Energy use, conductive-convective layers and air films

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SUMMARY

The discussion focuses on calculating heat loss through a refrigerator door with specific dimensions and thermal conductivity. The door's dimensions are 1.5 m high, 0.80 m wide, and 6.0 cm thick, with a thermal conductivity of 0.21 Wm-1°C-1. The heat loss calculations involve using the equation Q=kA(ΔT/Δx)t for conductive heat transfer. Participants discuss the impact of conductive-convective layers on heat loss, particularly in still air conditions, and the importance of accurately determining the conduction-convection parameter "h" for precise calculations.

PREREQUISITES
  • Understanding of thermal conductivity and its units (Wm-1°C-1)
  • Familiarity with heat transfer equations, specifically Q=kA(ΔT/Δx)t
  • Knowledge of conductive-convective layers and their effects on heat transfer
  • Ability to calculate temperature differences (ΔT) in thermal contexts
NEXT STEPS
  • Research the conduction-convection parameter "h" and its derivation
  • Learn about the impact of air movement on heat transfer in thermal systems
  • Explore advanced heat transfer equations for complex scenarios
  • Study the principles of thermal insulation and its applications in refrigeration
USEFUL FOR

Students in thermodynamics, engineers involved in refrigeration design, and anyone interested in understanding heat transfer principles in practical applications.

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Homework Statement


The door of a refrigerator is 1.5 m high, 0.80 m wide and 6.0 cm thick. Its thermal conductivity is 0.21Wm-1 degrees Celsius-1.
a) what is the heat loss per hour through the door neglecting convection effects?
b) Air is usually still inside the refrigerator so there will be a conductive convective layer on the inside but in a busy kitchen such a layer will be absent on the outside. What is the heat loss per hour in this case and what is the temperature of the inside surface of the door?
C) at night the kitchen is also still; what is the heat loss per hour now, and what are the temperatures of the inside and outside surfaces?

A=1.2 m^2
Δx=.06 m
k=.21Wm-1°C-1
ΔT=27°C
t=3600 seconds

Homework Equations


For a) Q=kA(ΔT/Δx)t
For b) part one, Q=(Tf-Ta)xhxAxt, where Tf is Temp in fridge and Ta is temp of air outside fridge.
For b) part two, I have no idea.
For c) I have no idea.

The Attempt at a Solution


I was able to solve a) through the equation above. I know that k=.21Wm-1°C-1, A=1.2m^2, ΔT=27, Δx=.06, and t=3600 seconds.

For b) part one, I used the equation above to solve for the first part. I'm not even sure if I did it right because the book rounds the answer up kind of by a lot. Using that equation, I got 1.7 * 10^5 Joules. The book says 2.0*10^5 Joules. I realized though that for this part, I thought "h" meant height, but it's actually the conduction-convection parameter which is 1.8(ΔT)^1/4. In this case, ΔT is 27°C, but the equation already incorporates ΔT into the equation so I don't understand why we use ΔT twice in this equation. If I solve for "h" using 27°C, I get h=4.1 and plugging that back into the equation, I get 4.8*10^5 Joules which is definitely wrong.

For b) part two, is it right to assume that the temperature at the surface inside the door is right between the temperature in the fridge and outside of the fridge? Which means it would be 13.5°C. Or is there a way to actually solve for this? The book says it's 13.5°C so it seems like we just assume it's in the middle.
 
Last edited:
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In part b, the ##\Delta T## refers to the temperature difference between the air inside the refrigerator and the inner surface of the door.
In part c, the ##\Delta T## refers separately to the temperature difference between the outer surface of the door and the room temperature.

And, yes, there is a way of solving all this.
 

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