Thermoelectric Materials and Devices

🔋Thermoelectric Materials and Devices Unit 13 – Thermoelectric Energy Harvesting Applications

Thermoelectric energy harvesting converts waste heat into electricity using the Seebeck effect. This process relies on materials with high electrical conductivity, low thermal conductivity, and a large Seebeck coefficient. Efficiency is quantified by the figure of merit (ZT), with higher values indicating better performance. Applications range from waste heat recovery in industrial processes to powering space missions and wearable electronics. Challenges include low conversion efficiency, material scarcity, and thermal management issues. Future research focuses on nanostructured materials, new material systems, and improved manufacturing techniques to enhance performance and expand applications.

Key Concepts and Principles

  • Thermoelectric energy harvesting converts waste heat into usable electrical energy based on the Seebeck effect
  • Seebeck effect generates a voltage when a temperature gradient is applied across a thermoelectric material
  • Peltier effect is the reverse process where applying a voltage creates a temperature difference used for cooling applications
  • Figure of merit (ZTZT) quantifies the efficiency of a thermoelectric material higher ZTZT values indicate better performance
  • Thermoelectric materials require high electrical conductivity, low thermal conductivity, and a large Seebeck coefficient to maximize efficiency
    • Balancing these properties is challenging as they are often interdependent
  • Carnot efficiency sets the upper limit for thermoelectric energy conversion determined by the hot and cold side temperatures
  • Thermoelectric generators (TEGs) consist of multiple thermoelectric couples connected electrically in series and thermally in parallel

Thermoelectric Materials Overview

  • Ideal thermoelectric materials exhibit a combination of high electrical conductivity, low thermal conductivity, and a large Seebeck coefficient
  • Common thermoelectric materials include bismuth telluride (Bi2Te3Bi_2Te_3), lead telluride (PbTePbTe), and silicon germanium (SiGeSiGe) alloys
    • Bi2Te3Bi_2Te_3 is widely used for near-room-temperature applications (refrigeration, waste heat recovery)
    • PbTePbTe and SiGeSiGe are suitable for mid to high-temperature applications (automotive, industrial waste heat recovery)
  • Nanostructuring techniques (quantum dots, superlattices) can enhance thermoelectric properties by reducing thermal conductivity through phonon scattering
  • Doping with impurities or alloying can optimize carrier concentration and improve electrical conductivity
  • Organic and polymer-based thermoelectric materials offer advantages such as flexibility, low cost, and ease of processing
    • Examples include PEDOT:PSS and carbon nanotube composites
  • Skutterudites, clathrates, and half-Heusler alloys are promising high-temperature thermoelectric materials with complex crystal structures

Device Structure and Components

  • Thermoelectric devices consist of multiple thermoelectric couples connected electrically in series and thermally in parallel
  • Each thermoelectric couple comprises a p-type and n-type semiconductor leg connected by metallic interconnects
  • P-type legs have positive Seebeck coefficients and conduct holes, while n-type legs have negative Seebeck coefficients and conduct electrons
  • Ceramic substrates provide electrical insulation and structural support for the thermoelectric legs
  • Thermal interfaces (heat exchangers, heat spreaders) facilitate efficient heat transfer between the thermoelectric device and the heat source/sink
  • Electrical contacts and interconnects are made of highly conductive materials (copper, gold) to minimize electrical losses
  • Protective coatings and encapsulation ensure device stability and prevent oxidation or degradation of thermoelectric materials

Energy Conversion Mechanisms

  • Thermoelectric energy conversion relies on the Seebeck effect, where a temperature gradient induces a voltage across a thermoelectric material
  • Charge carriers (electrons in n-type, holes in p-type) diffuse from the hot side to the cold side, creating a net current flow
  • The generated voltage is proportional to the temperature difference and the Seebeck coefficient of the material (V=αΔTV = \alpha \Delta T)
  • In a thermoelectric generator, the temperature gradient drives the current through an external load, producing useful electrical power
  • The Peltier effect, the reverse of the Seebeck effect, is used for thermoelectric cooling and temperature control applications
    • Applying a current causes heat absorption at one junction and heat release at the other, creating a temperature difference
  • Thomson effect describes the reversible heat absorption or release in a single conductor with a temperature gradient and an electric current
  • Joule heating, an irreversible effect, occurs due to electrical resistance and reduces the overall efficiency of thermoelectric devices

Performance Metrics and Efficiency

  • Efficiency of a thermoelectric device depends on the material properties, temperature gradient, and device geometry
  • Figure of merit (ZTZT) is a dimensionless quantity that characterizes the performance of a thermoelectric material
    • ZT=(α2σ/κ)TZT = (\alpha^2 \sigma / \kappa) T, where α\alpha is the Seebeck coefficient, σ\sigma is electrical conductivity, κ\kappa is thermal conductivity, and TT is the absolute temperature
  • Higher ZTZT values indicate better thermoelectric performance, with values above 1 considered suitable for practical applications
  • Power factor (α2σ\alpha^2 \sigma) is another metric that focuses on the electrical properties of a thermoelectric material
  • Thermoelectric conversion efficiency (η\eta) is the ratio of the electrical power output to the heat input
    • η=THTCTH1+ZT11+ZT+TCTH\eta = \frac{T_H - T_C}{T_H} \frac{\sqrt{1 + ZT} - 1}{\sqrt{1 + ZT} + \frac{T_C}{T_H}}, where THT_H and TCT_C are the hot and cold side temperatures, respectively
  • Carnot efficiency sets the upper limit for thermoelectric conversion efficiency, which is lower than the ideal Carnot limit due to irreversible losses
  • Thermal and electrical contact resistances, as well as parasitic heat losses, can significantly reduce the overall device efficiency

Applications and Use Cases

  • Waste heat recovery is a primary application of thermoelectric energy harvesting, converting unused heat into useful electricity
    • Examples include industrial processes, automotive exhaust systems, and power plants
  • Space applications utilize radioisotope thermoelectric generators (RTGs) for long-duration power supply in remote locations
    • RTGs convert heat from radioactive decay into electricity and have been used in various space missions (Voyager, Cassini)
  • Portable and wearable electronics can benefit from thermoelectric energy harvesting, using body heat to power devices
    • Thermoelectric generators can be integrated into clothing, watches, or other accessories
  • Thermoelectric cooling modules (Peltier coolers) are used for temperature control in applications such as electronics cooling, medical devices, and scientific instruments
    • Advantages include compact size, no moving parts, and precise temperature control
  • Thermoelectric air conditioning and refrigeration systems offer an alternative to traditional vapor-compression systems, with potential for higher efficiency and reduced environmental impact
  • Remote sensing and wireless sensor networks can utilize thermoelectric energy harvesting to power sensors in hard-to-reach or inaccessible locations

Challenges and Limitations

  • Low conversion efficiency of thermoelectric materials compared to other energy conversion technologies (solar, mechanical)
    • Current high-performance materials have ZTZT values around 1-2, limiting practical efficiency to 5-10%
  • Scarcity and high cost of some thermoelectric materials (tellurium, germanium) hinder widespread adoption
    • Developing cost-effective and abundant alternative materials is an ongoing challenge
  • Thermal management and heat transfer issues can limit the performance of thermoelectric devices
    • Efficient heat exchangers and thermal interfaces are crucial for maintaining the required temperature gradient
  • Electrical contact resistance and compatibility between thermoelectric materials and electrodes can cause performance degradation over time
  • Mechanical stresses due to thermal expansion mismatch can lead to device failure, especially in high-temperature applications
  • Optimizing thermoelectric materials often involves trade-offs between conflicting properties (electrical conductivity, thermal conductivity, Seebeck coefficient)
    • Nanostructuring and complex material design are needed to decouple these properties
  • Nanostructured and complex thermoelectric materials with enhanced ZTZT values through phonon scattering and energy filtering
    • Examples include quantum dots, superlattices, and hierarchical structures
  • Exploration of new material systems and compositions, such as organic semiconductors, metal-organic frameworks (MOFs), and hybrid materials
  • Development of high-temperature thermoelectric materials for waste heat recovery in industrial processes and power generation
    • Focus on materials with high thermal stability and mechanical robustness
  • Flexible and printable thermoelectric devices for wearable and conformable applications
    • Investigating novel fabrication techniques like 3D printing and roll-to-roll processing
  • Integration of thermoelectric devices with other energy harvesting technologies (photovoltaics, piezoelectrics) for enhanced performance and functionality
  • Computational materials design and machine learning approaches to accelerate the discovery and optimization of new thermoelectric materials
  • Addressing scalability, manufacturing, and system-level integration challenges for widespread deployment of thermoelectric energy harvesting technologies


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© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.