Heat pipe

Overview

For a heat pipe entity with one input connection on one side and one output connection on the opposite side, the temperature drop per segment is 1 + (P / 15) °C, where P is the power transmitted in megawatts (MW). Because heat exchangers must reach 500°C to generate steam and heat generators (for example, nuclear reactors) have a maximum of 1000°C, the maximum possible temperature difference between a heat source and a heat exchanger is 500°C. The maximum straight-line length L of heat pipe segments that can carry power P and still allow a heat exchanger to reach 500°C is therefore L = 500 / (1 + P/15). For example, a single nuclear reactor outputting 40 MW of thermal power to a single straight line of heat pipes can reach roughly 500 / (1 + 40/15) ≈ 136 heat pipe segments before the temperature has dropped too far to reach 500°C.
A nuclear reactor can itself act as a thermal conductor similar to a heat pipe whether or not it is fueled. In that role the reactor reduces temperature by 1 + (P / 387) °C per reactor entity, with P in MW; measured values indicate the denominator is approximately 386.847. Because a reactor occupies more tiles than a single heat pipe segment, one must compare it to multiple heat pipe segments in aggregate (for a typical reactor footprint that comparison is to about five lines of five heat pipes). Compared to equivalent length of heat pipe, a reactor reduces temperature less per tile: with near-zero transmitted power it reduces temperature about five times less than equivalent heat pipe tiles, and at very high transmitted power it reduces temperature nearly twenty-six times less. As an illustrative example, a straight line of 100 reactors (equivalent to 500 tiles) carrying 1 GW of thermal power will lower the temperature by roughly 360°C.
In the Space Age scenario on 
- Practical notes:
- Temperature drop per heat pipe increases with transmitted power; keep runs short or reduce power per line to preserve temperature.
- Use the formula L = 500 / (1 + P/15) to estimate maximum straight-run length from a heat source to a heat exchanger for given power.
- Consider using multiple parallel runs to split power and reduce per-segment temperature loss.
- When using reactors as conductors, account for their larger footprint and more favorable per-tile temperature loss at low power, but worse behavior at extremely high power.
Raw materials
| Reference | Count |
|---|---|
| Copper plate | 20 |
| Steel plate | 10 |
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