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RAP opportunity at Air Force Science and Technology Fellowship Program     AF STFP

Thermal Energy Storage

Location

Aerospace Systems Directorate, RQ/Control, Power and Thermal Management Division

opportunity location
13.30.10.B7102 Wright-Patterson AFB, OH 454337542

Advisers

name email phone
Quinn H. Leland quinn.leland@us.af.mil 937.255.3060

Description

Many high power density systems, including power electronics, lasers, and microwaves often operate cyclically and intermittently, generating enormous amounts of waste heat in a short period of time. Any thermal management system (TMS) designed for the peak thermal load will be over capacity on average, resulting in a larger, heavier TMS. An intermediate thermal energy storage system would store the peak thermal load and allow the heat to be rejected at an average rate, resulting in a smaller and lighter heat rejection system.

Many mechanisms are available to store heat at a near constant temperature, including latent heat of phase change (e.g., melting of solid like paraffins, vaporization of liquid like water and ammonia), chemical reactions (e.g., endothermic reaction of metal hydrides [MH]), and adsorptions (e.g., zeolite). Each approach has its advantages and disadvantages. The disadvantages pose a great challenge when they’re packaged into an airborne TES system. For example, paraffin based PCMs offer excellent operating temperature ranges, yet they have very low thermal conductivity and relatively low latent heat (heavy). Vaporization of water or ammonia offers a magnitude of higher mass energy density but the volume of the vapor is not feasible for airborne application (big). While the temperature range and mass energy density of metal hydrides are desirable, their endothermic reaction product, hydrogen gas, is not. Another severe application issue is the recharging of MH. Adsorption based TES also has problems with its operating temperature and recharging.

This research focuses on thermal energy storage materials and technologies. Specific technical goals include high thermal energy mass and volume density, high heat transfer rate (high effective thermal conductivity), and reversible (rechargeable TES) and near constant temperature (i.e., sensible heat approaches will not be considered).

 

Reference

Kota K, et al: Journal of Thermophysics and Heat Transfer (22)4: 2008

 

key words
Thermal energy storage; Phase change material; TES; TM; PCM; High rate thermal energy storage;

Eligibility

Citizenship:  Open to U.S. citizens
Level:  Open to Postdoctoral and Senior applicants

Stipend

Base Stipend Travel Allotment Supplementation
$95,000.00 $5,000.00

Experience Supplement:
Postdoctoral and Senior Associates will receive an appropriately higher stipend based on the number of years of experience past their PhD.

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