids mechanics textbook: Y.A. Cengel and J.M. Cimbala, Fluid Mechanics: Fundamentals and Applications, 2nd edition, McGraw-Hill, 2010.
Heat transfer textbook: Bergman, T.L., Lavine, A.S. Incropera, F.P., and DeWitt D.P., Introduction to Heat Transfer, 6th edition, Wiley. 8th edition Heat and Mass Transfer in Fall 2018.
Statics textbook: Hibbeler, R.C., Engineering Mechanics, Statics, Fourteenth Edition, Pearson Prentice Hall, 2016.
I don't have time to answer all of the questions submitted. I hope you understand. Thanks.
Thermodynamics textbook: M.J. Moran, H.N. Shapiro, D.D. Boettner, M.B. Bailey, Fundamentals of Engineering Thermodynamics, 7th Edition, Wiley, 2011.
Fluids mechanics textbook: Y.A. Cengel and J.M. Cimbala, Fluid Mechanics: Fundamentals and Applications, 2nd edition, McGraw-Hill, 2010.
Heat transfer textbook: Bergman, T.L., Lavine, A.S. Incropera, F.P., and DeWitt D.P., Introduction to Heat Transfer, 6th edition, Wiley. 8th edition Heat and Mass Transfer in Fall 2018.
Statics textbook: Hibbeler, R.C., Engineering Mechanics, Statics, Fourteenth Edition, Pearson Prentice Hall, 2016.
Combustion 150percent methane with air given Ti and Te calc Tdew Qdot
Thermodynamics II
zhlédnutí: 2 971
Video
me4293 ideal gas mixture expands isentropically in turbine iteration to calc T2 Wdot
zhlédnutí 1,5KPřed 3 lety
Thermodynamics II
me4293 Evaporative cooling unit with heater and then soaked liquid pad
zhlédnutí 859Před 3 lety
Thermodynamics II
me3293 Water dam electric generator calc value of electricity produced per day2
zhlédnutí 668Před 3 lety
Thermodynamics I
me3293 air compressor use air table or const cp to calc T2min T2act W Sgen
zhlédnutí 680Před 3 lety
Thermodynamics I
me4293 ideal gas mixture expands isentropically in turbine iterate to calc T2 Wdot
zhlédnutí 840Před 3 lety
Thermodynamics I
me3293 air flow in nozzle calc T2 and isentropic efficiency
zhlédnutí 1,8KPřed 3 lety
Thermodynamics I
me3293 CO2 expands adiabatically and reversibly in turbine calc T2 and w
zhlédnutí 501Před 3 lety
Thermodynamics I
me3293 steam turbine with isentropic efficiency calc exit quality and power
zhlédnutí 3,5KPřed 3 lety
Thermodynamics I
me3293 isentropic compression of steam in piston cylinder calc T2 and W12
zhlédnutí 1,2KPřed 3 lety
me3293 isentropic compression of steam in piston cylinder calc T2 and W12
me3293 air heated and stirred in rigid tank calc S_transfer and S_gen
zhlédnutí 627Před 3 lety
me3293 air heated and stirred in rigid tank calc S_transfer and S_gen
me4293 heat exchanger pinch analysis R134a condenser
zhlédnutí 4,1KPřed 3 lety
me4293 heat exchanger pinch analysis R134a condenser
me4293 geothermal heat pump with R134a and exergy calcs
zhlédnutí 4KPřed 3 lety
me4293 geothermal heat pump with R134a and exergy calcs
me4293 Refrigeration polytropic compressor and water cooled condenser with exergy calc
zhlédnutí 1,2KPřed 3 lety
me4293 Refrigeration polytropic compressor and water cooled condenser with exergy calc
me4293 vapor compression refrigeration with exergy calcs
zhlédnutí 3,4KPřed 3 lety
me4293 vapor compression refrigeration with exergy calcs
me4293 R134a evaporator superheat condenser subcool
zhlédnutí 1,2KPřed 3 lety
me4293 R134a evaporator superheat condenser subcool
me3293 Calc Qdot Tb and Sgen for electric generator
zhlédnutí 426Před 3 lety
me3293 Calc Qdot Tb and Sgen for electric generator
me3293 R134a Q and Sgen for expansion process
zhlédnutí 222Před 3 lety
me3293 R134a Q and Sgen for expansion process
me3293 entropy change of oxygen with const cp or var cp
zhlédnutí 353Před 3 lety
me3293 entropy change of oxygen with const cp or var cp
me3293 nitrogen gas polytropic process calc Q and entropy change
zhlédnutí 598Před 3 lety
me3293 nitrogen gas polytropic process calc Q and entropy change
me3293 Clausius inequality for abstract power plant calc eff th
zhlédnutí 228Před 3 lety
me3293 Clausius inequality for abstract power plant calc eff th
Clausius inequality for vapor power plant eff th and Sgen cycle
zhlédnutí 398Před 3 lety
Clausius inequality for vapor power plant eff th and Sgen cycle
me3293 Carnot power cycle with air in piston cylinder assembly
zhlédnutí 3KPřed 3 lety
me3293 Carnot power cycle with air in piston cylinder assembly
me3293 mixing tank 3 inlet and 1 outlet stream
zhlédnutí 504Před 3 lety
me3293 mixing tank 3 inlet and 1 outlet stream
Hello, Ive been confused sometimes about the feedwater exits. Is its enthalpy always equal to the sat. Liq of the extracted steam? When using the pump method, i noticed it is not, assuming the given state when both extracted and feedwater mixed
Great video Dr. Mantufel! Thank you!
I have written out the solution myself, but when I tried to post the Drive link here CZcams keeps shadowbanning this comment. For now I will just leave my explanation of how I got equation of the line and how to express r as a function of Z. The part about getting r(z) might confuse some people. It certainly confused me at first. I did not use the method explained in this video. My approach was slightly different. What I had done as seen on my solution, is that I drew a 2D projection view of the Y and Z axes as shown in the question's diagram. The outer edge of the cone (highlighted in green on my solution) was considered to be a line within the set coordinate system and the equation for this line was determined. We can see that the green line is going down (as you go from left to right) therefore its gradient is negative. We can also see that the line intercepts the vertical axis (in this case the Z axis) at h, therefore the y-intercept is h. It intercepts the horizontal axis at "a" and therefore the gradient of the line can be determined. It is rise over run and since we know that the lengths of "h" and "a" are the "rise" and the "run" respectively, the gradient of the line is -h/a. The full equation of the line is Z=-h/a*y+h The trick now is understanding that Z is our variable that we need to integrate with respect to, as our infinitesimal element has a dZ in it. That immediately gives us a clue that we have to somehow somewhere integrate with respect to Z. We also need to be cognizant of the fact that the quantity "r" which is the radius of the infinitesimal element, is a CHANGING quantity. It's not a constant as the infinitesimal element (the small quarter cone slice indicated on the diagram) can be placed anywhere in the whole quarter cone so the r value can be higher or lower. This tells us that "r" is a VARIABLE and therefore we cannot treat it as a constant (generally you can pull constants outside the integral when solving but you can never do that with variables). We will have to integrate with respect to "r" either directly or indirectly. As previously mentioned, we have a dZ as our infinitesimal element's height, so immediately this tells us that we have to find some way to represent the quantity r as a function of Z. Once we do that, the hardest part of the problem is solved. If you look at the 2D sketch I drew, "r" in that 2D sketch would essentially be horizontal lines that start from the Z axis and end at the actual line (determined by the equation above). The LENGTH of those horizontal lines (r) is given by the y value of the green line. This would essentially mean that the "r" quantity can be expressed as equivalent to y in the function of the straight line. Essentially all that means is that you take the equation above, and you make y the subject of the formula and then you can simply call "y" r(z) because that function now describes the length of r as it changes with respect to Z or the Z axis (so as the infinitesimal element moves up and down). Finally that would leave us with r(z) = a[1-(z/h)] And this equation does satisfy the common sense checks outlined in this video. When Z=h then r must be 0. When Z=0 then r must be a. From there the question is pretty easy but expressing r as a function of Z allows us to integrate r (which is a CHANGING quantity) indirectly with respect to Z. Generally that's how you're supposed broadly think when doing applied maths problems like this.
This make this realistic than i was thought in class. Thanks man
Thank you very much.
Can this equation work for the center of mass
Thank you so much Manteufel! You were my thermodynamics professor in college and your lectures are great. Had to brush up on this chart and this really helped.
I seriously cannot commend you enough. Clear and concise. I wish I had found you at the start of the semester. Thank you.
Great video, thanks very much. Seriously, this video should appear higher on the recommended list.
Where can i get the excel sheets for the calculation? Thank you
You're a legend man
Thank you very much sir
i have a problem right after adding the add-ins thermodynamic where it brings me to the VBA windows and the ThisWorkbook.VBProject.HelpFile = ThisWorkbook.Path & "\ThermoTablesHelp.chm" is in yellow. what can i do ?
I got full credit for this in transport phenomena 2. It still makes me angry that peter is a tubby boy whose wife is angry at him and hes teaching our class. Peter should stop lecturing about what we know from undergraduate and start teaching the students he has today. If peter were smart with words he would stop calling the equations animals. When peter talks about the power of words, i think about calculating the power in kcals stored in his body fat. Peter sweats when he takes a lot of steps. Maybe peter should build an excel spreadsheet to track his daily caloric intake.
you lack an explanation: "because we have more nitrogen" why? you dont explain why we have "more" nitrogen. "then we need to fix the nitrogen" I wonder what your class avg is? probably one of those teachers that have to use a bell curve to prevent the class from failing. P.S. if you are one of those teachers who implements a curve in the class because class performance is poor, newsflash is not because your students are dumb. Its because you teach poorly.
hi, thanks for the nice video. can you send me the add in?
Thanks 😊, Really helped
Why would air heat up in uniform fashion when the delta T with the refrigerant varies so much? Doesn't make sense.
x-axis is fraction of heat transfer. Specific heat of air is constant over temp range from T_in to T_out. If cp was highly dependent on T, then would not be straight line.
How can 2 to 3 is constant pressure when we add the heat? Shouldnt it be the reverse where pressure increae with the increae of heat?
love you
gay
Thank you, Dr.Manteufel. First I was your student back in UTSA and learned Heat Transfer. Now, I am teaching Heat transfer at North Park University Chicago, IL.
Ildar, glad you are doing well and teaching heat transfer!
Thank you so much professor
THANK YOUUUUU !!!! Litteraly discovering the software the evening before my exam Your saving my ass (maybe)
Well illustrated and to the point. It was difficult to find a good review of both y and x bar. Going in to take my FE next week and needed this refresher. Thank you
Many thanks! Good info.
Thank you (^^)/
You explained it so well!! Thank you!!!
super useful
33:01 Re= G(D)/miu
Do PVT have to equal zxy respectively? Or they can be anyone? I tried PVT as xyz, and I ended up getting R/V x R/P after partial differentiating
why - i mean wh y the 3 is negative
thank you sir
Why is air temperature increasing lineary? This is not what I learnt about T-A (temperature-area) diagram
How we calculate x4 ?
goat
هل من مصل على النبي محمد صل الله عليه وسلم وبارك الصلاة الإبراهيمية
When i did this question i had to multiply the given mass by 9.81 to get the weight and that was how i got correct answers but your process was right otherwise but could be a different question type so idk
friction for turbulent is not 0.316Re^0.25 BUT 0.316/Re^0.25, correct it???????
Are the reaction moments in these 2 hinges negligible in real-life? Or is it just the conditions given in the problem?
very helpful, thank you so much!
Live long
💖
@Randall Manteufel, at 30:38, shouldnt we have O2 in the product? considering that we have EXCESS AIR
you are correct, fix problem so it is 100% theoretical air (not %150), The rxn eqn is OK. The Q/nf eqn coefficient is 2 for O2_R (not 3) so final answer is -719,402 kJ/kmol. thanks
❤
What about finding temperature Ty?