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Ian why are you confounding this even more? Why not stick with the original thought experiment and prove it right, instead of continually altering it? That ones already established here, its been written out, and yet you continue to claim its right but refuse to use it to show its right...
If wire wants to continue playing your silly deflection its on him, but your "physics" persona is done for.. You know about as much physics as my 13 year old...
BTW Ian, remember the chamber, and the vacuum.. And thats all the help im giving you..
wirebender doesnt take the radiating abilities of the different areas into account. hell, if you push the two bars together you have lost 20% of the area (10% if end to end). that would magically increase the bars temperature dramatically wouldnt it? and you dont even have to consider the change by adding conduction to the mix because wirebender thinks they are both the same temperature anyways!If another identical non-heated and colder plate is inserted into the Vacuum Chamber next to the heated Plate then:
The 2nd Plate also has an emissivity = 1 and a surface Area for the 2nd plate = 1 m^2
We can easily determine the equilibrium temperature of both plates by using the Stefan-Boltzmann Law and The Law of Conservation of Energy.
The TOTAL amount of energy available is 744.95 Watts and both plates will have the same temperature at equilibrium, so they can be considered to be a single radiating body with double the radiating surface area.
The area of both plates = 2 m^2 so the Radiation emitted by both plates at equilibrium = 744.95 Watts / 2 m^2 = 372.48 w/m^2
And the equilibrium temperature for both plates will be 284.69 K or 53 deg
which is wrong not only because he has failed to calculate the effective surface area of the masses but because there is a temperature gradient on and between both bars. the only part of his calculations which is right is the part where he states the power input equals the power output. and even that is only true after equilibrium has been reached.wirebender stated- equilibrium temperature for both plates will be 284.69 K
where did your comment go wirebender?
anyways, so why dont you start cranking out the math.
first define the heater and show what the inside gradient to the outside is. once you have found the outside temps then show how much radiation will go into the second bar. then mathematically show how the heat will cross the second bar and come out of the surfaces. for bonus points you could show the radiation difference from the container side closest to the heated bar compared to the container side directly opposite across the second bar.
the reason I keep making small alterations to the thought experiment is to imagine what different results will occur.
now I will try to imagine a scenario where you two could be correct.
what are the absolute basics of the experiment? a heater producing 750w and a cooled container capable of recieving 750w without changing temperature. is this the point where your thinking stops. the trivial position of 750w in then out? any material inside the container is meaningless, only the input and output?
the bare heater radiating directly to the cold walls is the lowest temperature possible. once the bar is placed around it, insulating it, the temperature of the heater must increase to compensate for the shrinking of the temperature differential.
once the bar is placed around it, insulating it, the temperature of the heater must increase to compensate for the shrinking of the temperature differential.
the bar itself has a temperature gradient from the heater to the outside surface which can then radiate to the cooled wall. wirebender's math has already broken down, there has been an increase in the temperature of the heater due to insulation and there is a temperature gradient in the bar. but the input still equals the output.
adding a second bar only increases the insulation. which increases the the temperature of the first bar which then increases the temperature of the heater. but input still equals the output. 750w.
is it possible that wirebender and gslack are only considering the final outcome?
even then wirebender's math is wrong because...
If another identical “non-heated” and colder plate is inserted into the Vacuum Chamber next to the heated Plate then:
The 2nd Plate also has an emissivity = 1 and a surface Area for the 2nd plate = 1 m^2
We can easily determine the equilibrium temperature of both plates by using the Stefan-Boltzmann Law and The Law of Conservation of Energy.
The TOTAL amount of energy available is 744.95 Watts and both plates will have the same temperature at equilibrium, so they can be considered to be a single radiating body with double the radiating surface area.
The area of both plates = 2 m^2 so the Radiation emitted by both plates at equilibrium = 744.95 Watts / 2 m^2 = 372.48 w/m^2
And the equilibrium temperature for both plates will be 284.69 K or 53 deg
wirebender is a fool to invoke general formulas when the results of those formulas are not the answer we are looking for.
where did your comment go wirebender?
anyways, so why dont you start cranking out the math.
first define the heater and show what the inside gradient to the outside is. once you have found the outside temps then show how much radiation will go into the second bar. then mathematically show how the heat will cross the second bar and come out of the surfaces. for bonus points you could show the radiation difference from the container side closest to the heated bar compared to the container side directly opposite across the second bar.
he is tired of your silly ass for one, and hes not here...
he isn't going to do any more work for you, its wasted on you. You don't care about the truth, you care about being right..
Apply the Stefan-Boltzman Law to what we know
P = e*BC*A*T^4
Where P = net radiated power (Watts), e = emissivity, BC = Stefan’s constant 5.67 X 10^-8, A = area and T = temperature of radiator in K
744.9=5.67 X 10^-8 X .25 m^2 X(478.79K)^4
as usual wirebender doesnt think these things through, he confounds one thing for another.
P = e*BC*A*T^4 what is this formula describing? it is describing the power emitted by a body at a certain temperature. in a system where there is no back radiation. in other words a container at zero degrees Kelvin.
I agree that the heated bar in a zero degree Kelvin container would be 479K. his math is correct to this point.
as usual wirebender doesnt think these things through, he confounds one thing for another.
P = e*BC*A*T^4 what is this formula describing? it is describing the power emitted by a body at a certain temperature. in a system where there is no back radiation. in other words a container at zero degrees Kelvin.
There is no such thing as backradiation Ian, any more than there is back conduction or back convection. Backradiation defies the 2nd law of thermodynamics. Which derivitive of the SB law do you believe suggests the existence of backradiation and can you show even one shred of observed, repeatable, experimental evidence to support the claim?
I agree that the heated bar in a zero degree Kelvin container would be 479K. his math is correct to this point.
My math is correct from beginning to end Ian.
all of the SB derivatives incorporate backradiation except the ones that deal with a single radiating body.
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the T^4 - T^4 tem is the backradiation.
Ian, If you poke a hole in the sidewall of your cars tire, can you place your hand a few centimeters away and force the air back in it? or is the energy from the expelling air to great to allow the air to go back whence it came?
if you point a flashlight at a mirror will it make that flashlight brighter? or will the illumination make the mirror and environment brighter?
You can virtually take any type of real world application and find the same type of examples. Every single one in the natural world without help to achieve a difference will result in the stronger energy winning over the weaker energy.
Yet somehow you seem to think its not going to apply in spencers experiment or in your variations... WOW... I have no words man... Good luck with your patent on your endless heat engine bud...LOL
interesting description there wirebender....no back conduction!
does that mean that no molecules are allowed to jiggle in the opposite direction of the heat flow? is it a physical impossibility? is it like the radiation that magically disappears (somewhere, you wont be specific) after being emitted from a CO2 molecule towards the earth? hahahaha.
all of the SB derivatives incorporate backradiation except the ones that deal with a single radiating body.
![]()
the T^4 - T^4 tem is the backradiation.
Sorry Ian, but they do not. The equation p=sigma (T^4 - T^4) most certainly does not describe backradiation. That equation accurately describes the SB law as proven by SB. ( T^4 - T^4) describes radiation from a blackbody at temperature T^4 into a background at temperature T^4. There is nothing like backradiation in that equation.
If you want an equation incorporating backradiation, then it must take the form P=(sigma T^4)-(sigma T^4).
Algebraically the two look similar but they describe physics that are very different. One describes the SB law as derived and proven by SB and the other describes a non physical event that has never been seen to happen in nature or the laboratory.
p=sigma (T^4 - T^4) is the actual SB law and it describes radiation from the blackbody to the background, period.
P=(sigma T^4)-(sigma T^4) on the other hand describes (sigma T^4) radiation from the blackbody to the background minus (sigma T^4) radiation from the background to the blackbody.
The SB law in the form p=sigma (T^4 - T^4) has appeared in physics texts since the late 1800's. The law in the form P=(sigma T^4)-(sigma T^4) on the other hand only appears in atmospheric physics textbooks and is a new phenomenon. If you are interested in verifying that bit of information, here is a short list of physics texts that teach SB as derived by SB. Interestingly enough, I can't find a single physics text printed before 1980 that teaches the corrupt SB law.
Radiative Transfer by Chandrasekhar
An Introduction to Radiative Transferby Peraiah
Radiative Heat Transfer by Modest
And here are a few that teach the corrupted SB law that describes backradiation.
An Introduction to Atmospheric Physics by Fleagle-Businger
Radiative Transfer in the Atmosphere and Ocean by Thomas-Stamnes
An Introduction to Atmospheric Physic by Andrews
A First Course in Atmospheric Radiation by Petty
Interesting to note who is teaching backradiation as reality and why, isn't it?
interesting description there wirebender....no back conduction!
does that mean that no molecules are allowed to jiggle in the opposite direction of the heat flow? is it a physical impossibility? is it like the radiation that magically disappears (somewhere, you wont be specific) after being emitted from a CO2 molecule towards the earth? hahahaha.
You are proof of Clark's adage that any sufficiently advanced technology is indistinguishable from magic. In this case, the math (which isn't that tough by the way) is so far over your head that you seem to be able to only refer to what it describes as "magic". Not surprising, but really, really sad.