Materials, devices, and methods for resonant ambient thermal energy harvesting
The present disclosure is directed to materials, devices, and methods for resonant ambient thermal energy harvesting. Thermal energy can be harvested using thermoelectric resonators that capture and store ambient thermal fluctuations and convert the fluctuations to energy. The thermal resonators can include heat engines disposed between masses of varying sizes or diodes. The masses or diodes can be made of high and ultra-high effusivity materials to transfer thermal energy through the resonator and optimize power output. The masses or diodes of the resonator can be tuned to the dominant frequency of the temperature waveform to maximize the amount of energy being converted. The resonators can be added to existing structures to supply or generate power, and, in some embodiments, the structures themselves can be a mass of the thermal resonator. Methods for constructing and/or using such devices are also provided, as are methods for formulating ultra-high effusivity materials.
1. An energy harvesting system, comprising:
a first thermal mass having a first thermal diffusion time scale;
a second thermal mass having a second thermal diffusion time scale;
a heat engine disposed between the first thermal mass and the second thermal mass and configured to translate a spatial temperature difference between the first thermal mass and the second thermal mass into power;
a feedback loop that includes a microprocessor, the feedback loop being configured to tune at least one of the first thermal mass or the second thermal mass based on the respective first thermal diffusion time scale or the second thermal diffusion time scale such that the spatial temperature difference exists across the heat engine for power extraction,
wherein tuning based on at least one of the first thermal diffusion time scale or the second thermal diffusion time scale further comprises the system being configured to regulate a value of a geometry of at least one of the first thermal mass or the second thermal mass, or regulate a value of a thermal effusivity of at least one of the first thermal mass or the second thermal mass to create the spiral temperature difference between the first thermal mass and the second thermal mass.
2. The energy harvesting system of claim 1 , wherein at least one of the first thermal mass or the second thermal mass comprises one or more ultra-high thermal effusivity materials.
3. The energy harvesting system of claim 2 , wherein the one or more ultra-high thermal effusivity materials are disposed within a housing of the at least one of the first thermal mass or the second thermal mass such that the one or more ultra-high thermal effusivity materials substantially fills a volume of the housing.
4. The energy harvesting system of claim 2 , wherein the one or more ultra-high thermal effusivity materials comprise at least one of a Copper/Graphene/Octadecane phase-change material composite or a Nickel/Graphene/Octadecane phase-change material composite.
5. The energy harvesting system claim 1 , wherein each of the first diffusion time scale and the second diffusion time scale is configured to be controlled by a thermal effusivity of the respective first thermal mass and the second thermal mass, with the thermal effusivity being controlled by each of a thermal conductivity of the respective first thermal mass and second thermal mass, a density of the respective first thermal mass and second thermal mass, and a specific heat capacity of the respective first thermal mass and the second thermal mass.
6. The energy harvesting system of claim 1 , wherein each of the first diffusion time scale and the second diffusion time scale is configured to be controlled by a thermal effusivity of the respective first thermal mass and the second thermal mass, with the thermal effusivity being controlled by each of a thermal conductivity of the respective first thermal mass and second thermal mass, a density of the respective first thermal mass and second thermal mass, and a latent heat of the respective first thermal mass and the second thermal mass.
7. The energy harvesting system of claim 1 , wherein the heat engine is configured to be coupled to the second thermal mass in which the second thermal mass comprises a pre-existing object.
8. The energy harvesting system of claim 1 , wherein the at least one of the first thermal mass or the second thermal mass is configured to be tuned based or: (1) the respective first thermal diffusion time scale or the second thermal diffusion time scale: (2) at least one of a size of the at least one of the first thermal mass or the second thermal mass: or (3) a thermal effusivity of the at least one of the first thermal mass or the second thermal mass.
9. The energy harvesting system of claim 1 , wherein the at least one of the first thermal mass or the second thermal mass is configured to be tuned based on: (1) the respective first thermal diffusion time scale or the second thermal diffusion time scale: or (2) a temperature oscillation frequency of the at least one of the first thermal mass or the second thermal mass such that the power generated by the heat engine is optimized.
10. The energy harvesting system of claim 1 , further comprising:
a monitor in communication with the energy harvesting system and configured to acquire data related to at least one of the energy harvesting system or an environment surrounding the energy harvesting system; and
the microprocessor configured to adjust one or more parameters of at least one of the energy harvesting system or the environment surrounding the energy harvesting system in response to the data acquired by the monitor.
11. The energy harvesting system of claim 1 , wherein the system is configured to produce a dual polarity voltage output.
12. The system of claim 1 , wherein the at least one of the first and second thermal masses is configured to be tuned to a dominant frequency of a temperature waveform to capture temperature fluctuations that yield power outputs.
13. The system of claim 1 , wherein the feedback loop is further configured to adjust at least one of the first thermal mass or the second thermal mass to an ideal temperature oscillation frequency to optimize a value of the performance factor.