DDIV
Mechanical
- Sep 25, 2020
- 2
It all started with question around heat dissipation of shaft power, that I think got it sorted out thanks to this forum.
But another question came up to surface when a somebody starts to talk about the Joule-Thompson effect.
So if we consider following (this is the actual case):
Ducting with a square area of 1 m2
Air velocity = 10 m/s = 10 m3/2
Air temp = 20 degree Celsius, assume density 1.2 kg/m3
In the middle of the ducting there is an obstruction causing 1000 Pa in pressure drop, so we have same mass flow in and out.
Then I mean that due to this there will be an increase of temperature after the obstruction of:
Power loss over obstruction = volumeflow*dP = 10*1000 = 10 kW
The obstruction is well insulated, therefore I say that this power loss will be transformed into a temperature raise:
dT = power loss / (massflow * cp) = 10 / (12*1.005) = 0.83 degree Celsius.
After the obstruction the temperature is 20.83 degree Celsius.
The above example must be suited to classify as an ideal gas (compression factor roughly 0.9999).
This was my thinking until somebody started to talk about Joule-Thomson effect.
I found here that if you go from 6 atm to 1 atm there is temperature drop around 2 degree Celsius due to the Joule-Thompson coefficient for air at 20 degree.
If I take my example above but change the obstruction to cause a pressure drop of 5 atm.
Then the temperature raise should be roughly 414 degree Celsius:
Power loss over obstruction = volumeflow*dP = 10*500 000 = 5000 kW
dT = power loss / (massflow * cp) = 5000 / (12*1.005) = 414 degree Celsius.
But the Joule-Thomson effect says a temperature drop on roughly 2 degree Celsius.
The above example is almost an ideal gas (compression factor roughly 0.998).
Ideal gas law also states that there should be a temperature drop after the obstruction, but maybe this is not applicable due to that its not a closed volume. I’m thinking of a moving boundary (closed volume) that goes from inlet to outlet and apply ideal gas law to it without adjusting for compression factor.
So my question comes down to following, why there is different outcome depending on approach:
Power equation = 20+414 = 434 degree Celsius (big increase of temperature)
Joule-Thompson effect = 20-2 = 18 degree Celsius (drop of temperature)
Ideal gas law = 6/20=1/x --> x= 3.33 degree Celsius (drop of temperature)
But another question came up to surface when a somebody starts to talk about the Joule-Thompson effect.
So if we consider following (this is the actual case):
Ducting with a square area of 1 m2
Air velocity = 10 m/s = 10 m3/2
Air temp = 20 degree Celsius, assume density 1.2 kg/m3
In the middle of the ducting there is an obstruction causing 1000 Pa in pressure drop, so we have same mass flow in and out.
Then I mean that due to this there will be an increase of temperature after the obstruction of:
Power loss over obstruction = volumeflow*dP = 10*1000 = 10 kW
The obstruction is well insulated, therefore I say that this power loss will be transformed into a temperature raise:
dT = power loss / (massflow * cp) = 10 / (12*1.005) = 0.83 degree Celsius.
After the obstruction the temperature is 20.83 degree Celsius.
The above example must be suited to classify as an ideal gas (compression factor roughly 0.9999).
This was my thinking until somebody started to talk about Joule-Thomson effect.
I found here that if you go from 6 atm to 1 atm there is temperature drop around 2 degree Celsius due to the Joule-Thompson coefficient for air at 20 degree.
If I take my example above but change the obstruction to cause a pressure drop of 5 atm.
Then the temperature raise should be roughly 414 degree Celsius:
Power loss over obstruction = volumeflow*dP = 10*500 000 = 5000 kW
dT = power loss / (massflow * cp) = 5000 / (12*1.005) = 414 degree Celsius.
But the Joule-Thomson effect says a temperature drop on roughly 2 degree Celsius.
The above example is almost an ideal gas (compression factor roughly 0.998).
Ideal gas law also states that there should be a temperature drop after the obstruction, but maybe this is not applicable due to that its not a closed volume. I’m thinking of a moving boundary (closed volume) that goes from inlet to outlet and apply ideal gas law to it without adjusting for compression factor.
So my question comes down to following, why there is different outcome depending on approach:
Power equation = 20+414 = 434 degree Celsius (big increase of temperature)
Joule-Thompson effect = 20-2 = 18 degree Celsius (drop of temperature)
Ideal gas law = 6/20=1/x --> x= 3.33 degree Celsius (drop of temperature)