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1.
内蒙古气象局气象为构建社会主义和谐社会服务调研领导小组 《内蒙古气象》2008,(1):3-7
党的十六届六中全会作出《中共中央关于构建社会主义和谐社会若干重大问题的决定》,是党中央顺应历史发展变化,全面分析和把握我国发展面临的机遇和挑战,为推进中国特色社会主义伟大事业作出的重大战略举措。构建社会主义和谐社会,对气象部门提出了新的更高的要求,是各级气象部门义不容辞的职责。为充分发挥气象科技业务服务在构建和谐社会中的作用,认真贯彻党中央关于构建和谐社会的重大战略部署,按照中国气象局党组的要求,内蒙古气象部门就气象为构建社会主义和谐社会服务工作开展了深入、细致的调查研究,现报告如下。 相似文献
2.
党的十四次代表大会在总结我国14年改革开放伟大实践的基础上,提出了建立社会主义市场经济体制的改革目标模式。这一理论上和认识上的重大突破,必然给气象部门当前“以气象事业结构调整和建立完善相应运行机制为重点”的深化改革提供新的外部环境。希望与困难同在,机遇和挑战并存。“抓住时机、深化改革、加速发展”是摆在各级气象部门面前的中心任务。笔者通过学习建设有中国特色社会主义的理论,提出一些不成熟的思考,旨在与基层台站能够在某些方面取得共识。 相似文献
3.
文章以金坛市气象局实践探索为研究案例,对党的建设、文化建设和廉政建设与气象层级,确立气象部门党的建设、文化建设和廉政建设主项,气象部门党的建设、文化建设和廉政建设向度,建构气象部门党的建设、文化建设和廉政建设范式四个问题进行研究,探索和建立气象部门科学、客观、系统的党的建设、文化建设和廉政建设的空间与范式取舍体系。 相似文献
4.
帕尔哈特 《沙漠与绿洲气象(新疆气象)》1999,22(5):40-42
党的十四届六中全会指出:建设社会主义精神文明,关系跨世纪宏伟蓝图的全面实现,关系我国社会主义事业的兴旺发达。十一届三中全会以来,新疆气象部门大力加强社会主义精神文明建设,坚持改革开放,积极推动气象事业现代化建设,成功地走出了一条有气象特色、有新疆特色的气象事业的发展路子,促进了新疆气象事业发展。王新回气象部门社会主义征神文明建设的回顾和主要成组建设社会主义精神文明,创建文明气象行业,是新疆气象部门一项跨世纪的战略任务。多年来,新疆气象部门的精神文明建设有了很大的发展,取得了丰硕的成果。在建国50周… 相似文献
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正1黑龙江省气象科技服务的现状近年来,黑龙江省气象服务中心以新发展理念为统领,围绕全面推进气象现代化、全面深化气象改革、全面推进气象法治建设和全面加强气象部门党的建设四项重点任务,主动适应经济发展新常态,认真分析公共气象服务发展面临的新形势、新需求,深化气象服务供给侧改革,着力解决关键问题和重点难点问题,在开拓具有龙江特色的公共气象服务方面取得了一定成绩。 相似文献
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提高气象系统经济实体效益刍议席国耀气象部门兴办经济实体,是适应改革和建立社会主义市场经济的需要,是发展中国特色气象事业的需要。气象部门是一个从事高科技公益服务、依靠国家财政全额拨款的事业单位。但近年来由于国家财政困难,气象事业费增加较少,国家主渠道拨... 相似文献
9.
今年1月在京召开的全国气象部门精神文明建设工作会议指出:深刻理解社会主义精神文明建设的战略地位.必须坚持全面的、历史的、发展的观点,把精神文明建设放在建设有中国特色社会主义整个事业的大局和整个世界的大局中来认识。 相似文献
10.
前言社会主义市场经济的建立,促使气象部门向多元化方向发展,气象部门发展以高新技术产业为重点的综合经营是建设有中国特色社会主义气象事业的重要标志之一,也是气象部门走向市场,为社会提供服务的进一步拓宽和发展。建立新型的气象事业结构是气象部门发展战略决策之一,全国各级气象部门深入贯彻改革开放的方针,初步建立了“三大块”事业结构的运行机制,坚持发展以高新技术产业为重点的综合经营体系也将逐步形成。目前气象部门的高新技术产业及以气象科技产品精加工的信息产业已有了长足发展,取得了较好的经济效益,同时为产业发展… 相似文献
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The kinetics of the aqueous phase reactions of NO3 radicals with HCOOH/HCOO– and CH3COOH/CH3COO– have been investigated using a laser photolysis/long-path laser absorption technique. NO3 was produced via excimer laser photolysis of peroxodisulfate anions (S2O
8
2–
) at 351 nm followed by the reactions of sulfate radicals (SO
4
–
) with excess nitrate. The time-resolved detection of NO3 was achieved by long-path laser absorption at 632.8 nm. For the reactions of NO3 with formic acid (1) and formate (2) rate coefficients ofk
1=(3.3±1.0)×105 l mol–1 s–1 andk
2=(5.0±0.4)×107 l mol–1 s–1 were found atT=298 K andI=0.19 mol/l. The following Arrhenius expressions were derived:k
1(T)=(3.4±0.3)×1010 exp[–(3400±600)/T] l mol–1 s–1 andk
2(T)=(8.2±0.8)×1010 exp[–(2200±700)/T] l mol–1 s–1. The rate coefficients for the reactions of NO3 with acetic acid (3) and acetate (4) atT=298 K andI=0.19 mol/l were determined as:k
3=(1.3±0.3)×104 l mol–1 s–1 andk
4=(2.3±0.4)×106 l mol–1 s–1. The temperature dependences for these reactions are described by:k
3(T)=(4.9±0.5)×109 exp[–(3800±700)/T] l mol–1 s–1 andk
4(T)=(1.0±0.2)×1012 exp[–(3800±1200)/T] l mol–1 s–1. The differences in reactivity of the anions HCOO– and CH3COO– compared to their corresponding acids HCOOH and CH3COOH are explained by the higher reactivity of NO3 in charge transfer processes compared to H atom abstraction. From a comparison of NO3 reactions with various droplets constituents it is concluded that the reaction of NO3 with HCOO– may present a dominant loss reaction of NO3 in atmospheric droplets. 相似文献
14.
K. Zeller 《Meteorology and Atmospheric Physics》1950,2(4):401-403
Zusammenfassung A. undE. Vassy haben in der Frage der Temperatur-abhängigkeit des Ozongehalts der Atmosphäre aus der Gleichung loge
n
–logJ
n
logK(T
n
) geschlossen, daß auch die Gleichung loge
n
logJ
n
+logK(T
n
) gültig sei. Es wird hier nun gezeigt, daß die bei der ersten Gleichung erlaubten Vernachlässigungen bei der zweiten zu großen Fehlern führen können und daß daher von A. undE. Vassy kein Beweis für die Richtigkeit der Beziehunge=J.K(T) erbracht ist.
Summary In the question of temperature dependence of ozone content of the atmosphere A. andE. Vassy have concluded from the equation loge n –logJ n logK(T n ) that also the formula loge n logJ n +logK(T n ) must be valid. In this paper it is proved that the neglections which may be admitted for the first equation, can conduct to great errors. Therefore A. andE. Vassy have not produced a proof for the correctness of the equatione=J.K(T).
Résumé A. etE. Vassy en étuidant le problème de la teneur de l'ozone atmosphérique en relation avec la température ont admis que l'équation loge n –logJ n logK(T n ) entraînait aussi la relation loge n logJ n +logK(T n ). On montre ici que les simplifications admises pour la première équation conduisent pour l'application de la seconde à de fortes erreurs, et que par conséquent ces auteurs n'ont pas fourni de preuve de la justesse de la relatione=J.K(T).相似文献
15.
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
16.
Summary ?Above orographically structured terrain considerable differences of the regional wind field may be identified during large-scale
extreme wind events. So far, these regional differences could not be resolved by climate models. To determine the relationships
between large-scale atmospheric conditions, the influence of orography, and the regional wind field, data measured in the
upper Rhine valley within the framework of the REKLIP Regional Climate Project were analyzed and calculations were made using
the KAMM mesoscale model. In the area of the upper Rhine valley, ratios of the wind velocity in the Rhine valley at 10 m above
ground level, νval, and the large-scale flow velocity, νlar, are between νval/νlar ≈ 0.1 and νval/νlar ≈ 1. The νval/νlar ratio exhibits a strong dependence on thermal stratification, δ, and decreases from νval/νlar ≈ 1 at δ = 0 K m−1 to νval/νlar ≈ 0.2 at δ = 0.0075 K m−1. In areas, where the lateral mountainous border of the Rhine valley is interrupted, the νval/νlar ratio increases again with increasing stability or decreasing Froude number. This is obviously due to flow around the Black
Forest under stable stratification. It is demonstrated by model calculations that a complex wind field develops in the Rhine
valley at small Froude numbers (Fr < 1) irrespective of the direction of large-scale flow. The νval/νlar ratio is characterized by small values in the direct lee side (νval/νlar ≈ 0.2) and high values on the windward side of the lateral mountainous border of the Rhine valley (νval/νlar ≈ 0.8).
Received October 22, 2001; revised June 18, 2002; accepted June 23, 2002 相似文献
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18.
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
19.
Heinz Reuter 《Meteorology and Atmospheric Physics》1956,9(4):433-438
Zusammenfassung Eine Überprüfung der vonNamias abgeleiteten Formel zur Konstruktion sogenannter Trendkarten an Hand 20 ausgewählter Höhenkarten in der Zeit vom November 1955 bis Mai 1956 ergab eine vollkommene Bestätigung der vonNamias für Amerika angegebenen Korrelationskoeffizienten und des Faktors der entsprechenden Regressionsgleichung für den mitteleuropäischen Raum, obwohl die Untersuchungen sich auf die 850 mb-Topographie bezogen zum Unterschied vonNamias, der die 700 mb-Fläche zugrunde legte. Durch eine sinngemäße Kombination der in der synoptischen Praxis üblichen Konstruktionsmethode für 24 stündige Vorhersagekarten mit statistischen Überlegungen über die Abweichungen vom Normalwert gelingt die Ableitung einer Prognosenformel für eine dreitägige Mittelkarte, die als Grundlage für mittelfristige Wetterprognosen (Halbwochenprognosen) Verwendung findet. Die Formel weist gegenüber der Trendformel vonNamias den Vorteil auf, daß sie mit praktisch derselben Treffergenauigkeit einen wesentlich größeren Vorhersagezeitraum erfaßt.
Herrn Prof. Dr.H. Ficker zum 75. Geburtstag gewidmet. 相似文献
Summary Using 20 different contour charts during the period from November 1955 to May 1956 the formula for the construction of socalled trendcharts, primarily derived byNamias, has been verified for Central Europe though the investigations were based upon data from the 850 mb-level instead of the 700 mb-level used byNamias. Through a combination of the synoptic method for construction of forecast maps 24 hours in advance with statistic considerations about the departure from normals a formula is finally derived for a forecast of a three day mean chart. This formula has been successfully used for an extended forecast half week in advance. The described method shows an essential improvement upon theNamias procedure since a much greater forecast period can be obtained with almost the same accuracy.
Résumé La formule établie parNamias en vue de construire les cartes d'évolution a fait l'objet d'un examen critique fondé sur la discussion de vingt cartes d'altitude de la période de novembre 1955 à mai 1956. Les valeurs des coefficients de corrélation données par cet auteur pour l'Amérique du Nord ainsi que le coefficient de l'équation de régression correspondante ont été confirmés pour l'espace européen, bien que les topographies étudieés n'aient pas été les mêmes (850 mb au lieu de 700 mb). Combinant les méthodes usuelles de construction des cartes de prévision de vingt-quatre heures à des critères statistiques d'écart à la normale, l'auteur établit une formule de prévision destinée à calculer une carte moyenne de trois jours servant de base à la prévision à moyenne échéance. Cette formule présente sur celle deNamias l'avantage d'atteindre une plus longue période de prévision avec une égale exactitude.
Herrn Prof. Dr.H. Ficker zum 75. Geburtstag gewidmet. 相似文献
20.
F. Möller 《Meteorology and Atmospheric Physics》1954,7(1):158-169
Zusammenfassung Für eine Reihe von Atmosphärenmodellen, die untereinander gleiche Temperaturschichtung und konstante relative Feuchtigkeit, aber verschieden hohe Temperatur und Feuchtigkeit im festen Niveau haben, wird der NettostrahlungsstromE in 400 mb und am Boden durch Berechnungen in den bekannten Strahlungsdiagrammen bestimmt. Es läßt sich zeigen, daßE
400 (E
B
) als Funktion der Temperaturt
400 (t
B
) und der Feuchtigkeit bzw. des Taupunktes
400 (
B
) dargestellt werden kann [Abb. 1 und 3, Gl. (1) und (3)], ählich, wie das für die effektive Strahlung des BodensE
B
bereits früher durch die Formeln vonÅngström, Brunt u. a. geschehen ist. Wolkenschichten können durch Korrektionsfaktoren berücksichtigt werden. Die Abweichungen zwischen den so gewonnenen Strahlungssummen und den durch Planimetrieren im Strahlungsdiagramm berechneten sind im Durchschnitt kleiner als 3,5% (11%), für die Differenz E=E
400–E
B
sind sie kleiner als 6%.
Mit 4 Textabbildungen. 相似文献
Summary For a series of model atmospheres which have the same stratification of temperature and constant relative humidity but different temperatures and humidities at a fixed level, the net radiation fluxE at 400 mb and at the surface are determined by computations in the well known radiation charts. It is shown thatE 400 (E B ) can be represented as a function of the temperaturet 400 (t B ) and humidity resp. dew point 400 ( B ) [Fig. 1 and 3, formula (1) and (3)], in a similar manner as the outgoing radiationE B is already approximated by the formulae ofÅngström, Brunt, a. o. Cloud layers may be accounted for by correction factors. The differences between the radiation fluxes found in this way and those computed by integration in a radiation chart are in the average smaller than 3.5% (11%); with E=E 400–E B , the differences are smaller than 6%.
Résumé Pour plusieurs modèles de l'atmosphère qui ont la même structure par rapport à la température et une humidité relative constante, mais à un niveau fixe des températures et humidités différentes, on calcule à l'aide de diagrammes de radiation connus le flux net de radiationE pour 400 mb et au sol. On peut montrer queE 400 (E B ) peut être représenté comme fonction de la températuret 400 (t B ) et de l'humidité, resp. du point de rosée 400 ( B ) [Fig. 1 et 3, formules (1) et (3)], tout comme cela a déjà été fait pour la radiation effective au solE B grâce aux formules d'Ångström, deBrunt et d'autres. Par un facteur de correction on tient compte des couches de nuages. Les écarts entre les sommes de radiation ainsi obtenues et celles calculées à l'aide des diagrammes de radiation sont en moyenne plus petits que 3,5% (11%), la différence E=E 400–E B ne dépasse pas 6%.
Mit 4 Textabbildungen. 相似文献