1. Introduction
During the winter season, heavy rainfall events in the western United States are known to be associated with the intraseasonal oscillation (ISO; e.g., Mo and Nogues-Paegle 2005). In the Intermountain West region, a different weather event is gaining increasing attention, that is, persistent inversions. Deep inversions often develop in valleys and mountain basins and frequently lead to poor air quality and associated human health problems (Reeves and Stensrud 2009). Recently, a close linkage between the occurrence of persistent inversions and the 20–40-day ISO was identified (Gillies et al. 2010, hereinafter GWB). The 20–40-day ISO is a pronounced mode in the wintertime midlatitude circulations (e.g., Horel and Mechoso 1988; Lau and Nath 1999), but, more so, its intraseasonal time scale implies that forecasting persistent inversions in the Intermountain West is somewhat beyond the ∼10-day horizon of weather forecast models (GWB).
A number of studies (e.g., Weickmann et al. 1985; Mo 1999; Jones 2000) suggest that the ISO in North America is an atmospheric response to diabatic heating anomalies associated with the Madden–Julian oscillation (MJO; Madden and Julian 2005). Empirical and dynamical forecasts of the MJO exhibit skill at lead times beyond 2 weeks (Waliser 2005), including the operational Climate Forecast System (CFS) of the National Centers for Environmental Prediction (NCEP), which has demonstrated credible skill in predicting the MJO as far out as 1 month (Seo et al. 2007, 2009; Weaver et al. 2009). Additionally, the CFS shows similar skill in forecasting West Coast extreme-rainfall events during winter (Jones et al. 2009). Such circumstances, together with the inversion–ISO relationship observed in GWB, imply that the CFS may exhibit potential in predicting the inversion development with a lead time beyond that of ∼10 days. These circumstances lead us to undertake an investigation of the CFS’s performance skill in predicting persistent inversions for Salt Lake City, Utah.
2. Datasets and the inversion–ISO relationship
The CFS is a fully coupled ocean–land–atmosphere dynamical seasonal prediction system and has been operational at NCEP since August 2004. Model specifications of the CFS are detailed in Saha et al. (2006). The NCEP provides historical CFS hindcast data starting at 1981 and extending through 2008. For each predicted period, the CFS hindcast is initialized from three ensemble means (denoted by μ1, μ2, and μ3) of five consecutive days computed from days 10 to 14 and from 20 to 24 of a particular month, and from days 1 to 4 of the following month (cf. Seo et al. 2009). Hence, the hindcasts for μ1, μ2, and μ3 start at days 12, 22, and 2, respectively, and extend throughout the period of interest (i.e., to end on 28 February). Observed atmospheric variables were obtained from the NCEP–U.S. Department of Energy Global Reanalysis 2 (GR-2; Kanamitsu et al. 2002). Upper-air soundings at Salt Lake City International Airport (KSLC) in Utah were utilized to analyze inversion conditions over the period from December 1980 to February 2008, as identified in GWB. For air quality measurements, we adopted daily observations of particulate matter of 2.5 μm in diameter or smaller (PM2.5) from a Utah Division of Air Quality station in Salt Lake City (site identifier 4-035-3006). Criteria for capping and deep stable layers (Wolyn and McKee 1989) were utilized by GWB to classify two types of inversion layers: 1) a capping inversion with an inversion lid capping a mixed or unstable layer above the ground level and 2) a surface inversion with a neutral or increasing temperature profile extending from the ground level up to a certain height. The dates and classifications of inversions are summarized in GWB.
GWB established an index via bandpass-filtered (20–40 days) KSLC geopotential height (hereinafter Z30d) at 300 hPa and used the index to conduct a composite analysis for the inversion frequency and PM2.5 concentrations. The composite was made of eight phases that evenly divide the Z30d “index cycle,” following Knutson and Weickmann (1987). The selection of this 20–40-day spectrum is due to the fact that the North American circulation seems to respond only to the high-frequency end (∼30 days) of the MJO (GWB), corresponding to previous findings (e.g., Mo and Nogues-Paegle 2005) that the tropical–extratropical linkages of the MJO are most sensitive to shorter time scales of the MJO. Moreover, the winter ISO in the midlatitudes has been attributed to the dominant beta effect of the free Rossby wave resulting in a distinct spectral peak at 30 days (Lau and Nath 1999). It therefore seems feasible that such a midlatitude forcing would confine the variation time scale to the higher-frequency end of the MJO.




As an example, the estimated SIP and PM2.5 concentrations during the 2003/04 winter are shown in Fig. 2b. A persistent surface inversion event occurred in mid-January 2004 that lasted for 14 days (denoted by a sequence of black dots). Two shorter events also occurred around 20 December 2003 and 16 February 2004. The estimated SIP from the KSLC Z30d (blue-shaded area) corresponds well to all three persistent surface inversion events, with a higher probability centered around the 14-day event. Shown in Fig. 2d is the circulation pattern for this surface inversion event calculated as an average over the 10–20 January period. A ridge system is dominant over western North America with Salt Lake City situated to the east of the ridge axis; this is the typical synoptic pattern associated with prolonged valley cold pools in the Great Basin (Reeves and Stensrud 2009). Moreover, the estimated PM2.5 concentrations (Fig. 2c; yellow-shaded area) are in good agreement with observed PM2.5 (black line), and both strongly coincide with the observed persistent surface inversion events. Since Eqs. (1) and (2) use the filtered geopotential height, short-term variations in the inversion and PM2.5 estimates are inevitably smoothed out. Nevertheless, short inversion events, such as observed on 24–25 January, are coupled with higher-frequency synoptic modes that are not as crucial as the 30-day cycle and so are not captured in long-range predictions owing to the 2-week “Lorenz limit” in weather forecasting.
3. CFS prediction skill
To predict the SIP, we constructed the Z30d index using the CFS’s 200-hPa geopotential height at the grid point nearest to KSLC (40°N, 112.5°W). For each CFS member, 2 months of the observed (GR-2) data prior to the initial day were added to the CFS output before filtering in order to avoid “ends of data” problems associated with the second-order Butterworth bandpass filter. The predicted SIP from all three CFS ensembles for January 2004 (as denoted in Fig. 2b) captures the mid-January persistent surface inversion event, but the CFS nearly misses the mid-February event. The predicted PM2.5 concentrations (as denoted in Fig. 2c) are similar, indicating that the CFS exhibits reasonable skill in predicting the ISO for up to 1 month, consistent with Jones et al. (2009). Further substantiation is found in the 200-hPa geopotential height during 10–20 January 2004 averaged from the three CFS ensembles (Fig. 2d); here, the predicted ridge is phase coincident with the observed ridge, albeit slightly weaker.
Forecast skill for the synoptic circulation pattern was assessed by calculating the spatial correlation between the CFS and the verifying values of the GR-2. For the domain, as defined in Fig. 2d (20°–65°N, 150°–80°W), the bandpassed geopotential height at 200 hPa was added to the mean eddy geopotential height of each winter in both the CFS and the GR-2. Correlations were then computed between the two: for the CFS, we used the hindcast for December–February from 1981 to 2008. As shown in Fig. 3a, the CFS correlation skills are positive beyond 7 weeks of lead time. Using a threshold of 0.5 for the correlation skill, as was used in Seo et al. (2009), the CFS appears to predict the synoptic pattern that pertains to persistent inversion events for up to about 4 weeks. Moreover, the 1-standard-deviation range of the CFS correlation skills exceeds 0.5 through day 49, suggesting that the CFS can occasionally predict the ISO circulation patterns for up to 7 weeks in advance.
For evaluation purposes, the CFS forecast skills were compared with various empirical forecast skills, including a principal component (PC)–lagged regression model (PCRLAG) that uses the first two PCs of the filtered geopotential height at 200 hPa, an autoregression (AR) model with the filtered geopotential height at each grid point, and the persistence forecast. These empirical forecast methods have been operational for short-term climate prediction at the NCEP/Climate Prediction Center. We used 3 months of the GR-2 data prior to the initial day of each ensemble and applied these to the empirical forecasts. As shown in Fig. 3a, the CFS skill is consistently greater than the PCRLAG and AR forecasts and is substantially better than the persistence forecast.


Figure 3b shows the number of hits (histogram) and the score (time series) of the CFS prediction with respect to lead time. The number of hits declines steadily with longer lead time but reveals three peaks in weeks 1–2, 3–4, and 5–6. This “wavy pattern” may be partly due to the 1-week interval between the three ensembles causing uneven sample sizes. Regardless, the CFS’s score exhibits a similar downward tendency but remains above 50% until week 4 and rises again to above 50% near week 6. Such prediction skill is consistent with the 2004 case in which the CFS successfully predicted the persistent surface inversion events out to 5 weeks (cf. red line in Fig. 2b), yet the CFS barely predicts the mid-February event with a similar lead time (cf. blue dashed line in Fig. 2b). These forecasts echo the ∼50% skill scores between weeks 5 and 6 in Fig. 3b. Nevertheless, skill scores of the CFS are consistently higher than those obtained from the empirical models, suggesting that the CFS offers a better forecast of persistent surface inversion events with a 4-week lead time. Such skill greatly surpasses the current inversion prediction procedure that relies solely on medium-range weather forecast models. Moreover, since Eq. (2) is practically a function of Eq. (1), the results also indicate an extended predictability of prolonged, high-PM2.5 concentration events by the CFS.
4. Discussion
Past studies of the MJO prediction have noted that forecast skill for precipitation typically declines faster than that for the atmospheric circulation (e.g., Waliser 2005). This is attributable to precipitation’s sensitivity to high-frequency weather disturbances, which have little long-term predictability. The proposed regression scheme with the CFS output, to predict persistent surface inversion events in the Intermountain West, may show relatively high skill simply because such inversion events are coupled with slow-moving circulation patterns (i.e., ridges) in contrast to unstable, highly variable precipitation systems (such as fronts). Another factor may be the CFS’s documented capability in predicting tropical circulations associated with the MJO. This factor was inspected through a compiled composite of the 200-hPa streamfunction and velocity potential, following the eight phases of the Z30d index at KSLC (Fig. 1). Each phase covers 3 days centered on the second day (dates of the composite are identical to those analyzed in GWB). Prior to the composite analysis, the streamfunction and velocity potential were bandpassed with 20–40 days, denoted respectively as ST30d and VP30d.
As shown in Fig. 4, the eight phases of the composite depict a clear eastward propagation of VP30d with predominant zonal wavenumber-1 patterns. Embedded within this typical MJO structure are a series of short-wave VP30d cells across the northeast Pacific Ocean and North America. These regional short-wave cells are accompanied by similarly definite, yet spatially in-quadrature, wave trains of ST30d. At phases 2 and 3 when the SIP in Salt Lake City is elevated, the ST30d wave trains appear to follow the classic “great circle” route of the Pacific–North America pattern (Horel and Wallace 1981), leading to a prevailing ridge in western North America. An oppositely signed circulation anomaly is also evident at phases 6 and 7. Despite the pronounced eastward propagation of global VP30d, the regional wave trains of both VP30d and ST30d appear to be quasi-stationary. Such a feature underscores the fact that wintertime stationary waves in North America fluctuate in response to the tropical–extratropical linkages of the MJO excited by tropical Pacific diabatic heating anomalies (e.g., Kushnir 1987; Mo and Nogues-Paegle 2005). These results strongly suggest that the occurrence of persistent inversions in the Intermountain West region is “phase locked” with the MJO evolution. As a result, the CFS’s skill in predicting the MJO (Seo et al. 2007, 2009; Weaver et al. 2009) likely assists in predicting the circulation systems in western North America that lead to persistent inversions.
Acknowledgments
Valuable comments by three anonymous reviewers were highly appreciated. We thank Marty Booth for preparing the PM2.5 data. This study was supported by the USDA–CSREES-funded Drought Management, Utah Project, and the Utah Agricultural Experiment Station, Utah State University, and approved as journal paper number 8186.
REFERENCES
Gillies, R. R., Wang S-Y. , and Booth M. R. , 2010: Atmospheric scale interaction on wintertime Intermountain West inversions. Wea. Forecasting, 25 , 1196–1210.
Horel, J. D., and Wallace J. M. , 1981: Planetary-scale atmospheric phenomena associated with the Southern Oscillation. Mon. Wea. Rev., 109 , 813–829.
Horel, J. D., and Mechoso C. R. , 1988: Observed and simulated intraseasonal variability of the wintertime planetary circulation. J. Climate, 1 , 582–599.
Jones, C., 2000: Occurrence of extreme precipitation events in California and relationships with the Madden–Julian oscillation. J. Climate, 13 , 3576–3587.
Jones, C., Gottschalk J. , Carvalho L. , and Higgins W. , 2009: Probabilistic forecast skill of extreme weather in weeks 1–4 in the United States during winter. Abstracts, 34th Annual Climate Diagnostics and Prediction Workshop, Monterey, CA, NCEP/Climate Prediction Center–Naval Meteorology and Oceanography Command, 4.02.
Kanamitsu, M., Ebisuzaki W. , Woollen J. , Yang S-K. , Hnilo J. J. , Fiorino M. , and Potter G. L. , 2002: NCEP–DOE AMIP-II Reanalysis (R-2). Bull. Amer. Meteor. Soc., 83 , 1631–1643.
Knutson, T. R., and Weickmann K. M. , 1987: 30–60 day atmospheric oscillations: Composite life cycles of convection and circulation anomalies. Mon. Wea. Rev., 115 , 1407–1436.
Kushnir, Y., 1987: Retrograding wintertime low-frequency disturbances over the North Pacific Ocean. J. Atmos. Sci., 44 , 2727–2742.
Lau, N. C., and Nath M. J. , 1999: Observed and GCM-simulated westward-propagating, planetary-scale fluctuations with approximately three-week periods. Mon. Wea. Rev., 127 , 2324–2345.
Madden, R. A., and Julian P. R. , 2005: Historical perspective. Intraseasonal Variability in the Atmosphere–Ocean Climate System, K.-M. Lau and D. E. Waliser, Eds., Springer, 1–16.
Mo, K. C., 1999: Alternating wet and dry episodes over California and intraseasonal oscillations. Mon. Wea. Rev., 127 , 2759–2776.
Mo, K. C., and Nogues-Paegle J. , 2005: Pan-America. Intraseasonal Variability in the Atmosphere–Ocean Climate System, K.-M. Lau and D. E. Waliser, Eds., Springer, 95–124.
Reeves, H. D., and Stensrud D. J. , 2009: Synoptic-scale flow and valley cold pool evolution in the western United States. Wea. Forecasting, 24 , 1625–1643.
Saha, S., and Coauthors, 2006: The NCEP Climate Forecast System. J. Climate, 19 , 3483–3517.
Seo, K-H., Schemm J. K. E. , Wang W. , and Kumar A. , 2007: The boreal summer intraseasonal oscillation simulated in the NCEP Climate Forecast System: The effect of sea surface temperature. Mon. Wea. Rev., 135 , 1807–1827.
Seo, K-H., Wang W. , Gottschalck J. , Zhang Q. , Schemm J. K. E. , Higgins W. R. , and Kumar A. , 2009: Evaluation of MJO forecast skill from several statistical and dynamical forecast models. J. Climate, 22 , 2372–2388.
Waliser, D., 2005: Predictability and forecasting. Intraseasonal Variability in the Atmosphere–Ocean Climate System, K.-M. Lau and D. E. Waliser, Eds., Springer, 389–423.
Weaver, S., Wang W. , and Kumar A. , 2009: Representation of MJO variability in the NCEP Climate Forecast System. Abstracts, 34th Annual Climate Diagnostics and Prediction Workshop, Monterey, CA, NCEP/Climate Prediction Center–Naval Meteorology and Oceanography Command, 4.04.
Weickmann, K. M., Lussky G. R. , and Kutzbach J. E. , 1985: Intraseasonal (30–60 day) fluctuations of outgoing longwave radiation and 250 mb streamfunction during northern winter. Mon. Wea. Rev., 113 , 941–961.
Wolyn, P. G., and McKee T. B. , 1989: Deep stable layers in the Intermountain western United States. Mon. Wea. Rev., 117 , 461–472.

Composite 300-hPa Z30d index at KSLC and the evenly divided eight phases (red line), probability of surface inversion days (blue bars; %), and PM2.5 concentrations at the Salt Lake City site (black line). Error bars are added for the probability and PM2.5. Modified from Gillies et al. (2010).
Citation: Weather and Forecasting 25, 4; 10.1175/2010WAF2222419.1

Composite 300-hPa Z30d index at KSLC and the evenly divided eight phases (red line), probability of surface inversion days (blue bars; %), and PM2.5 concentrations at the Salt Lake City site (black line). Error bars are added for the probability and PM2.5. Modified from Gillies et al. (2010).
Citation: Weather and Forecasting 25, 4; 10.1175/2010WAF2222419.1
Composite 300-hPa Z30d index at KSLC and the evenly divided eight phases (red line), probability of surface inversion days (blue bars; %), and PM2.5 concentrations at the Salt Lake City site (black line). Error bars are added for the probability and PM2.5. Modified from Gillies et al. (2010).
Citation: Weather and Forecasting 25, 4; 10.1175/2010WAF2222419.1

(a) Climatological frequencies of persistent surface inversion events (gray bars) for the period 1980–2008 and days with PM2.5 > 35 μg m−3 (golden line) and PM2.5 > 70 μg m−3 (dark red line) for the period 1999–2008. A 5-day smoothing was applied on all frequencies. (b) Estimated SIP from Eq. (1) using the KSLC Z30d at 200 hPa (blue shaded curve) overlaid with surface inversion days (dots) during December 2003–February 2004. (c) Estimated PM2.5 concentrations for Salt Lake City from Eq. (2) (green shaded curve) superimposed with the observed PM2.5 concentrations (black line). In (b) and (c) three CFS ensembles (μ1, μ2, and μ3) are plotted as color lines. (d) The 200-hPa geopotential height from GR-2 (black solid contours) and the average of all three CFS ensembles (pink dashed contours) for 10–20 Jan 2004. The contour interval is 100 m. KSLC is indicated with a blue star.
Citation: Weather and Forecasting 25, 4; 10.1175/2010WAF2222419.1

(a) Climatological frequencies of persistent surface inversion events (gray bars) for the period 1980–2008 and days with PM2.5 > 35 μg m−3 (golden line) and PM2.5 > 70 μg m−3 (dark red line) for the period 1999–2008. A 5-day smoothing was applied on all frequencies. (b) Estimated SIP from Eq. (1) using the KSLC Z30d at 200 hPa (blue shaded curve) overlaid with surface inversion days (dots) during December 2003–February 2004. (c) Estimated PM2.5 concentrations for Salt Lake City from Eq. (2) (green shaded curve) superimposed with the observed PM2.5 concentrations (black line). In (b) and (c) three CFS ensembles (μ1, μ2, and μ3) are plotted as color lines. (d) The 200-hPa geopotential height from GR-2 (black solid contours) and the average of all three CFS ensembles (pink dashed contours) for 10–20 Jan 2004. The contour interval is 100 m. KSLC is indicated with a blue star.
Citation: Weather and Forecasting 25, 4; 10.1175/2010WAF2222419.1
(a) Climatological frequencies of persistent surface inversion events (gray bars) for the period 1980–2008 and days with PM2.5 > 35 μg m−3 (golden line) and PM2.5 > 70 μg m−3 (dark red line) for the period 1999–2008. A 5-day smoothing was applied on all frequencies. (b) Estimated SIP from Eq. (1) using the KSLC Z30d at 200 hPa (blue shaded curve) overlaid with surface inversion days (dots) during December 2003–February 2004. (c) Estimated PM2.5 concentrations for Salt Lake City from Eq. (2) (green shaded curve) superimposed with the observed PM2.5 concentrations (black line). In (b) and (c) three CFS ensembles (μ1, μ2, and μ3) are plotted as color lines. (d) The 200-hPa geopotential height from GR-2 (black solid contours) and the average of all three CFS ensembles (pink dashed contours) for 10–20 Jan 2004. The contour interval is 100 m. KSLC is indicated with a blue star.
Citation: Weather and Forecasting 25, 4; 10.1175/2010WAF2222419.1

(a) Correlation skill of the 200-hPa geopotential height as a function of forecast time for the CFS, PCRLAG, AR, and persistence forecasts. The shaded area outlines 1 std dev of the CFS skill. (b) Scores of persistent surface inversion forecasting (lines) for the CFS, PCRLAB, and AR, superimposed with the number of hits of persistent surface inversion events by the CFS (gray bars). The computation was performed over a 28-yr (1981–2008) period.
Citation: Weather and Forecasting 25, 4; 10.1175/2010WAF2222419.1

(a) Correlation skill of the 200-hPa geopotential height as a function of forecast time for the CFS, PCRLAG, AR, and persistence forecasts. The shaded area outlines 1 std dev of the CFS skill. (b) Scores of persistent surface inversion forecasting (lines) for the CFS, PCRLAB, and AR, superimposed with the number of hits of persistent surface inversion events by the CFS (gray bars). The computation was performed over a 28-yr (1981–2008) period.
Citation: Weather and Forecasting 25, 4; 10.1175/2010WAF2222419.1
(a) Correlation skill of the 200-hPa geopotential height as a function of forecast time for the CFS, PCRLAG, AR, and persistence forecasts. The shaded area outlines 1 std dev of the CFS skill. (b) Scores of persistent surface inversion forecasting (lines) for the CFS, PCRLAB, and AR, superimposed with the number of hits of persistent surface inversion events by the CFS (gray bars). The computation was performed over a 28-yr (1981–2008) period.
Citation: Weather and Forecasting 25, 4; 10.1175/2010WAF2222419.1

Composite eight phases of the 200-hPa Z30d index at KSLC in terms of the filtered streamfunction (ST30d; contours) and velocity potential (VP30d; shadings) at 200 hPa superimposed with the divergent winds (vectors; above the 10% significance level). The calculation was based on the 28-yr GR-2 data. The contour interval (CI) of ST30d is 1.5 × 106 m2 s−1, and the zero contours are omitted. The golden line at 120°W roughly indicates the position of the winter mean ridge. The ST30d wave train is illustrated by a red dashed arrow at phases 3 and 7.
Citation: Weather and Forecasting 25, 4; 10.1175/2010WAF2222419.1

Composite eight phases of the 200-hPa Z30d index at KSLC in terms of the filtered streamfunction (ST30d; contours) and velocity potential (VP30d; shadings) at 200 hPa superimposed with the divergent winds (vectors; above the 10% significance level). The calculation was based on the 28-yr GR-2 data. The contour interval (CI) of ST30d is 1.5 × 106 m2 s−1, and the zero contours are omitted. The golden line at 120°W roughly indicates the position of the winter mean ridge. The ST30d wave train is illustrated by a red dashed arrow at phases 3 and 7.
Citation: Weather and Forecasting 25, 4; 10.1175/2010WAF2222419.1
Composite eight phases of the 200-hPa Z30d index at KSLC in terms of the filtered streamfunction (ST30d; contours) and velocity potential (VP30d; shadings) at 200 hPa superimposed with the divergent winds (vectors; above the 10% significance level). The calculation was based on the 28-yr GR-2 data. The contour interval (CI) of ST30d is 1.5 × 106 m2 s−1, and the zero contours are omitted. The golden line at 120°W roughly indicates the position of the winter mean ridge. The ST30d wave train is illustrated by a red dashed arrow at phases 3 and 7.
Citation: Weather and Forecasting 25, 4; 10.1175/2010WAF2222419.1