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==== 2. Methodological deep dive (statistics & error analysis) ==== ===== 2.1 Error propagation framework ===== Frank uses textbook propagation of uncertainty: * Generic single-step formula (his Eq. 3) and multistep propagation (Eq. 4) are standard: variance of a function of uncertain variables, with root-sum-square (RSS) behavior and covariance terms. Propagation_of_Error_and_the_Re… * For a sum of terms, he emphasises that uncertainty in the sum is RSS of individual uncertainties. Propagation_of_Error_and_the_Re… * He then treats each year’s tropospheric flux error as ±u₁, ±u₂, … and applies σTn=∑i=1nui2\sigma_{T_n} = \sqrt{\sum_{i=1}^n u_i^2}σTn=i=1∑nui2 (his Eq. 6). Propagation_of_Error_and_the_Re… This is formally correct for independent, zero-mean random errors in a linear sum. The critical questions are: * Is ±4 W/m² the right error metric to use? * Is it independent from year to year? * Is it additive in the way he assumes? All three are highly problematic. ===== 2.2 How he builds the ±4 W/m² LWCF “calibration error” ===== He pulls three main pieces together: # TCF error from Jiang et al. 2012 (and related work) - CMIP5 models have ~±12.1% RMS error in global annual mean total cloud fraction, derived from 25-year means (1980–2004) compared to satellite datasets (MODIS, ISCCP2). Propagation_of_Error_and_the_Re… - Error patterns across models are strongly lag-1 autocorrelated and pair-wise correlated, so he argues they must be systematic theory errors, not random noise. Propagation_of_Error_and_the_Re… # Conversion from cloud fraction error to LWCF error - Using Lauer & Hamilton (2013), he states CMIP5 models have ~±4 W/m² RMSE in long-wave cloud forcing (LWCF). Propagation_of_Error_and_the_Re… - This is consistent with their findings that model LWCF biases vs satellite climatologies are a few W/m² for multi-year means. American Meteorological Society Journals<ref>{{cite web|title=American Meteorological Society Journals|url=https://journals.ametsoc.org/view/journals/clim/26/11/jcli-d-12-00451.1.xml|publisher=American Meteorological Society Journals|access-date=2025-12-10}}</ref> # Treating that ±4 W/m² as “annual average LWCF thermal flux calibration error” per year - He labels this as ±4 W/m² yr⁻¹, and calls it a “lower limit of resolution” for atmospheric forcing in CMIP5 models. Propagation_of_Error_and_the_Re… - He then compares this per-year flux “uncertainty” to the trend in GHG forcing (~0.035 W/m² per year) and notes the factor ~114 difference. Propagation_of_Error_and_the_Re… Where this goes off the rails: * The ±4 W/m² in Lauer & Hamilton is a climatological bias/RMSE of mean cloud radiative effect, not a year-to-year random error that gets re-drawn each year. It’s a systematic model bias in the multi-year mean spatial field. American Meteorological Society Journals<ref>{{cite web|title=American Meteorological Society Journals|url=https://journals.ametsoc.org/view/journals/clim/26/11/jcli-d-12-00451.1.xml|publisher=American Meteorological Society Journals|access-date=2025-12-10}}</ref> * Frank effectively re-interprets that bias as a per-time-step random uncertainty that accumulates like a random walk. That’s not what Jiang/Lauer’s diagnostics represent, and it is not how climate models treat their fluxes internally. ===== 2.3 Treatment of measurement vs structural/model error ===== Frank is right that: * Calibration vs observations constrains model structural error, analogous to instrument calibration. Propagation_of_Error_and_the_Re… But then he: * Treats structural error as if it were a per-step additive uncertainty on the prognostic variable (tropospheric energy flux), and * Propagates it forward as if each year added a new independent realization of that error. If the LWCF error is truly systematic (his own lag-1 and pair-wise correlation analysis argues that strongly), then: * It behaves like a bias in the mean flux or spatial pattern, not as a zero-mean random variable with fresh draws each year. * A bias affects the level of simulated temperature (and probably feedback strength), but: - It does not blow up as √N in time. - Much of that bias cancels when we take anomalies relative to a baseline period, which is exactly what is done in projections and in observational datasets. He actually undercuts himself: he stresses that the TCF error is deterministic and systematic (R≥0.95, common patterns across models; Table 1, Figure 4). Propagation_of_Error_and_the_Re… That is not the error structure for which Eq. 6 is appropriate. ===== 2.4 Time-series aspects ===== Frank claims: * GCM global-mean temperature projections follow from Eq. 1: ΔTt=fCO2⋅33 K⋅F0+∑iΔFiF0+a,\Delta T_t = f_{\mathrm{CO2}} \cdot 33\,\text{K} \cdot \frac{F_0 + \sum_i \Delta F_i}{F_0} + a,ΔTt=fCO2⋅33K⋅F0F0+∑iΔFi+a, with f_CO2 and a fitted per model. Propagation_of_Error_and_the_Re… * He shows many examples where this emulation tracks GCM projections closely for historical and SRES/RCP runs (Figures 1–3, S4-1–S4-7). Propagation_of_Error_and_the_Re… Observations: * It is not surprising that a simple energy-balance-like model and GCM ensemble means show near-linear relation between global mean ΔT and effective radiative forcing – that’s standard and used all over the literature (e.g., Gregory plots, transient climate response). IPCC<ref>{{cite web|title=IPCC|url=https://www.ipcc.ch/site/assets/uploads/2018/02/WG1AR5_Chapter09_FINAL.pdf|publisher=ipcc.ch|access-date=2025-12-10}}</ref> * However, this does not mean the GCM is literally a one-equation linear model. The GCM’s complexity (spatial structure, internal variability, nonlinear feedbacks, ocean heat uptake) is simply being summarized in the global mean response to forcing. Frank’s emulation is a fit, not a mechanistic equivalence. Time-series methods: * He doesn’t really use formal time-series modeling (no explicit AR(1) treatment of internal variability in temperatures, no autocorrelation correction to trend uncertainty). * He focuses instead on cloud-fraction error statistics (including lag-1 structure in space, not time) and then treats the cloud forcing error as a per-year flux uncertainty in his emulation. This is a category mismatch: temporal propagation of uncertainty is being based on a spatial climatological bias. ===== 2.5 Where error types are conflated or double-counted ===== Some key conflations: * Systematic vs random error - He correctly notes cloud errors are systematic. Propagation_of_Error_and_the_Re… - Then uses random-error propagation formulas (RSS over N steps) as if the ±4 W/m² were independent draws each year. This is inconsistent with his own diagnosis. * Calibration RMSE vs “resolution limit” - A ±4 W/m² climatological LWCF RMSE does not mean the model “cannot resolve” smaller perturbations in forcing; it means its long-term cloud radiative effect has that level of bias/noise relative to a particular satellite product. In practice, differences between scenarios and temporal changes can be simulated with much higher precision than the bias vs observations. * Spatial field error vs global-mean flux uncertainty - Lauer & Hamilton’s RMSE is over grid-point fields. Frank treats it as a global scalar flux uncertainty that must apply directly to the global-mean energy budget each year. That’s a strong and unjustified simplification.
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