Thermal Conductivity

This article has not been revised for the current version (U51-600112). It was last updated for U47-562984. It may contain inaccuracies.

This article has not been revised for the current version (U51-600112). It was last updated for U47-562984. It may contain inaccuracies.

Thermal Conductivity is the property of a material that determines how quickly it heats or cools as it comes into contact with objects of different temperatures. Although the game states that between two objects, the lowest thermal conductivity is used, this is not true for all cases.

Equations

The calculation of Heat Transfer $q$ in $DTU$ is mainly a product of:

• $\Delta T$ the Temperature difference in °C
• $\Delta t$ the passing time, which is always one tick, $0.2s$
• $k$ the applicable thermal conductivity in $DTU/(m \cdot s \cdot \text{°}C)$
  • ${\color {Cerulean}k_{lowest}}$ is the lower of the two
  • ${\color {Green}k_{geom}}$ is the geometric mean of the two: $\sqrt{k_1 \cdot k_2}$
  • ${\color {Red}k_{avg}}$ the arithmetic average of the two: $0.5 (k_1 + k_2)$
  • ${\color {Blue}k_{mult}}$ the two multiplied together: $0.5\cdot k_{1}\cdot k_{2}$

For heat transfer with buildings, there is an additional factor:

• $C_{hot}$ the thermal mass per area of the hotter object: ${\frac {m\cdot c\cdot \left[{\frac {1}{5}}\right]_{\text{if building}}}{A}}$ where $m$ is mass, $\,c$ is specific heat capacity (SHC), $\,A$ is the area of the building/cell (1 for cells), and divide by 5 if the hotter object is a building.

Equations

Scenario	Formula
Cell ↔ adjacent Cell
Solid ↔ Solid	$q=\Delta T\cdot \Delta t\cdot {\color {Green}k_{geom}}\cdot 1000$
Solid ↔ Liquid
Gas ↔ Liquid
Gas ↔ Gas
Solid ↔ Gas	$q=\Delta T\cdot \Delta t\cdot {\color {Green}k_{geom}}\cdot 1000\cdot 25$
Liquid ↔ Liquid	$q=\Delta T\cdot \Delta t\cdot {\color {Green}k_{geom}}\cdot 1000\cdot 625$
Entity lying on a Solid	$q=\Delta T\cdot \Delta t\cdot {\color {Cerulean}k_{lowest}}\cdot 62.5$
Building ↔ Solid tile below it	$N/A$
pipe ↔ adjacent pipe	$N/A$
Inside a Cell
Entity ↔ Cell	$q=\Delta T\cdot \Delta t\cdot {\color {Cerulean}k_{lowest}}\cdot 1000$
Building ↔ Cell	$q=\Delta T\cdot \Delta t\cdot {\color {Blue}k_{mult}}\cdot C_{hot}$
Building ↔ Building	$N/A$
Building ↔ Conduction Panel	Use Building ↔ Cell but treat panel as a 100 kg cell and divide result by 11
Building ↔ Entity	$N/A$
Building's Contents
pipe ↔ pipe contents	$q=\Delta T\cdot \Delta t\cdot {\color {Red}k_{avg}}\cdot 50$
Insulated pipe ↔ contents	$q=\Delta T\cdot \Delta t\cdot {\color {Cerulean}k_{lowest}}\cdot 50$
pipe contents ↔ conduction panel	$q=\Delta T\cdot {\color {Red}k_{avg}}\cdot 50$ (as the packet teleports across the panel)
Cell ↔ pipe contents	$N/A$: transfers through the pipe instead
pipe bridge ↔ bridge contents	$N/A$: bridges teleport elements, NO contents
Building ↔ building contents	$N/A$
Building's Cell of Interest ↔ building contents	see Cell↔Entity

Thermal Element Categories

Category	Examples
Cell	Gas, Liquid, Solid Block, Tiles, closed Doors, Joint Plate (middle), Tube Crossing (middle), etc
Entity	Dupes, Creatures, Plants, Debris, Mesh Tile, Airflow Tile, etc
Building	pipes, bridges, background buildings, geysers, generators, open Doors, Pneumatic doors (open/closed), etc
Pipe	Liquid Pipe, Gas Pipe, Conveyor Rail, Wires (all kinds), Automation Wire, and Automation Ribbons
Bridge	Liquid, Gas, Conveyor Wire, Automation, and Automation Ribbons
Contents	Building Production Storage (Input/Output), Reservoirs, Fridges, Compactors, etc
Special	Tempshift Plate, Conduction panel, Refrigerator, Compost

Certain buildings apply a modifier to their material thermal conductivity:

• Insulated Tiles: divide by $({\frac {2}{255}})^{2}$ (not correctly reflected under Properties)
• Insulated Liquid Pipe and Insulated Gas Pipe: divide by 32
• Wires of any kind: divide by 20 (this may be a legacy of a ditched feature making wires truly overheat)
• Radiant Pipes, Radiant Gas Pipes and Conduction Panel: multiply by 2

a Tempshift Plate conducts as a building, and also conducts to all Cells in a 3x3 (centered on it)

a Conduction Panel is a (long) pipe

• conducts as a building in its cells
• specially conducts building ↔ building in its MIDDLE tile
• conducts any elements passing through it via pipe ↔ pipe contents

A building's contents act like they are in the building's Cell of Interest, and exchange heat through the Cell↔Entity Equation.

• Powered Refrigerator, or Compost act as a normal building. BUT the contents will only interact with an imagined 277.15K (fridge) or 348.15K (compost) source at a locked conductivity of 1000 regardless of their material.

Bridges act as a long building, conducting along its length.

• You can stack multiple bridges to increase heat transfer along the cells
• You can use bridges to help stabilize a Guide/Liquid Airlock from evaporation or sublimation.

Joint Plates, & Tube Crossings act as a Cell, the connection points on the sides are cosmetic (for thermal conductivity)

Insulated Tiles reduce the thermal conductivity of their building material by (2/255)² (or 16 256) instead of 100 as stated in the game. It also uses ${\color {Cerulean}k_{lowest}}$instead of ${\color {Green}k_{geom}}$for the purpose of cell to cell conductivity, which is mostly going to be the insulated tile conductivity. Solid to gas multiplier still applies.

Note: in real life, the units would cancel out, but surface area plays no role in ONI's calculation. Therefore, an additional $[m]$ meter needs to be multiplied to the product to have the equation result in DTU. (Not just meter, but a large string of units when calculating buildings.)

Another way to interpret this is that the units of Thermal Conductivity are given in-game as $DTU/(m \cdot s \cdot \text{°}C)$ while the unit is actually interpreted as $DTU/(s \cdot \text{°}C)$.

Recap of Cell to Cell multipliers

				Gas	Liquid	Solid
Gas				1	1	25
Liquid				1	625	1
Solid				25	1	1

Because of the Gas to Solid x25 multiplier, it's recommended to add a double tiles layer or a thin liquid layer when trying to insulate two rooms, to instead get a x1 multiplier.

Limits of Heat Transfer

Lower Limits

Heat Transfer will not occur if:

• the temperature difference is less than 1 °C
• the calculated thermal flow is less than 0.1 DTU
• either of the masses is less than 1g

Upper limits

Heat Transfer between cells has the following cap:

• If the calculated heat transfer would result in a temperature jump of more than a fourth of their temperature difference $(T_1-T_2)/4$ in either material.

  $q_{\text{max }1a}=\frac{T_1-T_2}{4}\cdot m_1 \cdot c_1 \quad \text{or}\quad q_{\text{max }1b}=\frac{T_1-T_2}{4}\cdot m_2 \cdot c_2$

  Simply said: if the temperature difference is 40 °C, a materials temperature can change at most 10 °C per tick

Building Limits

Heat transfer between a building and a cell has different limits, the lower limits which are applied to cells do not apply to buildings, but the upper limit is conceptually similar.

A building exchanges heat with all cells it covers simultaneously. In order to ensure that thermodynamics will not be violated the game limits heat transfer per cell such that at most the final temperature of the building would be the equilibrium temperature, assuming that the building completely covers such cells:

$T_{eq} = \frac{T_{building} \cdot C_{building} + T_{cell} \cdot C_{cell} \cdot A}{C_{building} + C_{cell} \cdot A}$

The maximum permitted heat transfer per cell is the difference between the building's temperature and the equilibrium temperature divided by the Area of the building.

$q_{max} = C_{building} \cdot \frac{T_{building} - T_{eq}}{A}$

If the thermal mass of the cell is very large relative to the building, then the maximum temperature change can be approximated as simply $\frac{\Delta T}{A}$

Floating Point Calculation Limits

While the above limits are deliberately implemented, it is also possible for heat exchange to fail to happen due to limitations of the floating point calculations used to calculate temperature changes.

Internally ONI uses 32 bit floating point numbers to represent temperatures, and due to the limited precision of floating point numbers it is possible for the result of a floating point calculation to be the same number. For example with 32 bit floats, the calculation: 300.0 + 0.00001 = 300.0

The game has a rule that if either tile fails to change temperature, then no heat exchange is allowed to take place, this prevents an exploit where a large tile, especially an unnaturally large tile, infinitely dumps heat/cooling into a smaller tile without itself changing temperature.

In real games this limit comes up all the time when the temperature difference between an Insulated Tile and a solid or liquid tile is relatively small. For example an Igneous Rock Insulated Tile which is itself at 20 C, will not exchange heat with a solid or liquid tile unless the temperature delta is at least 248.05 C, and won't exchange heat with a gas tile unless the temperature delta is at least 9.92 C. This makes it quite easy to achieve actually zero heat transfer without resorting to the Insulite material or vacuum. The exact formulas governing this are: $\Delta T_{ignorable}=2^{\lfloor \log_2(T)-24 \rfloor}$ and $q_{max}=\Delta T_{ignorable} \cdot m \cdot SHC$, where $T$, $m$, and $SHC$ are for the cell holding everything constant, and $q_{max}$ is the heat-exchange formula relevant between the two cells, which can be reversed to find $\Delta T_{max}$.

It is also readily observed with liquid tiles, Magma and Water can have immense thermal mass which means relatively large DTU inputs are required to cause a temperature change. This results in the paradoxical outcome where full magma tiles don't exchange heat with insulated tiles, but partial magma tiles can exchange heat if they are sufficiently low mass. Using the above formula but applied to the Magma tile instead of the insulated tile, we can see that a cell with 715.6 kg or more magma will be unable to exchange temperature with an Igneous Rock Insulated Tile at 0C or higher, regardless of the magma temperature. For Mafic Rock, which has half the conductivity, only 357.8 kg of magma are needed.

Suffice to say that while floating point imprecision sometimes causes heat exchange to not happen at all, when temperature changes are small it also causes the actual temperature change to deviate quite significantly from what higher precision calculations would suggest.

Thermal descriptors

There are 4 thermal descriptors in the game, and they get attached to elements when their thermal characteristic reach a certain threshold. These descriptor does not affect the element any further.

• Thermally Reactive: Elements have a specific Heat Capacity of less than or equal to 0.2
• Slow heating: Elements have a specific Heat Capacity of greater than or equal to 1.0
• Insulator: Elements have a thermal conductivity of less than or equal to 1.0
• High Thermal Conductivity: Elements have a thermal conductivity of greater than or equal to 10.0

Pipes list

Liquid Pipes

Liquid Pipes

Pipe	Material	Thermal Conductivity
Insulated Liquid Pipe	Insulite	0.0000003125
Liquid Pipe	Insulite	0.00001
Insulated Liquid Pipe	Ceramic	0.019375
Insulated Liquid Pipe	Obsidian	0.0625
Insulated Liquid Pipe	Igneous Rock	0.0625
Insulated Liquid Pipe	Sedimentary Rock	0.0625
Insulated Liquid Pipe	Sandstone	0.090625
Insulated Liquid Pipe	Granite	0.1059375
Insulated Liquid Pipe	Wolframite	0.46875
Insulated Liquid Pipe	Tungsten	0.46875
Liquid Pipe	Ceramic	0.62
Liquid Pipe	Obsidian	2
Liquid Pipe	Igneous Rock	2
Liquid Pipe	Sedimentary Rock	2
Liquid Pipe	Sandstone	2.9
Liquid Pipe	Granite	3.39
Insulated Liquid Pipe	Thermium	6.875
Liquid Pipe	Wolframite	15
Liquid Pipe	Tungsten	60
Radiant Liquid Pipe	Lead	70
Radiant Liquid Pipe	Niobium	108
Radiant Liquid Pipe	Steel	108
Radiant Liquid Pipe	Iron	110
Radiant Liquid Pipe	Copper	120
Radiant Liquid Pipe	Tungsten	120
Radiant Liquid Pipe	Gold	120
Radiant Liquid Pipe	Cobalt	200
Liquid Pipe	Thermium	220
Radiant Liquid Pipe	Aluminum	410
Radiant Liquid Pipe	Thermium	440

Gas Pipes

Gas Pipes

Pipe	Material	Thermal Conductivity
Insulated Gas Pipe	Insulite	0.0000003125
Gas Pipe	Insulite	0.00001
Insulated Gas Pipe	Ceramic	0.019375
Insulated Gas Pipe	Mafic Rock	0.03125
Insulated Gas Pipe	Obsidian	0.0625
Insulated Gas Pipe	Igneous Rock	0.0625
Insulated Gas Pipe	Sedimentary Rock	0.0625
Insulated Gas Pipe	Sandstone	0.090625
Insulated Gas Pipe	Granite	0.1059375
Gas Pipe	Ceramic	0.62
Gas Pipe	Mafic Rock	1
Gas Pipe	Obsidian	2
Gas Pipe	Igneous Rock	2
Gas Pipe	Sedimentary Rock	2
Gas Pipe	Sandstone	2.9
Gas Pipe	Granite	3.39
Radiant Gas Pipe	Gold Amalgam	4
Radiant Gas Pipe	Iron Ore	8
Radiant Gas Pipe	Cobalt Ore	8
Radiant Gas Pipe	Copper Ore	9
Radiant Gas Pipe	Pyrite	9
Radiant Gas Pipe	Wolframite	30
Radiant Gas Pipe	Aluminum Ore	41
Radiant Gas Pipe	Niobium	108
Radiant Gas Pipe	Steel	108
Radiant Gas Pipe	Thermium	440

Solid Tiles list

Important: For Insulated Tiles, these numbers will not match what is seen in-game. This is because the value displayed in-game is $\frac{base}{100}$, but the actual value used by calculations (and shown here) is $base \cdot (\frac{2}{255})^2$.

Tiles

Tile	Material	Thermal Conductivity
Insulated Tile	Insulite	6.15e-10
Tile  Carpeted Tile	Insulite	0.00001
Insulated Tile	Ceramic	0.0000381
Insulated Tile	Mafic Rock	0.0000615
Insulated Tile	Fossil	0.000123
Insulated Tile	Igneous Rock	0.000123
Insulated Tile	Obsidian	0.000123
Insulated Tile	Sedimentary Rock	0.000123
Insulated Tile	Sandstone	0.000178
Insulated Tile	Granite	0.000209
Plastic Tile	Plastic	0.150
Plastic Tile	Solid Visco-Gel	0.450
Tile  Carpeted Tile	Ceramic	0.620
Window Tile	Glass	1.110
Tile  Carpeted Tile	Mafic Rock	1.000
Tile  Carpeted Tile	Fossil	2.000
Tile  Carpeted Tile	Igneous Rock	2.000
Tile  Carpeted Tile	Obsidian	2.000
Tile  Carpeted Tile	Sedimentary Rock	2.000
Tile  Carpeted Tile	Sandstone	2.900
Tile  Carpeted Tile	Granite	3.390
Metal Tile	Depleted Uranium	20.000
Metal Tile	Lead	35.000
Metal Tile  Bunker Tile	Steel	54.000
Metal Tile	Niobium	54.000
Metal Tile	Iron	55.000
Metal Tile	Copper	60.000
Metal Tile	Gold	60.000
Metal Tile	Tungsten	60.000
Window Tile	Diamond	80.000
Metal Tile	Cobalt	100.000
Metal Tile	Aluminum	205.000
Metal Tile	Thermium	220.000

Tips

• When cooling or heating an area it's better to run pipes through tiles than through atmosphere. In both cases the equation for "Building and the cells it occupies" is used which multiplies both Thermal conductivities, and in general, gases have a much lower thermal conductivity than liquids, which have lower conductivity than solids.
  • However, if drastic cooling is desired, then Steam Turbines and Aquatuners will have to be involved, which means a cavity filled with Steam will have to be used.
• Since Insulated Tiles have a factor of 1/16256, and pipes a factor of 1/32, much less heat is transferred if a regular pipe goes through an insulated tile than when an insulated pipe goes through a regular Tile. Though, of course, insulating both has an even better insulating effect.
• Even though Insulite has a lower thermal conductivity than any Insulated Tile, the change in formula from ${\color {Green}k_{geom}}$ to ${\color {Cerulean}k_{lowest}}$ makes insulated tiles much more practical insulators than a regular Tile made from Insulite. Indeed, they are so good that even using regular rock is often sufficient to shut down heat transfer completely, or to practically unnoticeable levels.

References

https://forums.kleientertainment.com/forums/topic/84275-decrypting-heat-transfer/