Newtons Law of Cooling applied to hot Neon and Hydrogen gas

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Discussion Overview

The discussion revolves around the application of Newton's Law of Cooling to the cooling rates of hydrogen and neon gases contained in copper containers. Participants explore the implications of thermal conductivity, specific heat, and the assumptions necessary for applying the law to this scenario.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents a problem involving the cooling of hydrogen and neon gases, applying Newton's Law of Cooling and providing initial calculations for cooling times.
  • Several participants question the units used for thermal conductivity and the implications for the calculations, suggesting that the units must be dimensionless for the exponential function in the cooling law.
  • There is a discussion about the relationship between thermal conductivity and the cooling constant in Newton's Law of Cooling, with questions about potential conversion factors.
  • One participant argues that additional information, such as the thickness of the copper container or convection coefficients, is necessary to solve the problem accurately.
  • Another participant emphasizes the complexity of the cooling process, noting that the rate of heat transfer depends on the temperature gradient and that the problem cannot be solved solely using Newton's Law of Cooling.

Areas of Agreement / Disagreement

Participants express disagreement regarding the application of Newton's Law of Cooling to this problem, with some arguing that it cannot be solved with the information provided, while others attempt to apply the law despite the noted complications. No consensus is reached on the validity of the initial calculations or the applicability of the law in this context.

Contextual Notes

Limitations include the lack of information on the thickness of the copper container and the convection coefficients, which are necessary for accurately determining the cooling rates. The discussion also highlights the confusion surrounding the units of thermal conductivity and their application in the context of Newton's Law of Cooling.

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Homework Statement


1 mole of Hydrogen gas at 300 Kevin is contained in a thin walled copper container.
In container #2 there is 1 mole of Neon gas also at 300 Kevin.
The volume= 22.4 liters and surface area ,A = .476 m^2
The surroundings are at 100 deg Kelvin.
The specific heat of H2= 5 cal/mole (K) Specific heat for Neon = 3cal/mole (K)
The thermal conductivity (k) H2 = .0433 cal/sec For Neon = .0116 cal/sec

How many seconds for each gas to cool to 120 Kelvin ?


Homework Equations


Since the heat transfer equation , Q/t = -kA (T2-T1)/L
is with T2 at a fixed temperatue and in the above problem T2 , the temp of the gases,
are changing. I am applying k to the solution to Newtons law of cooling .
T(t) = T surr. + (Tgas - Tsurr)e^-kt

120K (t) = 100K + 200K e^-kt


The Attempt at a Solution


So 20K/200K= e^-kt
2.3 = kt
For Hydrogen t = 53 seconds ,
For Neon t = 198 seconds

note I originally put this problem in the physics section but it should qualify for chemical
thermodynamics. Hopefully the chemists here can be of more help !
 
Last edited:
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Check your units: if kt is dimensionless (which it must be to take the exponential), k must have units of s-1. And why do your thermal conductivity values have units of power?
 
Mapes said:
Check your units: if kt is dimensionless (which it must be to take the exponential), k must have units of s-1. And why do your thermal conductivity values have units of power?

The units are in power since I converted Watts to calories.
This k value is for: Q/t = -kA (T2-T1)/L
So there is a unit problem in appling it in the Newtons Law of Cooling solution.
The question now is are there tables of k values that can be used with Newtons solution,
or can it only be obtained by taking temperatures at t0 ,t1,t2 and solving for k. ?

Or since the thermal conductivity (k) above in Q/t = -kA (T2-T1)/L in units
(cal/sec)/meter^2)C deg/meter
And (k) in units 1/sec here: T(t) = Tsurr + (T initial - Tsurr) e^-kt
Are both related to heat transfer for a specific material can there be a conversion ?
 
Last edited:
But thermal conductivity should have units of power length-1 degree-1...
 
Mapes said:
But thermal conductivity should have units of power length-1 degree-1...

Agree : Watts/(Kelvin ) (meter) multiplied by (delta T) ( Area m^2) divided by Length (m)
The units in post #3 were copied from a text, it is a confusing copy.
So with 1 watt = .238 cal/sec.
Thermal conductivity should be: cal/sec / kelvin * meter ( T2-T1) ( m^2) / m
Thats as in : Q/t = -kA (T2-T1)/L
With k itself in power/ degree * length
In Newtons law of Cooling: dT/dt = -k (T initial- T surr.)
With this k in 1/sec
And both of these constants are related to heat transfer in a specific material . Is There a conversion factor from the thermal conductivity k
to the law of cooling k ?
 
Last edited:
morrobay said:
Is There a conversion factor from the thermal conductivity k
to the law of cooling k ?

Not without more information, such as the thickness of the copper, or the convection coefficient on both sides. I don't see how the problem is solvable from the information given in post #1.
 
You cannot really solve this kind of problem just with Newton's law of cooling.
Even for a solid body, with no convection, it is a little more difficult than that.
The rate of heat transfer to the medium depends on the temperature difference between the surface of the material (your gas) and the temperature of the medium. But the evolution of the surface temperature depends on how fast can heat be transported from the inner volume to the surface.
You can imagine some extreme cases to see the point.
If the thermal conductivity is very high, then the temperature in the volume of the object is almost uniform and the whole material cools down as a whole. In this case you can find the solution just by using Newton's law of cooling. It probably works reasonably well for metals.

The other extreme is a very good (ideal) insulator. In this case the outer layer cools down to outside temperature but there is very little heat being transported from the inside to compensate for this. The inner volume stays at the same (initial temperature).

In real cases you are somewhere in between. There is a temperature gradient through the material. The question "how long it takes to cool down" is not even well defined.
 

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