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Phase II Final Report - NASA's Institute for Advanced Concepts

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Planetary Exploration Using Biomimetics<br />

An Entomopter <strong>for</strong> Flight on Mars<br />

The C rating is a gauge of the current producing capacity and discharge time of the battery. At<br />

1C the 930 mAh battery would produce 930 mA <strong>for</strong> 1 hour. At C/5 it would produce 186 mA <strong>for</strong><br />

5 hours, and at 2C it would produce 1,860 mA <strong>for</strong> 0.5 hour. It should be noted that as the discharge<br />

time decreases, the overall capacity of the battery will also decrease.<br />

Based on the estimated power consumption of the various systems, shown in Figures 3-168<br />

through 3-170, the maximum power consumption is 3.5 W, and the total energy consumption <strong>for</strong><br />

a mission cycle is 3.1 W-h. An estimate of the required battery capacity is 100% of the total<br />

energy required <strong>for</strong> the mission. This battery capacity allows the battery to provide power to the<br />

systems when the array is offline (shadowed). This also provides a redundancy <strong>for</strong> supplying<br />

sufficient power in the event the array fails. This requires a battery with 3.1 W-h of capacity.<br />

Based on the battery data listed in Table 3-25, the battery mass would be 0.023 kg.<br />

The overall system mass estimate <strong>for</strong> the array/battery system is listed in Table 3-26.<br />

Table 3-26: PV/Battery System Mass Estimate<br />

System Component<br />

Mass (kg)<br />

Solar Array 0.014<br />

Battery 0.023<br />

Contingency (50% <strong>for</strong> wiring, electronics, etc.) 0.037<br />

Total System Mass 0.0555<br />

It should be noted that the system mass shown in Table 3-26 represents values based on state-ofthe-art<br />

components. With future advancements in these components, this may be significantly<br />

reduced. Also any variation in the assumptions used to generate these numbers will also greatly<br />

affect these results.<br />

3.6.7 Thermoelectric Power Generation<br />

The basic principle behind a thermoelectric power generator is that if two different metals, semimetals,<br />

or semiconductors are joined at one end and separated along their length, a current will<br />

be produced in each metal strip as long as there is a temperature difference between each side of<br />

the junction. The configuration of a thermoelectric power generator is shown in Figure 3-181.<br />

The heat source provides a high-temperature source from which heat will flow through the converter.<br />

For the Entomopter application, heat can be generated either through the combustion of<br />

the propellant or from an isotope heat source. A heat sink must also be used to dissipate the<br />

excess heat and maintain the cold side of the thermoelectric generator at a temperature below<br />

that of the hot side. It is this temperature difference that produces the direct current electrical<br />

power. Thermoelectric generators can be made <strong>for</strong> power levels ranging anywhere from 10 -6 W<br />

to 10 2 W. Semiconductor material is by far the best choice <strong>for</strong> the construction of a thermoelectric<br />

generator. These materials can presently achieve efficiencies on the order of 5% to 10%.<br />

220<br />

<strong>Phase</strong> <strong>II</strong> <strong>Final</strong> <strong>Report</strong>

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