{"title":"Quantitative analysis of MMRTG power decay due to thermal inventory loss","authors":"Haoqian Qiu, Tailin Li, Yingzeng Zhang, Youhong Liu, Qingpei Xiang","doi":"10.1016/j.nucana.2026.100218","DOIUrl":null,"url":null,"abstract":"<div><div>The Multi-Mission Radioisotope Thermoelectric Generator (MMRTG) experiences electrical power decline due to Pu-238 decay and thermoelectric (TE) degradation. In this work, the contribution of Pu-238 decay is isolated and quantified by modeling thermal inventory loss as the sole aging mechanism. A full-scale three-dimensional coupled thermal-electrical finite-element model of the MMRTG is constructed and evaluated over a 17-year operating period, with temperature-dependent thermoelectric material properties retained in each quasi-steady solution, but with no time-dependent aging or degradation of thermoelectric properties, contact resistance, or radiative properties. The results indicate that fuel decay alone reduces the electrical output from approximately 124 W<sub>e</sub> at beginning-of-life to ∼98.4 W<sub>e</sub> after 17 years, corresponding to a cumulative reduction of ∼20.6%. This behavior is equivalent to an effective compounded electrical decay rate of approximately 1.3-1.35%/yr, exceeding the commonly assumed 1.1%/yr decay-only approximation and leading to a ∼4% overprediction of end-of-life power in simplified models. Comparison of this decay-only reference with published Curiosity MMRTG flight telemetry enables a quantitative decomposition of total power loss. Over 17 years, approximately 45% (∼25 W<sub>e</sub>) of the cumulative loss is attributable to Pu-238 decay, while the remaining ∼55% (∼30 W<sub>e</sub>) appears as a lumped non-decay residual, interpreted here primarily as the consequence of thermoelectric aging together with other non-decay loss mechanisms and model–flight mismatch effects. The decay-only trajectory defined here provides a physically constrained reference for interpreting MMRTG performance data and separating unavoidable nuclear decay effects from thermoelectric aging.</div></div>","PeriodicalId":100965,"journal":{"name":"Nuclear Analysis","volume":"5 1","pages":"Article 100218"},"PeriodicalIF":0.0000,"publicationDate":"2026-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Analysis","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S2773183926000054","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2026/3/10 0:00:00","PubModel":"Epub","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The Multi-Mission Radioisotope Thermoelectric Generator (MMRTG) experiences electrical power decline due to Pu-238 decay and thermoelectric (TE) degradation. In this work, the contribution of Pu-238 decay is isolated and quantified by modeling thermal inventory loss as the sole aging mechanism. A full-scale three-dimensional coupled thermal-electrical finite-element model of the MMRTG is constructed and evaluated over a 17-year operating period, with temperature-dependent thermoelectric material properties retained in each quasi-steady solution, but with no time-dependent aging or degradation of thermoelectric properties, contact resistance, or radiative properties. The results indicate that fuel decay alone reduces the electrical output from approximately 124 We at beginning-of-life to ∼98.4 We after 17 years, corresponding to a cumulative reduction of ∼20.6%. This behavior is equivalent to an effective compounded electrical decay rate of approximately 1.3-1.35%/yr, exceeding the commonly assumed 1.1%/yr decay-only approximation and leading to a ∼4% overprediction of end-of-life power in simplified models. Comparison of this decay-only reference with published Curiosity MMRTG flight telemetry enables a quantitative decomposition of total power loss. Over 17 years, approximately 45% (∼25 We) of the cumulative loss is attributable to Pu-238 decay, while the remaining ∼55% (∼30 We) appears as a lumped non-decay residual, interpreted here primarily as the consequence of thermoelectric aging together with other non-decay loss mechanisms and model–flight mismatch effects. The decay-only trajectory defined here provides a physically constrained reference for interpreting MMRTG performance data and separating unavoidable nuclear decay effects from thermoelectric aging.