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1.
利用2012—2019年新疆伊犁河谷10个气象站逐小时降水资料,分析该区域不同季节降水的日变化特征。结果表明:(1)伊犁河谷春季、夏季和冬季的累计降水量日变化呈单峰型,秋季呈双峰型。四季累计降水量日变化的低值都出现在下午(15:00—19:00),高值时段在春季、秋季和冬季的上午(10:00—12:00),夏季高值出现在前半夜(22:00)。(2)同一季节累计降水频次和累计降水量的日变化特征类似,逐时平均降水量和降水频次峰值的空间分布均存在明显区域差异。(3)伊犁河谷四季均以短历时降水事件为主,该类事件在夏季出现比例最高(89%),冬季出现比例最低(70%),且短历时降水事件是夏季总降水量的主要贡献者,而长持续性降水事件是冬季总降水量的主要贡献者。(4)伊犁河谷四季降水的日循环与降水的持续性之间都存在密切关系,其中持续2～8 h和1～4 h的降水事件是春季和夏季降水量日变化峰值的主要贡献者,不同持续时间降水事件对秋季和冬季降水量日变化峰值的贡献大致相等。  相似文献   

2.
基于临夏州2006—2018年4—9月自动气象站逐日小时降水量,在传统降水百分位法、Z指数法和平方根变换法3种方法中,确定了短时强降水阈值的最佳计算方法,在此基础上分析临夏州短时强降水的时空分布特征。平方根变换法确定的临夏州短时强降水阈值为14.6 mm·h^(-1)。临夏州短时强降水空间分布表现为自中南部分别向西北和东南减少,短时强降水年平均出现次数为7.3次,2018年出现次数最多;7—8月短时强降水出现频次最多,占短时强降水总频次的81.1%,8月达到最高峰,占总频次的55.8%;短时强降水日变化呈4峰分布,短时强降水主要出现在18:00—23:00,占短时强降水总频次的55.8%;小时最大降水量为55.8 mm,出现在22:00;短时强降水持续时间为1 h的占90.5%,同一时次出现1站次短时强降水的占93.3%,临夏州短时强降水多为阵发性,且空间分布多为孤立零散。  相似文献   

3.
李强  邓承之  张勇  何跃  邹倩  何慧根 《气象》2017,43(9):1073-1083
利用四川和重庆123个气象观测站1980—2012年小时降水资料,分析川渝地区主汛期5—9月小时强降水频次、强度和持续性等时间演变和空间分布特征。结果表明,≥20、≥30和≥50 mm·h-1三种强度阈值强降水时间演变上,1980—2012年年际和日变化具有较好的一致性,三种强降水年平均频次分别为504、184和28次。≥20 mm·h-1 强降水空间分布上,在山地地形动力辐合抬升,以及盆地西部较大的地形梯度作用下,≥20 mm·h-1强降水高频次区主要分布于盆地西北部的龙山山脉、西南部雅安及乐山周围与盆地过渡区。≥20 mm·h-1强降水频次的日峰值空间分布上,盆地南部主要出现在20:00—01:00（北京时,下同）,而盆地中部、北部和东部主要在02:00—07:00。持续不同小时时间尺度的强降水事件日变化上,具有双峰型结构,午后为第一个降水峰值,20:00至第二天07:00为第二个峰值,白天多为短时间（2~6 h）强降水事件,而傍晚开始至第二天清晨,持续2~18 h强降水事件均有发生。不同开始时间强降水事件的强度与频次和降水量具有一致性的日变化特征,呈现单峰型结构,峰值主要发生在18:00—06:00,且不同开始时间事件频次和降水量空间分布上,白天（09:00—20:00）相对于夜间（21:00—08:00）偏小,即夜间强降水事件特征表现明显。  相似文献   

4.
利用唐山2006—2013年区域自动站降水资料,分析了夏季降水和短历时强降水的日变化特征。结果指出,与一般性降水相比,短历时强降水更具夜间多发性,夜间降水量占总降水量的66.4%,降水量和降水频次日变化呈单峰结构,峰值出现在凌晨,谷值出现在午后,降水强度呈双峰结构,峰值出现在午后和凌晨,且8 a间夜间短历时强降水呈上升趋势。短历时强降水日变化特征地区差异较大,东北部出现频次最多,西南部频次最少、降水强度最大。唐山东北部呈簸箕状,西北东三面环山,强降水过程多东南风,迎风坡抬升加强上升运动,使其出现频次明显偏多;西南部临海,水汽条件比东北部好,故降水强度最大。东北部午后16时(北京时)的降水次峰值与西南部凌晨04时的峰值成因与海陆风昼夜变化关系密切。  相似文献   

5.
2008～2016年重庆地区降水时空分布特征   总被引：1，自引：0，他引：1  
利用2008~2016年国家气象信息中心提供的0.1°分辨率的中国地面与CMORPH融合逐小时降水产品,分析了重庆地区的降水时空分布特征,尤其是小时强降水的时空分布特征。结果表明:(1)年均降水量总体呈西低东高分布,大值中心位于重庆东北和东南部,且存在一定的季节性差异,特别是夏季,西部降水明显增强,总降水呈两高(西部、东部)一低(中部)的分布;降水频次、降水强度与地形的相关性较高,海拔高度较高的山区(海拔高度>1000 m)降水频次多大于盆地和丘陵区(海拔高度<1000 m),降水强度与之相反,且小时强降水多发生在迎风坡前侧的过渡区域,说明高海拔区域易出现降水,但降水强度不强,而地形抬升则是触发强降水的重要原因,导致山前降水明显大于山峰。(2)重庆地区降水主要集中在5~9月,降水量、降水强度和小时强降水频次均呈单峰型分布,峰值出现在6~7月,降水频次呈双峰型分布,一个峰值出现在5~6月,另一个峰值出现在10月,7~8月为低频期,与副高控制下的连晴高温天气有关。(3)重庆地区降水存在明显的日变化特征,降水以夜雨为主,且降水峰值出现时间表现为向东延迟的特征,重庆西部日峰值出现在凌晨02:00(北京时,下同),中部出现在清晨05:00,东北部出现在早上08:00。从不同季节来看,春季、秋季和冬季降水日变化呈单峰型分布,主要集中在清晨,而夏季受午后局地对流性天气的影响,在下午17:00左右存在一个次峰值。(4)强降水的主要集中在夏季,在空间上存在三个大值中心,受西南涡及地形的相互作用,夏季在缙云山以西的盆地区域,小时强降水频次明显较高。  相似文献   

6.
基于甘肃省81个自动气象站2002—2012年逐小时降水数据,分析了甘肃省近11 a来短时强降水的时空变化特征。结果表明:短时强降水频次自甘肃省西北向东南逐步递增,陇东南地区是甘肃省短时强降水发生频次最多、强度最强的地区。短时强降水存在2个高发中心,一个在以合水为中心的陇东地区,另一个在以徽县为中心的徽成盆地。短时强降水主要发生在午后至前半夜,出现时段集中在16:00—00:00,17时前后是短时强降水天气高发时段。短时强降水主要出现在5—9月,其中7—8月是一年中出现最多的月份,其次是6月。近11 a来,短时强降水频次呈上升趋势,2006年和2010年出现了2个峰值,其中2010年最多,发生52次,2004年最少只有17次。  相似文献   

7.
利用四川地区自动气象站逐小时降水观测资料,分析了2010~2019年5~9月短时强降水事件24h累计降水量、频次和强度的时空分布特征,探讨了短时强降水事件发生的频次、极值分布及其与地形、海拔高度等的关系。结果表明:四川地区平均24h累计降雨量基本在50mm以上,盆地东北部、西南部、南部及阿坝州东部甚至超过100mm,最大值出现在广安,达175mm。四川地区短时强降水事件开始时间的日变化特征表现为“V”型结构的夜间峰值位相,事件持续时段多为傍晚至凌晨,时长可达10h以上,最长甚至可持续22h。在强降水事件极值的日变化上,极大值频次和降水量呈单峰结构,在03时达到最大,其后逐渐减小至15时达到谷值,而后再次增大;降水强度呈弱双峰结构,分别在04时和16时达到谷值,13时和18时达到峰值,其日变化呈“增-减-增-减”的特征。四川短时强降水事件与复杂地形有密切的关系,5~6月事件活跃区在四川盆地中部,7月在盆地西部的龙门山脉一带,8月在雅安、乐山附近,9月在盆地北部且频次明显减少;短时强降水事件的最大小时雨强可达80mm以上,出现在7~8月的盆地西部龙门山一带和南部地区。短时强降水事件随着海拔高度的增加,发生频次和日数逐渐减少,海拔2000m以上地区基本无强降水发生日出现( 峨眉山气象站例外)。   相似文献   

8.
粤北暴雨中心的降水气候特征分析   总被引：1，自引：0，他引：1  
基于广东省1967—2018年气象观测站和2003—2018年自动监测站降水数据,统计分析了粤北暴雨中心的降水气候统计特征。结果表明:(1)粤北暴雨中心范围主要集中在清远南部-广州东北部-惠州北部,最大年平均降水量(2 488. 6 mm)和强降水日数(12. 3 d)均出现在龙门的南昆山,特殊地形分布特征与粤北暴雨中心形成密切相关;(2)从化和增城降水年际变化呈较明显增多趋势,其余变化趋势不明显;中心区域内降水主要集中在汛期(4—9月),而前汛期(4—6月)降水量约占汛期的60%～70%;(3)降水月变化呈单峰型分布,峰值出现在5—6月;(4)降水日变化特征与降水性质密切相关,5—6月季风影响期间降水概率显著增加,夜雨和白天降水均明显;短时强降水出现概率集中在5—6月08:00、15:00和21:00前后。  相似文献   

9.
利用2010—2018年夏季阿勒泰地区112个自动气象站逐时降水资料,采用常规统计方法分析了阿勒泰地区夏季短时强降水时空分布特征。结果表明,2010—2018年夏季阿勒泰地区短时强降水的空间分布极不均匀,主要发生在阿尔泰山和沙吾尔山迎风坡、地形陡升区、喇叭口地形、戈壁和乌伦古湖交界区等复杂地形附近;发生次数年际变化大,2017年出现最多达95次,2010年出现最少为10次;极大值出现在2017年6月30日15:00哈巴河县合孜勒哈克村（37.5 mm/h）,极小值出现在2015年8月9日17:00福海县工业园区（22.5 mm/h）。旬、日发生频次变化均呈单峰型,旬峰值出现在7月上旬,日高峰值时段出现在午后至傍晚（19时左右）;各站短时强降水持续时间为1—2 h,区域性短时强降水最长持续时间为5 h;2017年短时强降水出现最多、持续时间最长、范围最广、强度最强。  相似文献   

10.
利用丽水地区2004—2014年的加密气象观测站的逐小时降水观测资料,统计分析了丽水地区短时强降水的时空分布特征,同时结合当地地理环境特征,对时空分布特征的成因进行了分析。结果表明:空间上,丽水地区短时强降水主要存在两个活跃区,分别位于东南部地区与西南部高山地区,地形陡峭区、喇叭口等特殊地形有助于短时强降水的发生;小时雨量最大的站点紧邻水库。时间上,从月分布特征来看,丽水地区短时强降水主要发生在5—9月,受汛期降水与热带天气系统影响,峰值分别出现在6月与8月;从日变化特征来看,丽水地区短时强降水主要呈现三峰分布特征,包括一个显著峰值与另外两个不显著峰值,其中主峰发生在午后14:00—22:00,次峰分别在03:00和08:00,不同季节日变化峰值略有不同。此外,小时雨量最大值出现在日落前后,地形导致的局地热力环流对短时强降水有增幅作用。  相似文献   

11.
Precipitation samples were collected by filtrating bulk sampler in Kitakyushu City, Japan, from January 1988 to December 1990. Volume weighted annual mean of pH was 4.93, but the pH distribution indicated that most probable value lay in the range pH 6.0–6.4. Volume weighted annual mean concentrations of major ionic components were as follows; SO 4 2– : 84.2, NO 3 – : 28.1, Cl–: 86.3, NH 4 + : 45.5, Ca2+: 63.3, Mg2+: 27.0, K+: 3.4, Na+: 69.0 µ eq l–1. The highest concentrations of these ionic components were observed in winter and the lowest occurred in the rainy season. The ratio of ex-SO 4 2– /NO 3 – exhibited the lowest ratio in summer, and the highest ratio in winter. Good correlations were obtained between Cl– and Na+, ex-SO 4 2+ and ex-Ca2+, NO 3 – and ex-Ca2+, and NH 4 + and ex-SO 4 2– , respectively. However, no correlation between Cl– and Na+ with Ca2+ was observed. The relationship of H+ with (ex-SO 4 2– + NO 3 – ) - (ex-Ca2+ + NH 4 + ) indicated positive correlation.  相似文献   

12.
High volume bulk aerosol samples were collected continuously at three Antarctic sites: Mawson (67.60° S, 62.50° E) from 20 February 1987 to 6 January 1992; Palmer Station (64.77° S, 64.06° W) from 3 April 1990 to 15 June 1991; and Marsh (62.18° S, 58.30° W) from 28 March 1990, to 1 May 1991. All samples were analyzed for Na+, SO 4 2– , NO 3 – , methanesulfonate (MSA), NH 4 + ,210Pb, and7Be. At Mawson for which we have a multiple year data set, the annual mean concentration of each species sometimes vary significantly from one year to the next: Na+, 68–151 ng m–3; NO 3 – , 25–30 ng m–3; nss SO 4 2– , 81–97 ng m–3; MSA, 19–28 ng m–3; NH 4 + , 16–21 ng m–3;210Pb, 0.75–0.86 fCi m–3. Results from multiple variable regression of non-sea-salt (nss) SO 4 2– with MSA and NO 3 – as the independent variables indicates that, at Mawson, the nss SO 4 2– /MSA ratio resulting from the oxidation of dimethylsulfide (DMS) is 2.80±0.13, about 13% lower than our earlier estimate (3.22) that was based on 2.5 years of data. A similar analysis indicates that the ratio at Palmer is about 40% lower, 1.71±0.10, and more comparable to previous results over the southern oceans. These results when combined with previously published data suggest that the differences in the ratio may reflect a more rapid loss of MSA relative to nss SO 4 2– during transport over Antarctica from the oceanic source region. The mean210Pb concentrations at Palmer and Marsh and the mean NO 3 – concentration at Palmer are about a factor of two lower than those at Mawson. The210Pb distributions are consistent with a210Pb minimum in the marine boundary layer in the region of 40°–60° S. These features and the similar seasonalities of NO 3 – and210Pb at Mawson support the conclusion that the primary source regions for NO 3 – are continental. In contrast, the mean concentrations of MSA, nss SO 4 2– , and NH 4 + at Palmer are all higher than those at Mawson: MSA by a factor of 2; nss SO 4 2– by 10%; and NH 4 + by more than 50%. However, the factor differences exhibit substantial seasonal variability; the largest differences generally occur during the austral summer when the concentrations of most of the species are highest. NH 4 + /(nss SO 4 2– +MSA) equivalent ratios indicate that NH3 neutralizes about 60% of the sulfur acids during December at both Mawson and Palmer, but only about 30% at Mawson during February and March.  相似文献   

13.
Four case studies are described, from a three-site field experiment in October/November 1991 using the Great Dun Fell flow-through reactor hill cap cloud in rural Northern England. Measurements of total odd-nitrogen nitrogen oxides (NO y ) made on either side of the hill, before and after the air flowed through the cloud, showed that 10 to 50% of the NO y , called NO z , was neither NO nor NO2. This NO z failed to exhibit a diurnal variation and was often higher after passage through cloud than before. No evidence of conversion of NO z to NO3 - in cloud was found. A simple box model of gas-phase chemistry in air before it reached the cloud, including scavenging of NO3 and N2O5 by aerosol of surface area proportional to the NO2 mixing ratio, shows that NO3 and N2O5 may build up in the boundary layer by night only if stable stratification insulates the air from emissions of NO. This may explain the lack of evidence for N2O5 forming NO3 - in cloud under well-mixed conditions in 1991, in contrast with observations under stably stratified conditions during previous experiments when evidence of N2O5 was found. Inside the cloud, some variations in the calculated total atmospheric loading of HNO2 and the cloud liquid water content were related to each other. Also, indications of conversion of NO x to NO z were found. To explain these observations, scavenging of NO x and HNO2 by cloud droplets and/or aqueous-phase oxidation of NO2 - by nitrate radicals are considered. When cloud acidity was being produced by aqueous-phase oxidation of NO x or SO2, NO3 - which had entered the cloud as aerosol particles was liberated as HNO3 vapour. When no aqueous-phase production of acidity was occurring, the reverse, conversion of scavenged HNO3 to particulate NO3 -, was observed.  相似文献   

14.
We show that photochemical processes in the lower half of the troposphere are strongly affected by the presence of liquid water clouds. Especially CH2O, an important intermediate of CH4 (and of other hydrocarbon) oxidation, is subject to enhanced breakdown in the aqueous phase. This reduces the formation of HO x -radicals via photodissociation of CH2O in the gas phase. In the droplets, the hydrated form of CH2O, its oxidation product HCO2 –, and H2O2 recycle O2 – radicals which, in turn, react with ozone. We show that the latter reaction is a significant sink for O3. Further O3 concentrations are reduced as a result of decreased formation of O3 during periods with clouds. Additionally, NO x , which acts as a catalyst in the photochemical formation of O3, is depleted by clouds during the night via scavenging of N2O5. This significantly reduces NO x -concentrations during subsequent daylight hours, so that less NO x is available for O3 production. Clouds thus directly reduce the concentrations of O3, CH2O, NO x , and HO x . Indirectly, this also affects the budgets of other trace gases, such as H2O2, CO, and H2.  相似文献   

15.
顶点覆盖问题是经典的NP完全问题,在排序、计算机网络等现实生活中有许多的应用.近几年来,许多研究者开始探究它的推广形式——顶点Pk覆盖（VCPk）问题,即寻找一个顶点子集,从拓扑结构图中删除后使得剩下的顶点导出的子图不包含Pk路,其中Pk是指包含k个顶点的路.本文简单介绍了VCPk问题的应用背景,归纳了它在近似算法、精确算法、参数化算法3个方面的主要研究进展,并分析了一些主要的方法和技巧.在此基础上,对VCPk问题及其相关问题的研究前景进行了展望.  相似文献   

16.
The photochemical oxidation of SO2 in the presence of NO and C3H6 was studied in a 18.2 liter pyrex reactor. When light intensity, irradiation time and SO2 concentration were constant, SO4 2- concentration, derived from the total volume of aerosol produced, peaked when [C3H6]/[NO] was approximately 6.0. Another increase im SO4 2- formation was reached at very high ratios (>50). The experimental observations are consistent with the two SO2 oxidation mechanisms. At low [C3H6]/[NO] ratios, the processes proceed via the HO–SO2 reaction, while at high ratios the O3–C3H6 adduct is assumed to oxidize SO2 to produce SO4 2- aerosols.  相似文献   

17.
Rate constants for the gas-phase reactions of OH radicals, NO3 radicals and O3 with the C7-carbonyl compounds 4-methylenehex-5-enal [CH2=CHC(=CH2)CH2CH2CHO], (3Z)- and (3E)-4-methylhexa-3,5-dienal [CH2=CHC(CH3)=CHCH2CHO] and 4-methylcyclohex-3-en-1-one, which are products of the atmospheric degradations of myrcene, Z- and E-ocimene and terpinolene, respectively, have been measured at 296 ± 2 K and atmospheric pressure of air using relative rate methods. The rate constants obtained (in cm3 molecule–1 s–1 units) were: for 4-methylenehex-5-enal, (1.55 ± 0.15) × 10–10, (4.75 ± 0.35) × 10–13 and (1.46 ± 0.12) × 10–17 for the OH radical, NO3 radical and O3 reactions, respectively; for (3Z)-4-methylhexa-3,5-dienal: (1.61 ± 0.35) × 10–10, (2.17 ± 0.30) × 10–12, and (4.13 ± 0.81) × 10–17 for the OH radical, NO3 radical and O3 reactions, respectively; for (3E)-4-methylhexa-3,5-dienal: (2.52 ± 0.65) × 10–10, (1.75 ± 0.27) × 10–12, and (5.36 ± 0.28) × 10–17 for the OH radical, NO3 radical and O3 reactions, respectively; and for 4-methylcyclohex-3-en-1-one: (1.10 ± 0.19) × 10–10, (1.81 ± 0.35) × 10–12, and (6.98 ± 0.40) × 10–17 for the OH radical, NO3 radical and O3 reactions, respectively. These carbonyl compounds are all reactive in the troposphere, with daytime reaction with the OH radical and nighttime reaction with the NO3 radical being predicted to dominate as loss processes and with estimated lifetimes of about an hour or less.  相似文献   

18.
To investigate the stability of the bottom boundary layer induced by tidal flow (oscillating flow) in a rotating frame, numerical experiments have been carried out with a two-dimensional non-hydrostatic model. Under homogeneous conditions three types of instability are found depending on the temporal Rossby number Rot, the ratio of the inertial and tidal periods. When Rot < 0.9 (subinertial range), the Ekman type I instability occurs because the effect of rotation is dominant though the flow becomes more stable than the steady Ekman flow with increasing Rot. When Rot > 1.1 (superinertial range), the Stokes layer instability is excited as in the absence of rotation. When 0.9 < Rot < 1.1 (near-inertial range), the Ekman type I or type II instability appears as in the steady Ekman layer. Being much thickened (100 m), the boundary layer becomes unstable even if tidal flow is weak (5 cm/s). The large vertical scale enhances the contribution of the Coriolis effect to destabilization, so that the type II instability tends to appear when Rot > 1.0. However, when Rot < 1.0, the type I instability rather than the type II instability appears because the downward phase change of tidal flow acts to suppress the latter. To evaluate the mixing effect of these instabilities, some experiments have been executed under a weak stratification peculiar to polar oceans (the buoyancy frequency N2  10−6 s−2). Strong mixing occurs in the subinertial and near-inertial ranges such that tracer is well mixed in the boundary layer and an apparent diffusivity there is evaluated at 150–300 cm2/s. This suggests that effective mixing due to these instabilities may play an important role in determining the properties of dense shelf water in the polar regions.  相似文献   

19.
Products and mechanisms for the gas-phase reactions of NO3 radicals with CH2=CHCl, CH2=CCl2, CHCl=CCl2,cis-CHCl=CHCl andtrans-CHCl=CHCl in air have been studied. The experiments were carried out at 295±2 K and 740±5 Torr in a 480-L Teflon-coated reaction chamber and at 295±2 K and 760±5 Torr in a 250-L stainless steel reactor. NO3 was generated by the thermal dissociation of N2O5. Experiments with15NO3 and CD2CDCl have also been performed. The initially formed nitrate peroxynitrates decay into carbonyl compounds, nitrates, HCl and ClNO2. In adidtion, there are indications of nitrooxy acid chlorides being produced. The reactions with CH2=CCl2 and CHCl=CCl2 are more complex due to release of chlorine atoms which eventually lead to formation of chloroacid chlorides.A general reaction mechanism is proposed and the observed concentration-time profiles of reactants and products are simulated for each compound. The rate constants for the initial step of NO3 addition to the chloroethenes are determined as: (2.6±0.5, 9.4±0.9, 2.0±0.4 and 1.4±0.4) × 10–16 cm3 molecule–1 s–1 for CH2=CHCl, CH2=CCl2, CHCl=CCl2 andcis-CHCl=CHCl, respectively.  相似文献   

20.
以3个花生品种（开农49号、64号和69号）为材料,通过大田模拟试验,研究UV-B辐射增强对花生结荚期叶片的净光合速率（Pn）、气孔导度（Gs）、胞间CO2浓度（Ci）、蒸腾速率（Tr）和水分利用效率（Ewu）日变化的影响,为筛选高产、抗旱、抗UV-B辐射花生品种提供依据.UV-B辐射设2个水平即自然光（CK,1.5 kJ·m-2）和UV-B增强20%（T,1.8 kJ·m-2）.结果表明,UV-B辐射增强明显抑制花生的光合作用和蒸腾作用,与对照相比,UV-B增强条件下,开农49号、64号和69号Pn日均值分别降低19.4%、27.8%、24.7%;Gs日均值降低26.7%、42.9%、28.6%;Ci日均值降低27.2%、20.4%、23.1%;Tr日均值降低17.8%、23.3%、25.1%;Ewu日均值降低16.6%、23.2%、23.9%.UV-B辐射增强对3个品种生长都具有抑制效应,但品种间存在一定的敏感性差异,其中开农49号最不敏感,因此,开农49号在抗UV-B辐射方面比其他2个品种具有更大的优势.  相似文献   

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