Abstract:The first systematic comparison between Swarm-C accelerometer-derived thermospheric density and both empirical and physics-based model results using multiple model performance metrics is presented. This comparison is performed at the satellite's high temporal 10-s resolution, which provides a meaningful evaluation of the models' fidelity for orbit prediction and other space weather forecasting applications. The comparison against the physical model is influenced by the specification of the lower atmospheric fo… Show more
“…Following the conclusions in Kodikara et al (2018), one could expect the seasonal monthly mean results presented above to not change much based on the Weimer (2005) or Heelis et al (1982) ionosphere convection models. Nevertheless, an extended comparison with different high-latitude forcing methods during storm/quiet times may help to quantify the sensitivity of -T synchrony in the high latitudes even further.…”
Section: Discussionmentioning
confidence: 68%
“…Kodikara et al () discussed that, compared to accelerometer‐derived densities, the performance of both Weimer () and Heelis et al () ionosphere convection models are comparable under 2014/2015 geophysical conditions. Both Kodikara et al () and Wu et al () provided examples of the Weimer () model outperforming Heelis et al () model during storm times. While the type of ionosphere convection model is not expected to influence the seasonal, monthly mean results much, it may have an impact on the storm time results.…”
Section: Discussionmentioning
confidence: 99%
“…TIE-GCM's ability to reproduce the thermospheric density and temperature dynamics has been validated in some studies (see Emmert, 2015;Maute, 2017;Qian et al, 2014;Shim et al, 2012, and references therein). In particular, Kodikara et al (2018) validated the TIE-GCM version 2.0 using accelerometer-derived density data for 2014/2015, which is part of the period considered in this analysis. Below is a comparison of ground measurements of thermosphere temperature from multiple stations with TIE-GCM.…”
Section: Appendix A: Model Verification: a Comparison With Temperaturmentioning
The paper presents a detailed analysis of the density‐temperature (ρ‐T) synchrony in the thermosphere using a hydrostatic general circulation model. The numerical models in general offer not only great potential for forecasting the transient response of the thermosphere but also are excellent tools for understanding the driving mechanisms of various thermospheric trends and features. This study investigates and isolates the dependency of the ρ‐T synchrony on the season, altitude, space weather, high‐latitude electrodynamics, and the lower atmospheric tidal spectrum. The results demonstrate that the previously reported ρ‐T synchrony begins around 300‐km (350‐km) altitude at the equator (high latitudes). The effect of the lower atmospheric tidal spectrum on the ρ‐T synchrony patterns seems to be only marginal and more noticeable during the equinox months. The study demonstrates that the ρ‐T phase lag is larger in the high latitudes of the summer hemisphere and evolves through the day and is attributable to ion drag and temperature fluctuations via soft particle precipitation. The study provides physical insights into how the winds contribute to the ρ‐T synchrony. In addition, the results show that geomagnetic activity contributes significantly to the ρ‐T synchrony; the underlying mechanism may be related to temperature enhancements in the high latitudes via Joule heating and associated nonlinear interactions. While the ρ‐T phase lags attributable to different solar activity levels are modest, the solar heating is the primary source that maintains the ρ‐T synchrony in the low/middle latitudes via upward propagating thermal tides.
“…Following the conclusions in Kodikara et al (2018), one could expect the seasonal monthly mean results presented above to not change much based on the Weimer (2005) or Heelis et al (1982) ionosphere convection models. Nevertheless, an extended comparison with different high-latitude forcing methods during storm/quiet times may help to quantify the sensitivity of -T synchrony in the high latitudes even further.…”
Section: Discussionmentioning
confidence: 68%
“…Kodikara et al () discussed that, compared to accelerometer‐derived densities, the performance of both Weimer () and Heelis et al () ionosphere convection models are comparable under 2014/2015 geophysical conditions. Both Kodikara et al () and Wu et al () provided examples of the Weimer () model outperforming Heelis et al () model during storm times. While the type of ionosphere convection model is not expected to influence the seasonal, monthly mean results much, it may have an impact on the storm time results.…”
Section: Discussionmentioning
confidence: 99%
“…TIE-GCM's ability to reproduce the thermospheric density and temperature dynamics has been validated in some studies (see Emmert, 2015;Maute, 2017;Qian et al, 2014;Shim et al, 2012, and references therein). In particular, Kodikara et al (2018) validated the TIE-GCM version 2.0 using accelerometer-derived density data for 2014/2015, which is part of the period considered in this analysis. Below is a comparison of ground measurements of thermosphere temperature from multiple stations with TIE-GCM.…”
Section: Appendix A: Model Verification: a Comparison With Temperaturmentioning
The paper presents a detailed analysis of the density‐temperature (ρ‐T) synchrony in the thermosphere using a hydrostatic general circulation model. The numerical models in general offer not only great potential for forecasting the transient response of the thermosphere but also are excellent tools for understanding the driving mechanisms of various thermospheric trends and features. This study investigates and isolates the dependency of the ρ‐T synchrony on the season, altitude, space weather, high‐latitude electrodynamics, and the lower atmospheric tidal spectrum. The results demonstrate that the previously reported ρ‐T synchrony begins around 300‐km (350‐km) altitude at the equator (high latitudes). The effect of the lower atmospheric tidal spectrum on the ρ‐T synchrony patterns seems to be only marginal and more noticeable during the equinox months. The study demonstrates that the ρ‐T phase lag is larger in the high latitudes of the summer hemisphere and evolves through the day and is attributable to ion drag and temperature fluctuations via soft particle precipitation. The study provides physical insights into how the winds contribute to the ρ‐T synchrony. In addition, the results show that geomagnetic activity contributes significantly to the ρ‐T synchrony; the underlying mechanism may be related to temperature enhancements in the high latitudes via Joule heating and associated nonlinear interactions. While the ρ‐T phase lags attributable to different solar activity levels are modest, the solar heating is the primary source that maintains the ρ‐T synchrony in the low/middle latitudes via upward propagating thermal tides.
“…The Challenging Micro-Satellite Payload (CHAMP) and Gravity Recovery and Climate Experiment satellites are the most used satellites for the investigations of the neutral density and the associated atmospheric drag acting on satellites (Anderson et al, 2009;Bruinsma, 2015;Bruinsma & Forbes, 2010;Bruinsma et al, 2018;Huang et al, 2014;Liu et al, 2011;Picone et al, 2002;Xu et al, 2011). Recently, data from Swarm constellation has also been employed to derive the thermospheric neutral densities (Kodikara et al, 2018;Siemes et al, 2016;Zesta & Huang, 2016). In this kind of approach, the densities are calculated from the accelerometers on the spacecraft (Sutton et al, 2005).…”
Section: Introductionmentioning
confidence: 99%
“…Several metrics are employed to assess the model performances. For the neutral density studies, the most used metrics are the mean absolute error (MAE), bias (B), correlation (R), root mean square error (RMSE), standard deviation (Std), prediction efficiency (PE), ratio of maximum and ratio of average (Bruinsma, 2015;Elvidge et al, 2014Elvidge et al, , 2016Emmert et al, 2017;Kodikara et al, 2018;Pardini et al, 2012;Shim et al, 2012), and the version of the metrics in log space (Bruinsma et al, 2018;Picone et al, 2002;Sutton, 2018). Each of these metrics has advantages and disadvantages (Hyndman et al, 2006;Shcherbakov et al, 2013).…”
Accurate determination of thermospheric neutral density holds crucial importance for satellite drag calculations. The problem is twofold and involves the correct estimation of the quiet time climatology and storm time variations. In this work, neutral density estimations from two empirical and three physics‐based models of the ionosphere‐thermosphere are compared with the neutral densities along the Challenging Micro‐Satellite Payload satellite track for six geomagnetic storms. Storm time variations are extracted from neutral density by (1) subtracting the mean difference between model and observation (bias), (2) setting climatological variations to zero, and (3) multiplying model data with the quiet time ratio between the model and observation. Several metrics are employed to evaluate the model performances. We find that the removal of bias or climatology reveals actual performance of the model in simulating the storm time variations. When bias is removed, depending on event and model, storm time errors in neutral density can decrease by an amount of 113% or can increase by an amount of 12% with respect to error in models with quiet time bias. It is shown that using only average and maximum values of neutral density to determine the model performances can be misleading since a model can estimate the averages fairly well but may not capture the maximum value or vice versa. Since each of the metrics used for determining model performances provides different aspects of the error, among these, we suggest employing mean absolute error, prediction efficiency, and normalized root mean square error together as a standard set of metrics for the neutral density.
The paper presents experiments of driving a physics-based thermosphere model by assimilating electron density (Ne) and temperature (T n) data using the ensemble adjustment Kalman filter (EAKF) technique. This study not only helps to gauge the accuracy of the assimilation, to explain the inherent model bias, and to understand the limitations of the framework, but it also establishes EAKF as a viable technique in the presence of realistic data assimilation scenarios to forecast the highly dynamical thermosphere.The results from perfect model scenarios show that data assimilation changes and, more often than not, improves the model state. Data from Swarm-A, Swarm-C, CHAMP, and GRACE-A are used to validate the resulting analysis states. The independent validation results show that the Ne-guided thermosphere state does not outperform the model state without data assimilation along the considered orbits. This may be due to the limited number of bonafide Ne profiles available for the thermosphere specification tasks in the experiments. More importantly, the results show that the Ne-guided thermosphere state does not deteriorate much in performance during geomagnetic storm time. The results reveal a few challenges of using Ne profiles in a hypothetical operational data assimilation exercise. In terms of estimating the mass density along the orbits of both CHAMP and GRACE-A satellites, the experiment with assimilating T n shows more promise over Ne.The results show that the improvement gained in the overall forecasted thermosphere state is better during solar minimum compared to that of solar maximum. These results also provide insights into the biases inherent in the physics-based model. The systematic biases that the paper highlight could be an indication that the specification of plasma-neutral interactions in the model needs further adjustments.
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