Nuclear Material Temperatures - RTG Thoughts

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Discussion Overview

The discussion revolves around the temperatures of various nuclear materials, their heat generation rates, and the types of radiation they emit. Participants explore the implications of these factors in different environments, particularly in the context of radioisotope thermoelectric generators (RTGs) and their cooling mechanisms.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants inquire about charts or data relating to the temperatures of nuclear materials, their half-lives, and the types of radiation they emit.
  • One participant suggests using decay per unit volume to approximate heat generation, referencing the heat conduction equation and the activity of radionuclides.
  • Another participant emphasizes that the temperature of a material is influenced by its heat generation rate and the cooling method employed, noting that materials can reach different temperatures based on their environment.
  • There is a discussion about whether materials will continue to heat indefinitely without cooling, with some arguing that equilibrium will be reached due to radiative cooling, while others express uncertainty about the limits of temperature increase.
  • Participants discuss the specifics of heat transfer in space, highlighting that in a vacuum, radiative cooling is the primary means of heat dissipation.
  • One participant raises a practical question about measuring temperatures of nuclear materials in various environments, particularly in relation to adapting thermocouples for lower heat sources.

Areas of Agreement / Disagreement

Participants generally agree that cooling mechanisms play a crucial role in determining the temperature of nuclear materials, but there is disagreement about the implications of cooling and whether materials can reach unlimited temperatures without intervention. The discussion remains unresolved regarding the specifics of temperature behavior in different environments.

Contextual Notes

Limitations include assumptions about heat generation rates and cooling methods, as well as the dependence on specific environmental conditions. The discussion does not resolve the complexities of heat transfer in various scenarios.

Arctic Fox
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Are there any charts or information on how temperature-hot each nuclear material gets along with it's half-life and the type of radiation it releases (a, b, g)?

Thought about this from one of the nuclear meltdown threads...
 
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As a first approximation or in large volume (effectively infinite):

One simply needs the decay per unit volume. That provides a heat source \dot{Q}. With the heat source, then one simply solves the heat conduction equation.

\dot{Q} = E * A, where E is energy per decay, and A is activity.

The activity is simply A = \lambda N where \lambda is the decay constant and is defined by \lambda = \frac{0.69315}{t_\frac{1}{2}}. N is the atomic density of the radionuclide.

0.69315 is approximately ln(2).

This ignores the energy lost from particles, particularly gammas that leave the volume of interest. Alpha particles, on the other hand, travel on the order of 1 mm from parent nucleus, and beta particles travel a few mm or cm depending on energy.

=====================

For small finite sources, gamma rays would leave the source and scatter in whatever matter surrounds the source.

There is a special code, MCNP or Monte Carlo Neutron Photon, which does special calculations for the problem stated in the initial post.
 
Last edited:
Arctic Fox said:
Are there any charts or information on how temperature-hot each nuclear material gets along with it's half-life and the type of radiation it releases (a, b, g)?

Thought about this from one of the nuclear meltdown threads...

Artic_Fox,

The temperature is not dictated directly by the material.

As Astronuc points out - which material you have will determine a heat
generation rate. You also have to know how the material is being cooled -
and the net "resistance" to heat flow.

The material will get as hot as it needs to so that the outflow of heat will
equal the internal heat generation rate.

Thus if you have the material sitting in air - with relatively poor
heat conduction rate to the air - the material will get hotter than if
you immersed it in water - with relatively better heat transfer
characteristics.

Dr. Gregory Greenman
Physicist
 
So, the material will continue to get hotter and hotter with no limit, if there is no means/attempt at cooling?
 
No, the system will reach equilibrium, if one puts an appropriate radiator in the system (presuming this is an RTG in space). Without a radiator, the RTG would reach a high temperature, which might cause it to melt and disassemble itself.

An RTG system (on a spacecraft ) radiates heat to space (there is not conduction or convection in a vacuum), with the heat flux (Q") given by

Q'' = e \sigma (T_r^4 - T_s^4), where
e= emissivity (= 1 for ideal radiator),
\sigma= Stefan's constant,
T_r= temperature of radiator, and
T_s= temperature of space

It is know as "Stefan-Boltzmann Law" - find more at http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/stefan.html

The heat rejected is then Q = Q"A where A is the surface area of the radiator.

On a large body like a planet, e.g. Earth or Mars, or on a moon, on can use the ground as a heat sink (conduction). On Earth, the atmosphere or water bodies are the heat sink - combination of conduction and forced convection.
 
Last edited:
Arctic Fox said:
So, the material will continue to get hotter and hotter with no limit, if there is no means/attempt at cooling?

Arctic_Fox,

As Astronuc points out - there is ALWAYS cooling.

In the absence of any type of active or intentional cooling - there is
always "radiative cooling" - the hot object radiates heat away as
radiation.

This will ALWAYS limit the temperature.

Dr. Gregory Greenman
Physicist
 
Okay, let me try this again. :)

How hot would each element get if they were just sitting on a wooden table with a thermometer physically touching the top of the material? :D I'm trying to figure out just how much work may be involved in trying to adapt thermocouples to a lower heat source. Someone here meantion using beter TCs, and I am starting to agree.


And I'm not understanding how to remove heat in space; no air? If I remember right, 1)Radiated, 2)Conduction, 3)Convection.

Just "Radiated" into space? :confused:
 
Last edited:
The temperature depends on heat generation rate and heat transfer rate to the surroundings.

On a table in an atmosphere, one would have conduction to table and air, convection with the air, and perhaps radiative cooling, but the radiative cooling would be a small component compared to the other two.

Space is effectively a vacuum, so radiative cooling is all there is. I already provided an equation for temperature, based on heat flux.

To solve the problem, the heat flux needs to be specified, and on can assume about 3-4K for deep space temperature.
 

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