Bulletin of the American Meteorological Society Tornadoes in the Central United States and the "Clash of Air Masses" --Manuscript Draft-Manuscript Number: BAMS-D-13-00252 Full Title: Tornadoes in the Central United States and the "Clash of Air Masses" Article Type: Article Corresponding Author: David M. Schultz, Ph.D. University of Manchester Manchester, UNITED KINGDOM Corresponding Author's Institution: University of Manchester First Author: David M. Schultz, Ph.D. Order of Authors: David M. Schultz, Ph.D. Yvette P. Richardson Paul M. Markowski Charles A. Doswell Manuscript Classifications: 2.252: Fronts; 2.464: Tornadogenesis; 3.168: Fronts; 3.440: Tornadoes Abstract: After tornado outbreaks or individual violent tornadoes occur in the central United States, media stories often attribute the location, number, or intensity of tornadoes to the "clash of air masses" between warm tropical air and cold polar air. This article argues that such a characterization of tornadogenesis is oversimplified, outdated, and incorrect. Airmass boundaries and associated temperature gradients can be important in tornadogenesis, but not in the ways envisioned on the synoptic scale with the clashof-air-masses conceptual model. In fact, excessively strong horizontal temperature gradients (either on the synoptic scale or associated with a storm's own cool outflow) may be detrimental to tornadogenesis. Where adjacent air masses are relevant is through their vertical distribution that produces the requisite instability for the convective storm, but that instability is not directly related to the formation of tornadoes. Therefore, this article recommends that a greater effort be made to communicate accurately to the public the current scientific understanding of the conditions under which tornadoes are formed. Author Comments: We have attached a figure that might be used for the cover of BAMS if desired. Best regards, Dave Suggested Reviewers: Bob Ryan [email protected] Prominent media person Doyle Rice USA Today [email protected] Weather editor of USA Today Powered by Editorial Manager® and ProduXion Manager® from Aries Systems Corporation Manuscript (non-LaTeX) Click here to download Manuscript (non-LaTeX): ClashR2-submitted.doc 1 2 3 4 Tornadoes in the Central United States and 5 the “Clash of Air Masses” 6 7 8 DAVID M. SCHULTZ 9 10 11 Centre for Atmospheric Science, School of Earth, Atmospheric and Environmental Sciences, University of Manchester, Manchester, United Kingdom 12 YVETTE P. RICHARDSON AND PAUL M. MARKOWSKI 13 14 15 16 Department of Meteorology, Pennsylvania State University, University Park, Pennsylvania 17 Doswell Scientific Consulting, Norman, Oklahoma 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 CHARLES A. DOSWELL III An Article for the Bulletin of the American Meteorological Society Submitted 26 November 2013 Revised 20 January 2014 Revised 9 March 2014 Corresponding author address: Prof. David M. Schultz; Centre for Atmospheric Science; School of Earth, Atmospheric and Environmental Sciences; University of Manchester; Simon Building, Oxford Road; Manchester M13 9PL, United Kingdom. E-mail: [email protected] 35 36 ABSTRACT 37 After tornado outbreaks or individual violent tornadoes occur in the central United States, media 38 stories often attribute the location, number, or intensity of tornadoes to the “clash of air masses” 39 between warm tropical air and cold polar air. This article argues that such a characterization of 40 tornadogenesis is oversimplified, outdated, and incorrect. Airmass boundaries and associated 41 temperature gradients can be important in tornadogenesis, but not in the ways envisioned on the 42 synoptic scale with the clash-of-air-masses conceptual model. 43 horizontal temperature gradients (either on the synoptic scale or associated with a storm’s own 44 cool outflow) may be detrimental to tornadogenesis. Where adjacent air masses are relevant is 45 through their vertical distribution that produces the requisite instability for the convective storm, 46 but that instability is not directly related to the formation of tornadoes. Therefore, this article 47 recommends that a greater effort be made to communicate accurately to the public the current 48 scientific understanding of the conditions under which tornadoes are formed. In fact, excessively strong 49 50 CAPSULE 51 Media reports that clashing air masses produce tornadoes mischaracterize the abundant new 52 observational and modeling research on how tornadoes form. 53 54 2 55 The central United States is home to the most frequent violent tornadoes on Earth (Fig. 56 1). When major outbreaks of such tornadoes occur, the media often explains their 57 occurrence as the result of the “clash of air masses.” Consider the following example: 58 Oklahoma provides a fertile breeding ground for tornadoes because of the clash 59 between the warm, moist air from the Gulf and cold air from the Rockies and 60 Canada: One of the main keys to tornado formation … is “a large temperature 61 spread over a short distance.” “Water holds its heat more than land or air.... So 62 Oklahoma's proximity to the Gulf of Mexico means there is a source of very 63 warm, moist air. As cold air comes from Canada, you can get temperatures of 80 64 degrees [F] in the body of the state while it is in the 20s in the Panhandle.” [The 65 interviewee says this provides] the power to fuel severe thunderstorms. 66 http://www.usatoday.com/story/news/nation/2013/06/08/oklahoma-tornadoes- 67 ef5-moore/2401885/ 68 Other examples of media reporting that the clash of the air masses is responsible for tornadoes 69 may be found at http://www.independent.co.uk/news/tornado-disaster-clash-of-air-masses-in- 70 tornado-alley-1091490.html, 71 tornado-rotation, 72 (http://ngm.nationalgeographic.com/2013/11/biggest-storm/tornado-formation), and in Fig. 2. 73 There is no intention to single out any particular person or media source with this list, but rather 74 to exemplify the type of storyline that appears in the media. Therefore, the consistent message in 75 the media is that tornadoes form along the boundaries between air masses, such as cold fronts or 76 drylines, with tornado formation being directly linked to the intensity of the “clashing” between in the http://www.myfoxaustin.com/story/21871999/weather-factsNovember 2013 3 issue of National Geographic 77 adjacent air masses. Such clashing could perhaps be thought to provide the lift in the three 78 ingredients of deep, moist convection: lift, instability, and moisture (Johns and Doswell 1992). 79 80 The reality is that air masses “clash” all the time, but frontal zones only produce tornadoes on 81 relatively few occasions. Further, as we will discuss, many tornadoes occur outside of regions 82 where air masses are “clashing.” 83 occurrence of tornadoes is at best a gross oversimplification. Therefore, using this canard as an explanation for the 84 85 Why and when the specific phrase “clash of the air masses” was introduced to explain tornadoes 86 in the central United States is not clear. One possible origin may be this 1942 quote from 87 Sylvester E. Decker, the climatologist for the Weather Bureau Office in Des Moines, Iowa, 88 describing tornadoes in Iowa over the past 15 months (House 1963, p. 141): 89 Usually more than two air masses are present. There is first of all the original 90 cold air mass to the north of the front, a warm [air] mass to the south of the front 91 with a stable air mass that is drier and warmer aloft over the warm air mass. 92 Reference in the above quote is made to a front. The concept of fronts as airmass boundaries 93 originates from the Norwegian cyclone model (Bjerknes 1919; Bjerknes and Solberg 1921, 94 1922), which describes the formation of low-pressure systems along the polar front, a region 95 where cold polar air is adjacent to warm tropical air. That World War I had recently ended at the 96 time of the introduction of this frontal terminology (think All Quiet on the Western Front) is no 97 coincidence (Friedman 1989, pp. 187–188). 98 4 99 In the relatively flat central United States, continental polar, continental tropical, and maritime 100 tropical air masses meet easily, a factor in creating the baroclinic environments that favor 101 extratropical cyclones. The extratropical cyclones that bring together the ingredients for severe 102 convective storms (moisture from the Gulf of Mexico, steep lapse rates coming off the high and 103 dry terrain of the Rocky Mountains, and vertical wind shear) are closely tied to the pole-to- 104 equator thermal gradients, but the mere presence of those gradients on the synoptic scale is no 105 guarantee that these ingredients will be brought together to produce tornadoes in any specific 106 extratropical cyclone. 107 108 Horizontal temperature gradients also exist on the storm scale. Temperature gradients associated 109 with downdrafts and outflow are likely important in tornadogenesis in supercells (the most 110 violent tornadoes are almost always associated with rotating convective storms called supercells, 111 Fig. 3), but, as we will discuss, “airmass clashing” is not the best way to describe the role of such 112 storm-scale temperature gradients in tornadogenesis. In fact, excessively strong storm-scale 113 temperature gradients are associated with nontornadic supercells (e.g., Markowski and 114 Richardson 2009). 115 116 MOVING BEYOND THE “CLASH OF THE AIR MASSES” ON THE SYNOPTIC 117 SCALE. If the clash of the air masses has any validity as an explanation for tornadoes, there are 118 two ways that synoptic-scale horizontal temperature contrasts can be thought to have some 119 relevance in tornado development. One is through their link to vertical wind shear (essential to 120 supercell storms), and the other through their link, at times, to storm initiation. 121 5 122 With regard to vertical shear, the vertical derivative of the geostrophic wind is directly related to 123 the horizontal temperature gradient, which is why it is called the thermal wind shear. Thus, for 124 example, a north–south temperature contrast implies an increasing westerly wind component 125 with height. Another part of the wind shear is that associated with the ageostrophic wind, which 126 is not directly related to the horizontal temperature gradient. Moreover, whatever the source of 127 the shear, it must be located where there is buoyant instability to feed a storm. Tornadic storms 128 are not necessarily collocated with the maximum vertical shear; rather, they are located where 129 there is sufficient shear and that shear overlaps with buoyant instability. So, although there is a 130 loose connection between temperature gradients and vertical wind shear, the connection is even 131 looser between temperature gradients and tornadic storms. Indeed, Diffenbaugh et al. (2013) 132 showed that under expected climate change, while vertical shear at midlatitudes decreases in 133 general as a result of weakening meridional thermal gradients, the number of days with 134 conditions favorable for severe weather increases, owing to the greater overlap of regions of 135 favorable shear and instability. 136 137 With regard to the initiation of storms, all convective storms are initiated when air parcels with 138 convective available potential energy (CAPE) reach their level of free convection (LFC), with 139 one of the most common mechanisms for storm initiation being ascent associated with airmass 140 boundaries (e.g., fronts, drylines) or other subsynoptic-scale boundaries (e.g., outflow 141 boundaries, sea-breeze fronts). Thus, the frequent proximity of low-level temperature gradients 142 to developing convective storms is not unique to supercells. 143 convective storms initiated along airmass boundaries become tornadic. 144 6 Only a small percentage of 145 In addition, the strength of the temperature gradient along a synoptic-scale airmass boundary has 146 no precise relationship to the potential for storms initiated along the boundary to spawn 147 tornadoes (often supercells have moved a significant distance away from a synoptic-scale 148 initiating boundary by the time they reach maturity and pose a tornado threat).1 If anything, there 149 is some indication that squall lines, not supercells, are more likely when the temperature gradient 150 associated with an airmass boundary is intense (e.g., Roebber et al. 2002; Arnott et al. 2006; 151 Stonitsch and Markowski 2007; Dial et al. 2010; Duda and Gallus 2010; Schumann and Roebber 152 2010). In other words, strong horizontal temperature gradients may actually pose a decreased 153 risk of significant tornadoes (EF2 or greater tornadoes; Hales 1988), given that squall lines are 154 less likely to produce significant tornadoes than are discrete supercells (Trapp et al. 2005a; 155 Thompson et al 2012; Smith et al. 2012). 156 157 One instance in which an airmass boundary can influence tornadogenesis may be the interaction 158 of an ongoing supercell with a pre-existing airmass boundary. Some supercell storms move 159 along or across airmass boundaries such as warm fronts, stationary fronts, or outflow boundaries 160 produced by other storms, where the likelihood of tornado formation may be locally increased 161 owing to enhanced wind shear and moisture near the boundary (e.g., Maddox et al. 1980; 162 Markowski et al. 1998; Rasmussen et al. 2000; Wurman et al. 2007). So, in some cases, the 163 temperature gradient along a front may be a component of a favorable environment for tornadic 164 supercells, although certainly not in all cases. Supercells produce tornadoes in the absence of 165 such storm–boundary interactions, and many storm–boundary interactions result in weakening of 1 In contrast, nonsupercell tornadoes are favored in storms that have a slow forward motion relative to the initiating airmass boundary. Nonsupercell tornadoes (e.g., Wakimoto and Wilson 1989) also seem to require that the initiating boundary be associated with misocyclones at the surface (i.e., cyclonic vorticity at the surface that precedes the tornadoes) (e.g., Lee and Wilhelmson 1997). 7 166 the supercell and decreased tornado potential (Markowski et al. 1998; Doswell et al. 2002). 167 These interactions are not well understood and, moreover, are not essential for tornado 168 formation. If anything, storm-boundary interactions seem least likely to trigger tornadogenesis 169 when the boundary is accompanied by a large temperature gradient, which usually implies a 170 rapid increase in the convective inhibition (as well as decreasing surface-based CAPE) 171 encountered by a storm moving across the boundary (Doswell et al., 2002). 172 173 Not only is the strength of the temperature gradient associated with clashing air masses of 174 questionable relevance to tornadic supercell initiation, many tornadic supercells are not even 175 initiated along fronts. Three examples follow. First, tornadic storms commonly form along or 176 near a dryline, a zone of strong moisture contrast but only a modest temperature gradient, 177 depending on the time of day (e.g., Rhea 1966; Schaefer 1974; Ziegler and Rasmussen 1998). 178 Second, tornadic supercells commonly develop as a result of moist, unstable air flowing gently 179 upslope (i.e., toward the west) on the High Plains, especially in regions where such orographic 180 lifting is enhanced (e.g., Palmer Divide of eastern Colorado, Cheyenne Ridge of southeastern 181 Wyoming). Such upslope severe weather regimes typically are found on the cool side of (not 182 along) a synoptic-scale front or outflow boundary produced by an antecedent mesoscale 183 convective system (e.g., Doswell 1980). Third, supercells may even form along rainbands in 184 hurricanes (e.g., McCaul 1987; Baker et al. 2009; Molinari and Vollaro 2010; Green et al. 2011; 185 Edwards et al. 2012). Thus, there are diverse situations in which strong tornadoes could form 186 with no strong temperature gradient present. 187 8 188 If there is any clashing of air masses associated with supercell tornadoes, perhaps it is in the 189 vertical, rather than the horizontal. But, media explanations typically do not refer to this vertical 190 distribution of air masses. Specifically, deep moist convective storms, including supercells, form 191 as a result of the release of buoyant instability, and this instability in the central United States 192 frequently comes from the vertical collocation of maritime tropical air underneath continental 193 tropical air at midlevels from the southwest, the so-called elevated mixed layer (e.g., Carlson et 194 al. 1983). Critically, this vertical distribution of air masses must also be associated with deep- 195 layer shear over several kilometers in depth to allow storm-scale rotation to occur within 196 supercells. As described above, although a part of this wind shear is associated with horizontal 197 temperature gradients due to thermal wind balance, the area of greatest “clashing between two 198 air masses” is not necessarily the area of greatest tornado development. Moreover, this vertical 199 distribution of air masses occurs much more frequently in this region than the occurrence of 200 tornadoes, so the concept has limited predictive ability for tornadogenesis (as discussed in the 201 next section). 202 203 To summarize, the clash of air masses on the synoptic scale may be associated with strong 204 horizontal temperature gradients, but these situations tend not to be particularly favorable for 205 supercells and tornadoes. Instead, the clash of the air masses most relevant for supercells may be 206 in the vertical as warm moist air from the Gulf of Mexico underlies the steep lapse rates within 207 the elevated mixed layer, producing buoyant instability and vertical wind shear, environmental 208 conditions favorable for supercellular convection, but not specifically tornadogenesis. 209 210 MOVING BEYOND “CLASH OF THE AIR MASSES” ON THE STORM SCALE. 9 211 Existing understanding of tornadogenesis on the scale of a convective storm is far from 212 complete. Only around 25% of supercells with radar-detected mesocyclones (rotation of a 213 broader scale than a tornado) become tornadic (Trapp et al. 2005b), so the key issue is what 214 conditions permit tornado formation in only a minority of supercells. 215 216 Observations with airborne and mobile radars have suggested that strong rotation, down as low 217 as several hundred meters above the ground, can be present in a supercell without the potentially 218 damaging rotation of a tornado ever developing at the surface (e.g., Trapp 1999; Markowski et 219 al. 2011). Unlike the rotation at midlevels, rotation at the surface cannot develop with only an 220 updraft and environmental shear (horizontal vorticity) because parcels will be moving away from 221 the ground as the vorticity is tilted into the vertical (e.g., Davies-Jones and Brooks 1993). Thus, 222 the downdrafts in a supercell are essential to tornadogenesis. 223 224 Leading hypotheses for tornadogenesis suggest that vertical vorticity develops as air descends 225 within a storm-scale temperature gradient within the outflow (e.g., Davies-Jones et al. 2001; 226 Markowski and Richardson 2009; Wurman et al. 2013). If the near-surface circulation produced 227 in this manner within the outflow moves into a region of strong ascent, the circulation can be 228 accelerated upward and contracted to tornadic strength via conservation of angular momentum. 229 Although the degree of storm-scale baroclinity available to produce the tornadic circulation 230 increases as the outflow temperature decreases, the low-level temperature decrease makes it 231 difficult to carry out the final contraction because the low-level vertical accelerations required to 232 contract the circulation are inhibited by negatively buoyant air. Therefore, there is a “sweet 233 spot” in the temperature contrast that allows the development of significant circulation while still 10 234 allowing the final contraction to take place. This situation is in contrast to the hypothesis that 235 tornado likelihood increases with the intensity of the temperature contrast. In addition, there is 236 some indication that colder outflow in nontornadic supercells may be shunted away from the 237 location of maximum updraft, such that the final contraction does not occur (Snook and Xue 238 2008; Markowski and Richardson 2014). 239 240 Two empirical factors seem to be helpful in discriminating between tornadic and nontornadic 241 supercells: the lifting condensation level (LCL) and the vertical wind shear in the lowest 242 kilometer (e.g., Rasmussen and Blanchard 1998; Brooks et al. 2003; Thompson et al. 2003; 243 Grams et al. 2012; Thompson et al. 2012). A low LCL is related to high low-level relative 244 humidity and, presumably, warmer downdrafts (Markowski et al. 2002; Shabbott and Markowski 245 2006). Strong low-level shear enhances and lowers the base of the midlevel mesocyclone 246 (formed through tilting of environmental horizontal vorticity as described above), which is then 247 associated with greater ability to lift (and contract) the outflow air due to vertical pressure 248 gradients associated with changes in rotation with height (Markowski and Richardson 2014). 249 Therefore, the two empirical factors favored for tornado environments refute the concept that a 250 colder downdraft (i.e., “greater clashing”) is better on the storm scale. Thus, there appears to be 251 little support for clashing air masses on the storm scale being responsible for tornadogenesis. 252 253 CONCLUSION. Based on our arguments above, we conclude that the notion of tornadogenesis 254 being directly related to the “clash of air masses” has limited utility as an explanation on both the 255 synoptic scale and storm scale. Therefore, repeating this myth in the media does the public a 256 disservice and does not reflect the science of severe storms as it has developed in recent decades. 11 257 If there is any value in retaining the airmass concept, it is in the vertical collocation of air masses 258 that produce the instability requisite for intense convective storms, but this explanation does not 259 pertain to tornadoes specifically, just to the environment of convective storms in the central 260 United States. 261 262 Therefore, we recommend that the weather enterprise work with the media to adopt a new 263 explanation for tornadic storms. Instead of “Yesterday's storms were the result of a clashing of 264 air masses,” we believe that an explanation along these lines would be more appropriate for a lay 265 audience in the vast majority of cases [with parenthetical information included if applicable to 266 the specific case]. 267 “Yesterday's storms occurred when warm humid air near the surface lay under drier 268 air aloft with temperature decreasing rapidly with height [originating from higher 269 terrain to the west or southwest], providing energy for the storms through the 270 production of instability. Large changes in wind with height (“wind shear”) over both 271 shallow (lowest 1 km) and deep (lowest 6 km) layers—combined with the instability 272 and high humidity near the surface—created a situation favorable for tornadoes to 273 form.” 274 This explanation, albeit longer than the clashing explanation, is pithy and accurate, describing 275 both the ingredients that make the synoptic environment favorable for convective storms and the 276 known factors that favor tornado formation. 277 278 Given the large investment in tornado research by the National Science Foundation (e.g., over 279 $10 million on VORTEX2 alone; Wurman et al. 2013) and the rapid progress in understanding 12 280 of tornadoes that has resulted, we hope that future information provided to the public can better 281 reflect that growth in scientific understanding. 282 283 Acknowledgments. We thank Editor Jeff Waldstreicher, Greg Forbes, and three anonymous 284 reviewers for their comments that have improved this manuscript. Partial funding for Schultz 285 was provided by the U.K. Natural Environment Research Council to the University of 286 Manchester for the Diabatic Influences on Mesoscale Structures in Extratropical Storms 287 (DIAMET) project (grant NE/I005234/1) and the Tropopause Folding, Stratospheric Intrusions 288 and Deep Convection (TROSIAD) project (grant NE/H008225/1). Funding for Richardson and 289 Markowski was provided by the U.S. National Science Foundation (AGS-1157646). 290 291 REFERENCES 292 Arnott, N. R., Y. P. Richardson, E. M. Rasmussen, and J. M. Wurman, 2006: Relationship 293 between a weakening cold front, misocyclones, and cloud development on 10 June 2002 294 during IHOP. Mon. Wea. Rev., 134, 311–335. 295 296 Baker, A. K., M. D. Parker, and M. D. Eastin, 2009: Environmental ingredients for supercells and tornadoes within Hurricane Ivan. Wea. 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Shaded contours (see the key) showing the number of days per century a violent 410 tornado (EF4 to EF5) touched down within 25 miles (40 km) of a point during the period 1921– 411 2010 (inclusive) (Fig. 1 in Doswell et al. 2012). 412 413 Figure 2: British Broadcasting Corporation (BBC) Science Editor David Shukman’s tweet the 414 day after the 20 May 2013 Moore, Oklahoma, tornado. 415 http://www.bbc.co.uk/weather/feeds/22608236. The link points to 416 417 Figure 3. Photo of a previously tornadic supercell storm on 10 June 2010 near Last Chance, 418 Colorado (copyright C. A. Doswell III). 419 19 420 421 422 Figure 1. Shaded contours (see the key) showing the number of days per century a violent 423 tornado (EF4 to EF5) touched down within 25 miles (40 km) of a point during the period 1921– 424 2010 (inclusive) (Fig. 1 in Doswell et al. 2012). 425 20 426 427 Figure 2: British Broadcasting Corporation (BBC) Science Editor David Shukman’s tweet the 428 day after the 20 May 2013 Moore, Oklahoma, tornado. 429 http://www.bbc.co.uk/weather/feeds/22608236. 430 21 The link points to 431 432 433 Figure 3. Photo of a previously tornadic supercell storm on 10 June 2010 near Last Chance, 434 Colorado (copyright C. A. Doswell III). 22 Response to Reviewers Click here to download Response to Reviewers: Responses to Editor-R2.docx Responses to Editor We have received two reviews of your revised manuscript. The reviewers' comments are appended below. The manuscript is quite improved. I would like you to consider a couple of minor revisions before final acceptance of the paper. Jeff, thank you for your shepherding our manuscript through the peer-review process. Also, thanks for your suggestions that have resolved the differences between us and the reviewers. Reviewer 3 is still concerned about the highlighting of the USA Today article (lines 56-66), and its reflection on Mike Smith. While the revised version is improved in this regard, I am still a little uncomfortable with this situation. I would like to propose an alternative that I think would improve this situation and still effectively make your intended point. We now include a statement after the quote: “There is no intention to single out any particular person or media source, but rather to exemplify the type of storyline that appears in the media." This quote simply provides evidence that there is a problem with the explanations in the media. This week there was a national story about a physicist, Rongjia Tao from Temple University who was proposing (in a presentation at the American Physical Society's Annual Meeting) that a series of enormous walls be constructed in tornado alley to diminish the tornado threat in this region. His argument essentially is that the walls would prevent the clash of air masses in this region. Ironically, the experts quoted in the USA Today story (http://www.usatoday.com/story/weather/2014/02/25/giant-walls-tornadoalley/5808887/) refuting this proposal are Mike Smith and Harold Brooks. I suggest utilizing this article as the one highlighted in the text. The current article could be included among the other examples cited (lines 67-71) if you strongly believe that is necessary. We don’t believe it is necessary. Perhaps you could also include a comment (perhaps a footnote) regarding the potential for experts to be mis-quoted, quotes utilized out of context, or incorrect paraphrasing due to not-experts in the media attempting to merge expert comments into their use of this incorrect concept. We reiterate our concern that the issue of whether people are being quoted accurately or not is a distraction. Clearly, most stories are the result of the media’s simplified understanding of tornadic storms. Thus, accurate reporting is not relevant to our point. Reviewer 4 still has questions and concerns about the intended audience for this article. Aside from the original comments from Greg Forbes that you have addressed, I do not see any indication that the other reviewers share this concern, and neither do I. As a BAMS article, this piece addresses the various members of the weather enterprise, including but not limited to the "experts" within the media. As you have acknowledged in your response to Dr. Forbes, reaching the non-expert component of the media will have to be done via other forums. While the latter is the majority of the real problem, the former (the Weather Enterprise) needs to be cognizant of this issue and be prepared to help refute the mis-conceptions (and not fall into the easy sound-bite trap). We agree. However, I do think that line 259 needs a little rewording. This comes across like you are speaking directly to the non-expert media and not necessarily the weather enterprise. I think your recommendation of having "the media adopt a new explanation for tornadic storms" is the desired end goal, but for the purpose of the BAMS venue, I think the key point is having the weather enterprise (e.g., the experts) help make this happen. I suggest a rephrasing along the lines of "Therefore, we recommend that the weather enterprise encourage [alt. work with] the media to adopt a new explanation for tornadic storms." Thank you. That is a good suggestion. That change has been implemented. Regarding Reviewer 4's second point I do not believe the BAMS audience needs a comprehensive analysis of the climatology of horizontal temperature gradients and their relationship to tornadoes to be convinced of this argument. Yes, perhaps such a study might put this issue to bed for good. This could be a good future project for a student (or maybe an undergraduate class). I do not think this is necessary for this article. Such a study could be its own future technical journal submission. We agree. Such a study goes well beyond what is needed at this stage for this article in BAMS. Responses to Reviewer 3: Thank you again for your further suggestions on improving our manuscript. Reviewer #3: The revised version is generally acceptable to me, but I think that the authors are still (unfairly, for points that I made before regarding the tendency of reporters to misrepresent and/or misunderstand their interviewees) singling out Mike Smith, and still could make their point well enough without providing links to specific articles. Please consider simply paraphrasing this article and the others, including key misuses of 'air mass clashing'. The BAMS readership should be sufficiently savvy to use internet search engines to find articles with such phrases. We have proposed a suggested revision that Editor Waldstreicher has agreed will address this concern: “There is no intention to single out any particular person or media source, but rather to exemplify the type of storyline that appears in the media." We reiterate our concern that the issue of whether people are being quoted accurately or not is a distraction. Clearly, most stories are the result of the media’s simplified understanding of tornadic storms. Thus, accurate reporting is not relevant to our point. Responses to Reviewer 4: Reviewer #4: The authors have addressed a number of concerns with this second revision. These changes are sufficient for this reviewer to modify the previous recommendation from "reject" to "accept with major revision". There remain two significant areas of concern with respect to this work. Thank you for your comments. The first concern is one of confusion over who the intended audience is for the information contained within the manuscript. The readership of AMS BAMS may include those categorized as mass media communicators but this demographic must be a small percentage of total subscribers. Yet, this appears to be the target audience as stated on page 12, line 259: "Therefore, we recommend that the media adopt a new explanation for tornadic storms." Another reviewer has already noted: "When it comes to correcting media behavior, however, this article would need to be published in a trade journal or an on-line forum read by nonmeteorologists in the broadcast industry." We have followed the recommendation of Editor Waldstreicher with the following addition to the text: "Therefore, we recommend that the weather enterprise work with the media to adopt a new explanation for tornadic storms." We will pursue the trade journal recommendation once this work is online and can be referenced. While that approach (publishing in a trade journal) is one way of highlighting and possibly correcting the inaccuracies of the "clash" interpretation with respect to tornadoes, what the authors actually wish to accomplish by publishing in BAMS is the establishment of scientific evidence supportive of their argument, primarily for other meteorologists. It is meteorologists who will then be called upon to expertly convey the complexities of tornadoes and tornado outbreaks to the mass media. The manuscript's target audience includes the authors themselves who claim they have worked with the media and recognize the difference between the media and scientific literature. The peer-review process lends credence to, and provides support for, debunking the "clash" message amongst fellow meteorologists who are the conduits of this improved information to the media, and ultimately the masses. The article is for the entire weather enterprise: students who are learning how the atmosphere works, scientists as a reminder not to fall into slick-sounding but inaccurate soundbites, and the members of the broadcast media to not allow themselves to use these soundbites either. Each different component of our audience will take away from our article what they want and what they need. No change. The second issue is related to the first and presents a bit more work. To more fully support the hypothesis that the "clash" interpretation in the horizontal plane is patently false with respect to tornado outbreaks, additional evidence should be provided to the reader. In particular, a couple claims in the manuscript need references: On page 4, line 78: "The reality is that air masses "clash" all the time, but such a situation rarely produces tornadoes." And on page 5, line 102: "...the mere presence of those gradients on the synoptic scale is no guarantee that these ingredients will be brought together to produce tornadoes in any specific extra-tropical cyclone." If the intention of the authors is to convince other meteorologists reading BAMS that "clash of the air masses" (at least in the horizontal plane) should be sent to the dustbin of poor scientific explanation, then there is a need to define and investigate a climatology of horizontal temperature gradients and their relationship to tornado outbreaks. At a minimum, the authors should provide examples of horizontal temperature gradients analyzed for tornado outbreak cases and then use that analysis to show the relatively frequency of those gradients existing in the absence of tornado outbreaks. The evidence against the "clash" claim (in the horizontal) should be provided in sufficiently technical detail to establish a more convincing argument that will resonate with the meteorological community. Such a piece of research is outside the scope of this article. Although an interesting study, that would take this article well away from its intended purpose. No change. With a better description of who the information in the manuscript is directed at (meteorologists instead of "the media"), and the inclusion of detailed analyses of horizontal temperature gradients, their frequency, and their association with tornado outbreaks, the manuscript will be far more appropriate for the readership of AMS BAMS. Thank you for your comments. They have improved our manuscript. Figure 1 Click here to download Non-Rendered Figure: Fig-001-F4-days.eps Figure 2 Click here to download Non-Rendered Figure: ShukmanTweet.tif Figure 3 Click here to download Non-Rendered Figure: 3S0K4229_4.tif Copyright Form 1 Click here to download Copyright Form: AMS-copyright.pdf Copyright Form 2 Click here to download Copyright Form: CopyrightForm.pdf.PDF Page Charge Estimate Form Click here to download Page Charge Estimate Form: p10.pdf
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