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arxiv: 2604.11441 · v1 · submitted 2026-04-13 · ❄️ cond-mat.stat-mech

Optimization of cooling power of a thermoelectric refrigerator: A unified approach

Pith reviewed 2026-05-10 15:16 UTC · model grok-4.3

classification ❄️ cond-mat.stat-mech
keywords thermoelectric refrigeratorcooling power optimizationcoefficient of performanceinternal and external irreversibilitiesfigure of meritendoreversible modelexoreversible modelunified framework
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The pith

A unified model allows optimization of cooling power in thermoelectric refrigerators by balancing internal and external irreversibilities.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper unifies the endoreversible and exoreversible approximations for thermoelectric refrigerators under a single steady-state framework. It shows that cooling power becomes optimizable when external thermal conductances are large but finite, even though the pure endoreversible case with Newtonian heat transfer does not permit optimization. The authors derive an explicit expression for the coefficient of performance that incorporates both types of irreversibility through the thermoelectric figure of merit and the ratio of internal to external conductances. This expression recovers the two limiting models as special cases and indicates that realistic single-stage devices achieve COP values below one-half for small temperature differences.

Core claim

In the steady-state formalism for a thermoelectric refrigerator, the cooling power which cannot be optimized under the pure endoreversible model with Newtonian heat transfer becomes optimizable once external thermal conductances are taken as large but finite. Extending the analysis to include both internal and external irreversibilities produces a closed-form coefficient of performance that depends on the thermoelectric figure of merit and the ratio of internal to external thermal conductances; the same expression reproduces the endoreversible and exoreversible limits as special cases.

What carries the argument

The ratio of internal to external thermal conductances together with the thermoelectric figure of merit, which together yield an explicit COP formula that unifies the two irreversibility regimes.

If this is right

  • The combined irreversibilities reduce the COP to values below one-half for small temperature differences.
  • The expression supplies realistic numerical estimates for the performance of single-stage thermoelectric refrigerators.
  • The endoreversible and exoreversible models appear as exact limiting cases of the unified formula.
  • Cooling-power optimization is possible once external conductances are treated as large but finite.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Engineers could adjust the internal-to-external conductance ratio to improve COP in practical cooler designs.
  • The same unification technique might be applied to other irreversible heat devices that mix internal and external losses.
  • For larger temperature spans, experiments could test how far the linear Newtonian assumption must be relaxed before the closed-form result breaks down.

Load-bearing premise

The analysis assumes Newtonian heat transfer between the device and the reservoirs together with steady-state operation; if heat transfer deviates strongly from linear dependence on temperature difference the optimization and closed-form COP no longer hold.

What would settle it

Measure the actual coefficient of performance of a single-stage thermoelectric refrigerator whose internal and external thermal conductances are independently known, at small temperature differences, and check whether the measured value agrees with the formula that uses the figure of merit and the conductance ratio.

Figures

Figures reproduced from arXiv: 2604.11441 by Rajeshree Chakraborty, Ramandeep S. Johal.

Figure 1
Figure 1. Figure 1: FIG. 1 [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2 [PITH_FULL_IMAGE:figures/full_fig_p005_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: It is observed that the exoreversible model gives a higher COP than the endoreversible model, both of them leading to a value 1/2 for large ϵC or small temperature differences. On the other hand, the presence of both internal and external irreversibilities lowers the COP further. In this case, the limit of small temperature differences is dominated by the value: ϵ ∗ → 1 6 + p 1 − 2kz (1 − 2k(z + 3)) 3(1 + … view at source ↗
read the original abstract

We analyze the steady-state formalism for optimizing the cooling power of a thermoelectric refrigerator (TER), unifying the endoreversible and exoreversible approximations within one framework. Although the cooling power is non-optimizable within the endoreversible model based on Newtonian heat-transfer law, we show that the issue can be circumvented in the near-reversible regime where the external thermal conductances are large, but finite. We extend this analysis to optimize the cooling power in the presence of both internal and external irreversibilities and derive a closed-form expression for the coefficient of performance (COP) that depends on the thermoelectric figure of merit and the ratio of internal to external thermal conductances. The model reproduces the endoreversible and the exoreversible limits as special cases. We conclude that for small temperature differences, the combined irreversibilities reduce the COP to values below 1/2, which aligns with the observed performance of the single-stage TER, and can provide realistic estimates for the COP.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

0 major / 3 minor

Summary. The manuscript develops a unified steady-state model for thermoelectric refrigerators incorporating both internal irreversibilities (Joule heating and Fourier conduction) and external irreversibilities (finite-rate Newtonian heat transfer to the reservoirs). By maximizing cooling power with respect to electric current, the authors derive a closed-form expression for the coefficient of performance (COP) that depends only on the thermoelectric figure of merit ZT and the ratio of internal to external thermal conductances; this expression recovers the endoreversible and exoreversible limits as special cases. The work concludes that combined irreversibilities reduce the COP below 1/2 for small temperature differences, consistent with observed single-stage TER performance.

Significance. If the derivation holds, the closed-form COP provides a practical, analytically tractable tool that unifies prior approximations and yields realistic performance estimates without additional fitting parameters beyond ZT and the conductance ratio. The recovery of known limits and the explicit dependence on design parameters are strengths that could guide device optimization in thermoelectric cooling applications.

minor comments (3)
  1. The abstract states that cooling power is 'non-optimizable' in the pure endoreversible limit but can be circumvented in the 'near-reversible regime'; the main text should explicitly demonstrate this by showing the relevant derivative with respect to current (or the resulting independence) and define the near-reversible regime quantitatively (e.g., via a specific inequality on the conductance ratio).
  2. The conclusion that combined irreversibilities reduce COP 'below 1/2' for small temperature differences should be accompanied by a brief numerical example or plot illustrating the value of the derived COP expression at representative small ΔT and typical ZT values.
  3. Notation for the internal-to-external conductance ratio should be introduced with a clear symbol (e.g., r = K_int/K_ext) at first use and used consistently thereafter.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the supportive summary and significance assessment of our manuscript. The recommendation for minor revision is noted. However, no specific major comments were provided in the report, so we have no individual points to address. We are pleased that the unified model, closed-form COP, and recovery of known limits were viewed positively as a practical tool for thermoelectric cooling optimization.

Circularity Check

0 steps flagged

No significant circularity identified

full rationale

The derivation proceeds from the standard steady-state energy-balance equations for a thermoelectric refrigerator that include Joule heating, Fourier conduction (internal irreversibilities), and finite Newtonian heat-exchange conductances at the hot and cold sides (external irreversibilities). Cooling power is maximized with respect to electric current; the resulting optimal current is substituted into the COP definition to obtain an explicit algebraic expression in terms of the material figure of merit ZT (an external experimental input) and the conductance ratio (a design parameter). The expression recovers the endoreversible and exoreversible limits by construction when the appropriate conductance ratio tends to zero or infinity, but this is a mathematical limit check rather than a definitional reduction. No fitted parameter is renamed as a prediction, no self-citation supplies a load-bearing uniqueness theorem, and the central closed-form result is obtained directly from the model equations without circular substitution.

Axiom & Free-Parameter Ledger

2 free parameters · 2 axioms · 0 invented entities

The central claim rests on the Newtonian heat-transfer law for external exchange, the steady-state condition, and the use of the thermoelectric figure of merit and internal-to-external conductance ratio as inputs; no new entities are postulated.

free parameters (2)
  • thermoelectric figure of merit
    Material property taken as an input from experiment or prior measurement
  • ratio of internal to external thermal conductances
    Device-specific parameter characterizing relative strength of internal versus external heat leaks
axioms (2)
  • domain assumption Newtonian heat-transfer law
    Heat flow between device and reservoirs assumed proportional to temperature difference
  • domain assumption Steady-state operation
    All temperatures and currents treated as constant in time for the formalism

pith-pipeline@v0.9.0 · 5469 in / 1452 out tokens · 48656 ms · 2026-05-10T15:16:55.892754+00:00 · methodology

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Works this paper leans on

24 extracted references · 24 canonical work pages

  1. [1]

    Velasco, J

    S. Velasco, J. M. M. Roco, A. Medina, and A. C. Hern´ andez, New performance bounds for a finite-time Carnot refrigerator, Phys. Rev. Lett.78, 3241 (1997)

  2. [2]

    Velasco, J

    S. Velasco, J. M. M. Roco, A. Medina, and A. Calvo Hern´ andez, Irreversible refrigerators under per-unit-time coefficient of performance optimization, Applied Physics Letters71, 1130 (1997)

  3. [3]

    Izumida, K

    Y. Izumida, K. Okuda, A. Calvo Hern´ andez, and J. M. M. Roco, Coefficient of performance under optimized figure of merit in minimally nonlinear irreversible refrigerator, Europhysics Letters101, 10005 (2013)

  4. [4]

    Long and W

    R. Long and W. Liu, Coefficient of performance and its bounds with the figure of merit for a general refrigerator, Physica Scripta90, 025207 (2015)

  5. [5]

    de Tomas, J

    C. de Tomas, J. M. M. Roco, A. C. Hern´ andez, Y. Wang, and Z. C. Tu, Low-dissipation heat devices: Unified trade-off optimization and bounds, Phys. Rev. E87, 012105 (2013)

  6. [6]

    Yan and J

    Z. Yan and J. Chen, A class of irreversible Carnot refrigeration cycles with a general heat transfer law, Journal of Physics D: Applied Physics23, 136 (1990)

  7. [7]

    F. L. Curzon and B. Ahlborn, Efficiency of a Carnot engine at maximum power output, American Journal of Physics43, 22 (1975). 9

  8. [8]

    Schmiedl and U

    T. Schmiedl and U. Seifert, Efficiency at maximum power: An analytically solvable model for stochastic heat engines, Europhysics Letters81, 20003 (2007)

  9. [9]

    D. C. Agrawal and V. J. Menon, The thermoelectric generator as an endoreversible Carnot engine, Journal of Physics D: Applied Physics30, 357 (1997)

  10. [10]

    M. Chen, L. Rosendahl, I. Bach, T. Condra, and J. Pedersen, Irreversible transfer processes of thermoelectric generators, American Journal of Physics75, 815 (2007)

  11. [11]

    J. Kaur, R. S. Johal, and M. Feidt, Thermoelectric generator in endoreversible approximation: The effect of heat-transfer law under finite physical dimensions constraint, Phys. Rev. E105, 034122 (2022)

  12. [12]

    Angulo-Brown, An ecological optimization criterion for finite-time heat engines, Journal of Applied Physics 69, 7465 (1991)

    F. Angulo-Brown, An ecological optimization criterion for finite-time heat engines, Journal of Applied Physics 69, 7465 (1991)

  13. [13]

    Chen, The maximum power output and maximum efficiency of an irreversible Carnot heat engine, Journal of Physics D: Applied Physics27, 1144 (1994)

    J. Chen, The maximum power output and maximum efficiency of an irreversible Carnot heat engine, Journal of Physics D: Applied Physics27, 1144 (1994)

  14. [14]

    A., Thermal optimization of Curzon-Ahlborn heat engines operating under some generalized efficient power regimes, Eur

    Levario-Medina, S., Valencia-Ortega, G., and Arias-Hernandez, L. A., Thermal optimization of Curzon-Ahlborn heat engines operating under some generalized efficient power regimes, Eur. Phys. J. Plus134, 348 (2019)

  15. [15]

    Apertet, H

    Y. Apertet, H. Ouerdane, A. Michot, C. Goupil, and P. Lecoeur, On the efficiency at maximum cooling power, Europhysics Letters103, 40001 (2013)

  16. [16]

    D. C. Agrawal and V. J. Menon, Performance of a Carnot refrigerator at maximum cooling power, Journal of Physics A: Mathematical and General23, 5319 (1990)

  17. [17]

    A. E. Allahverdyan, K. Hovhannisyan, and G. Mahler, Optimal refrigerator, Phys. Rev. E81, 051129 (2010)

  18. [18]

    de Tom´ as, A

    C. de Tom´ as, A. C. Hern´ andez, and J. M. M. Roco, Optimal low symmetric dissipation Carnot engines and refrigerators, Phys. Rev. E85, 010104 (2012)

  19. [19]

    X. G. Luo, N. Liu, and J. Z. He, Optimum analysis of a brownian refrigerator, Phys. Rev. E87, 022139 (2013)

  20. [20]

    Parrott and A

    J. Parrott and A. Penn, The design theory of thermoelectric cooling elements and units, Solid-State Electronics 3, 91 (1961)

  21. [21]

    Apertet, H

    Y. Apertet, H. Ouerdane, C. Goupil, and P. Lecoeur, From local force-flux relationships to internal dissipations and their impact on heat engine performance: The illustrative case of a thermoelectric generator, Phys. Rev. E88, 022137 (2013)

  22. [22]

    Chakraborty and R

    R. Chakraborty and R. S. Johal, Optimal performance of thermoelectric devices with small external irre- versibility, Phys. Rev. E112, 034110 (2025)

  23. [23]

    Min and D

    G. Min and D. M. Rowe, Improved model for calculating the coefficient of performance of a Peltier module, Energy Conversion and Management41, 163 (2000)

  24. [24]

    G¨ ok¸ cek and F

    M. G¨ ok¸ cek and F. S ¸ahin, Experimental performance investigation of minichannel water cooled-thermoelectric refrigerator, Case Studies in Thermal Engineering10, 54 (2017)