1999年和2000年夏季南极菲尔德斯半岛N_2O浓度对比

1999与 2 0 0 0年夏季对南极菲尔德斯半岛不同地点大气中 N2 O浓度进行了监测 ,分析了苔藓植被区 N2 O浓度季节变化特征 ;2 0 0 0年夏季该植被区 N2 O浓度均值为 ( 31 0 .7± 4.4)×1 0 - 9(体积百分比 ) ,比 1 999年的 ( 32 1 .9± 3.3)× 1 0 - 9约低 1 1× 1 0 - 9;阿德雷岛企鹅滩及其沙坝处N2 O浓度变化趋势与苔藓植被区相一致 ,浓度均值分别为 ( 31 2 .4± 5 .1 )× 1 0 - 9和 ( 31 2 .7± 5 .3)× 1 0 - 9,比 1 999年约低 9× 1 0 - 9;另外 ,不同地点大气中 N2 O浓度普遍比 1 999年低 ,但整体变化规律相似 :各考察站区 N2 O浓度普遍高于无人区 ;唯一例外的是企鹅聚集区 N2 O浓度却高于各考察站区 ,暗示了企鹅及其排泄物、人为源是南极大气中 N2 O主要的源。本文初步探讨了 N2 O浓度异常降低的原因     

1999/2000年夏季南极普里兹湾及湾口区叶绿素a和初级生产力

20 0 0年 1月 1 9日至 2 7日在 70°3 0′E- 75°3 0′E,6 2°S以南的南极普里兹湾近岸陆架区的陆隆向深海区设三条纵断面进行浮游生物现存量、真光层深度和光合作用速率的现场观测。并在冰间湖站 - 1 2进行连续昼夜观测。结果表明 ,观测海区叶绿素 a浓度高值位于近岸海湾、冰间湖和测区中部的陆坡区 ;陆坡中部站 - 6和 - 8,0 - 5 0 m的浅水层为叶绿素 a高值区 (2 .1 6- 5 .0 8μg/dm3 )。各测站平均叶绿素 a浓度 2 5 m次表层 (1 .49± 1 .6 1 μg/dm3 )高于表层 (1 .1 4±1 .1 9μg/dm3 ) ,5 0 m以下更深层的浓度随深度的增加而降低 ,2 0 0 m层叶绿素 a浓度仅 0 .0 3±0 .0 2μg/dm3 。昼夜观测结果表明表层叶绿素 a浓度在南极夏季的午后出现最大值 ,晨间出现最小值 ;2 5 m以浅水层的叶绿素 a浓度明显高于深层水 ,与封冰消融冰藻的释放有关。测区真光层潜在初级生产力为 0 .76 - 1 2 .5 9mg C/(m3· h) ,平均值为 4.0 1± 4.0 7mg C/(m3· h) ;海湾和陆架区现场生产力均超过 1 .5 g C/(m2 · d) ,陆坡、深海区约 0 .5 g C/(m2 · d)。高生产力位于高生物量的近岸海湾、陆架冰间湖区。光合作用同化数在 0 .88- 3 .1 0 mg C/(mg Chla· h)。表层叶绿素a浓度与海水中溶解氧浓度呈紧密相关 (Y=0 .0 5 9X     

1998/1999年南极夏季普里兹湾及北部海区叶绿素a和初级生产力的分布特征

1998 /1 999年南极夏季 ,作者随“雪龙船”在南极普里兹湾及其北部海区 (63° - 69°1 2′S ,70°30′- 75°30′E) 3条断面 2 4个测站进行浮游生物现存量和初级生产力的现场观测 ,研究叶绿素a浓度和初级生产力的分布特征。测区表层叶绿素a浓度为 0 .1 6 - 3 .99μg/dm3,普里兹湾内和湾西部四女士浅滩海域浓度在 3 .5μg/dm3以上 ;平面分布趋势从湾内向西北方向递减 ,深海区浓度在 0 .5μg/dm3以下。从垂向看叶绿素a浓度的最大值大多出现于 2 5m或 50m层 ,50m以下更深层的浓度随深度的增加而降低 ,2 0 0m层叶绿素a浓度分布范围为 0 .0 1 - 0 .95μg/dm3。粒径分级叶绿素a浓度以微小型浮游生物的贡献占优势 (56 % ) ,微型浮游生物的贡献占2 4 % ,微微型浮游生物的贡献占 2 0 %。测区潜在初级生产力为 0 .1 1～ 1 1 .67mgC/(m3·h) ,平均值为 2 .0 0± 2 .80mgC/(m3·h)。高生产力区位于普里兹湾 ,平均现场生产力达到 0 .86gC/(m2 ·d) ;依次为陆架区、陆坡区 ,深海区生产力较低 ,平均现场生产力为 0 .1 7gC/(m2 ·d)。光合作用同化数较低 (1 .53± 1 .1 1mgC/(mgChla·h) )。粒径分级初级生产力以微小型浮游生物的贡献占优势 (58% ) ,微型浮游生物的贡献占 2 6 % ,微微型浮游生物的贡献占 1 6 %。浮游植     

南极拜尔斯半岛企鹅粪土沉积物元素地球化学特征

拜尔斯半岛位于南极利文斯顿岛最西部,是南设得兰群岛中最大的无冰区。对采自拜尔斯半岛的一根长55 cm的企鹅粪土沉积柱P1进行了元素和同位素地球化学分析。通过对沉积物C/N、有机质来源和δ15N的分析,发现P1沉积剖面中有机质主要来源于企鹅粪。利用富集系数、相关性分析、主成分分析等统计分析方法,识别出该沉积剖面中P、F、Cu、Hg、As、S六种元素具有共同的来源,与企鹅粪的输入密切相关,并且这些元素与TOC和δ15N显著正相关,说明沉积剖面中这些元素含量主要受控于企鹅粪的输入程度。通过与长城站区阿德雷岛、东南极戴维斯站加德纳岛企鹅粪土沉积物的标型元素特征比较,发现上述三个地区的标型元素组合大体上一致,反映了整个南极地区企鹅粪土沉积物生物标型元素组合的共性。研究结果为进一步恢复该地区的企鹅种群数量演化,及其对气候变化的响应提供了可能。     

南极普里兹湾及邻近南大洋水体N_2O分布特征

利用中国第25、26次南极科学考察航次获得南极普里兹湾及邻近南大洋附近水样,采用顶空气相色谱法分析其中N_2O含量,结果表明普里兹湾陆架水体N_2O浓度较低,介于13.2―17.4 nmol·L~(-1),且呈现不饱和状态,饱和度异常值为-7%;而普里兹湾附近南大洋水体中N_2O浓度较高,介于15.5―23.3 nmol·L-1,除表面一层极薄的不饱和层外,中层至底层水体相对工业革命前大气浓度为高度过饱和状态。该区域N_2O的分布格局与复杂的水团特性和水文过程有密切关系。N_2O含量不饱和的普里兹湾陆架水(SW)和绕极深层流(CDW)混合下沉形成南极底层水(AABW),可能为温室气体N_2O提供向深层海洋输运的通路。这个过程为大气N_2O提供了一个汇的机制,使南极近岸水体成为大气N_2O的汇区。     

1999/2000年夏季环南极表层海水叶绿素a和初级生产力

中国第 1 6次南极考察期间 ,作者随雪龙船于 1 999年 1 1月 2 2日至 2 0 0 0年 1月 1 8日从澳洲西南部到达东南极普里兹湾 ,后经南印度洋 -南大西洋 -德雷克海峡 -南大西洋 -南印度洋返回普里兹湾。航渡中定时采集表层海水 ,进行水温、盐度、营养盐、浮游生物现存量和光合作用速率的现场观测 ,研究环绕南极海域表层水叶绿素 a和初级生产力的分布特征。结果表明 ,南大洋表层水营养物质、浮游生物现存量和初级生产力分布具明显的区域性特征 ,南极辐合带以南的南极水营养盐浓度高于亚南极水和亚热带水。叶绿素 a浓度与营养物质的分布趋势一致 ,南极水、亚南极水和亚热带水的平均叶绿素 a浓度分别为 1 .77、1 .40和 0 .2 1 μg/dm3。在环绕南极的大洋中 ,南大西洋海域营养物质丰富 ,海水最为肥沃 ,叶绿素 a浓度和初级生产力高于南印度洋和德雷克海峡。在短期往返东南极 -西南极 -东南极的航渡观测中 ,由于南极夏季水温的升高 ,陆缘冰融化 ,冰藻释放 ,长城湾至普里兹湾的西 -东向航渡中观测的初级生产力、浮游植物细胞丰度、叶绿素 a浓度和光合作用同化数分别比普里兹湾至长城湾的东 -西向航渡中高 1 45%、1 1 3%、68%和 1 8%。与 1 0年前的观测结果比较 ,南大西洋仍为高生物量和高生产力海区 ;1 999/2 0 0 0     

热带与南极海域表层海水N2O饱和度异常差异性比较

本文比较了从北纬30?西太平洋至南纬30?东印度洋等热带海域与南大洋至东南极普里兹湾等南极海域的大气和表层海水N2O分压分布特征,表层海水pNO2饱和异常,分析引起异常差异性的主要影响因子。南极海域普里兹湾表层水中N2O分压（pN2O）平均为311.9 ± 7.6 nL/L (14.1 ± 0.4 nM),与大气中N2O混合比（318.5 nL/L）相比显略不饱和,融冰水的输入是导致不饱和的主要原因。海气N2O通量为-0.3 ± 0.8μmol m-2 d-1。而热带海域多数表层海水中N2O饱和度异常值都高于10%,在赤道海域发现最高值达54.7%,次高值为10°N的苏禄海为31%,计算出在赤道和苏禄海的海气通量分别为~12.4 μmol m-2 d-1和~4μmol m-2 d-1。表明高纬度的普里兹湾既不是大气中N2O源也不是汇,而低纬度热带海域表现为大气中N2O的源。造成热带与南极海域海洋N2O饱和度异常的影响因素,可能低纬度的热带海域由于海气间的气体交换较弱、上升流影响强,而高纬度的南极海域由于融冰分层和强偏西风影响;而海表面风速是影响N2O的海气交换N2O通量的重要因素。     

南极菲尔德斯半岛多环境介质中多环芳烃分布特征及环境行为研究

对南极菲尔德斯半岛地区采集的水体、土壤、苔藓、粪便和生物介质中16种多环芳烃(PAHs)进行了分析,考察了不同环境介质中PAHs的含量分布特征及其环境行为。结果表明,水体、土壤、苔藓、粪便和生物中∑PAHs浓度分别为34.9—346 ng·g-1(mean=184)、68.9—374 ng·g-1(mean=188)、122—894 ng·g-1(mean=251)、197—293 ng·g-1(mean=245)和137—443 ng·g-1(mean=265)。与其他地区相比,5种介质中2+3环PAHs的比例超过0.5,而5+6环PAHs的比例则0.2,说明大气传输是菲尔德斯半岛地区PAHs来源的主要途径。通过PAHs在土壤-苔藓(logQSM)、生物-海水(logQOW)和企鹅肌肉-企鹅粪土(logQPD)中的浓度比值与其理化参数的研究发现,logQSM与logpoL和logKOA成显著线性关系,logQOW和logQPD与logKOW成显著线性关系,表明不同环境介质间污染物浓度比值可以看作PAHs在极地偏远地区气-固分配行为以及在生物体内分配行为的镜像。     

量子共振检测仪在南极医学研究中的应用初探

本研究应用量子共振检测仪 (QRS)一种基于量子分析技术的灵敏能量分析器 ,测定了 1 0名南极考察队员的生理和心理改变。在出发前 (BD)、南极居留 6月时 (AR)和居留一年返回后次日 (RE)分别采取头发进行磁场分析。测定生理和心理指标 :三碘甲状腺胺酸 (T3)、四碘甲状腺胺酸 (T4)、促甲状腺激素 (TSH)、抑郁、孤独、不容忍、压力 ,评分以正负数值表示。结果表明 ,AR和RE各项指标的量化值与BD基础值相比都明显下降 (p <0 .0 1 )。例如 ,抑郁 (平均值±标准误 , X±S X)为 :1 .1 0± 0 .80 (BD) ,- 8.3± 0 .30 (AR) ,- 7.7± 0 .36(RE) ;TSH为 :- 2 .2± 0 .92 (BD) , 9.4± 0 .45(AR) ,- 8.4± 0 .40 (RE)。QRS量化值的负向改变反映了功能的异常 ,这一初步结果证实了文献报道的在南极长期居留可引起甲状腺活动改变和心境失调。     

1999年7月白令海海盆营养盐和溶解氧的垂直特征

1999年 7月下旬 ,雪龙号科学考察船在中国首次北极科学考察航次中在白令海海盆北部与中部完成了 2 2个深水站的采样作业。营养盐和溶解氧采样分 1 2层 ,共获得 2 71个样品。分析结果表明 :硅酸盐浓度 [Si]、磷酸盐浓度 [P]和无机氮浓度 [N](硝酸盐 [NO3- ]加亚硝酸盐[NO2 - ]加氨 [NH4 + ],主要成分为 [NO3 - ])垂直结构的相似之处在于 :在≤ 2 5m是第一层 ;随后为一个明显的跃层 ;第二层位于 5 0— 2 0 0m之间 ;然后有一个宽的跃层 ;从 5 0 0m至底部 (约3 90 0m)为第三层。其差别在于 :在第三层中 ,[Si]继续缓慢增加 ,而 [N]和 [P]略有减少。溶解氧[O2 ]与 [Si]、[P]、[N]的垂直分布表明在潜温 (θ)极小层以上 (0 .5— 2 .7°C ,盐度 3 3 .0 1— 3 3 .1 7,深度 81— 1 5 7m)的海水是海气充分交换层与生物主要活动层。在≥ 1 5 0m以下 ,[P]、[NO3 - ]两者和 [O2 ]有 >0 .9的正相关性。从表层至底部 ,在整个盐度范围内 ,[NO]∶[PO](其中 [NO]=9[NO3 - ]+[O2 ],[PO]=1 3 5 [P]+[O2 ])在 0 .786 - 1 .0 2 9之间大致均匀分布 ;这表明白令海海盆北部与中部海水的营养特性具有较强的保守性。     

亚暴等待时间的统计学分析:IMAGE卫星观测

利用IMAGE卫星FUV极光图像数据,对北半球极光椭圆带2760个亚暴事件进行统计分析,得到亚暴等待时间的统计分布,并利用简单的数学模型对卫星轨道的影响进行了讨论,得到以下结论:(1)亚暴等待时间在2-3h附近有一个峰值,较低纬度( MLat＜ 65°)发生的亚暴事件,其等待时间略长于较高纬度(MLat≥65°)发生的...     

A comprehensive model current system for high-latitude magnetic activity -II. The substorm component

Summary. In paper I of this series (Hughes & Rostoker) we have presented a composite model three-dimensional current system whose magnetic perturbation pattern is in good agreement with that observed at high latitudes during periods of moderate magnetospheric activity. In this paper we extend the model current system to demonstrate its ability to reproduce the magnetic perturbation pattern associated with the magnetospheric substorms. In agreement with previous workers, we find it necessary to include a region of intense equatorward current flow at the western edge of the westward travelling surge. For the particular substorm event presented in this paper, we find that the main eastward and westward electrojets intensified slightly before the appearance of the surge form, and we are able to evaluate quantitatively the amount of change involved.     

A study of two polar magnetic substorms with a two-dimensional magnetometer array

Summary. The paper reports studies of the three-dimensional magnetospheric—ionospheric current systems which produced polar magnetic substorms on 1974 September 7 and September 18. The data were magnetic perturbation fields observed with a two-dimensional array of 23 three-component magnetometers located in western Canada beneath the auroral oval. In an earlier study of a substorm of September 11 (Bannister & Gough) the fields fitted calculated field for a Boström Type 1 current loop with field-aligned currents at east and west ends of the ionospheric segment, and with uniform current density across the width. The substorms here reported could not be modelled with uniform current density. An inverse method due to Oldenburg was therefore used to estimate current density distributions, and satisfactory fits of calculated to observed field resulted. Each substorm was modelled at six representative epochs. In general the principal ionospheric current seem by the array was westward. At four epochs of the September 7 substorm and throughout the September 18 substorm, significant eastward ionospheric current (or its equivalent in terms of the fields produced) was observed north of the westward electrojet. Northwestward bends in the ionospheric current segments were found at four epochs on September 7 and at three epochs on September 18. As in the September 11 substorm (Paper 1), these bends were either west of or close to magnetic midnight. In some cases the bends may follow the auroral oval, but in others they are sharper and may be associated with the Harang discontinuity. East of geomagnetic the ionospheric currents tend to run in a constant geomagnetic midnight latitude range. The developments of the three substorms, of September 7, 11 (Paper 1) and 18, are compared. They showed a variety of shifts in longitude, though all moved eastward relative to magnetic midnight.     

南北半球亚极光区极化流分布特征的统计学研究

利用DMSP卫星粒子数据,对南北半球20 000多个亚极光区极化流(SAPS)事件进行统计学分析,重点研究SAPS的发生率及其发生位置隧季节和世界时的分布,研究表明:(1)SAPS的发生率有明显的季节和世界时依赖性,主要发生在春秋季节,显示出较强的地磁活动依赖性;(2)SAPS在冬至也较多发生,可能与亚暴过程有关;(3...     

Development of a polar magnetic substorm: a two-dimensional magnetometer array study

A polar magnetic substorm on 1974 September 11 was recorded by a two-dimensional array of 25 three-component magnetometers, so located that the westward ionospheric current passed over the array. The mean perturbation fields over five-minute intervals are presented at six representative epochs of the substorm, the first just before its onset and the sixth 21/2 hr later in the coda of the event. At four of the resulting 'time frames', the perturbation fields have been fitted, on a least-squares criterion, by calculated fields of three-dimensional current loops having downward field-aligned current at the east end of the ionospheric westward current, upward field-aligned current at the west end and closure in the magnetotail. The current density was constant across the width of each of these model currents. In three of the four time frames it proved necessary to introduce a bend to the northwest in the ionospheric current; this bend occurred within 27° (geomagnetic) west of geomagnetic midnight. An association with the Harang discontinuity is possible. The field-aligned current nearer to the array (in one time-frame the downward, east-end current, in two others the upward current at the west end) proved essential to secure any reasonable fit to the data. The ionospheric segment of the current loop moved at least 20° of longitude eastward, relative to the surface of the earth, between 07.48 and 08.58 UT. In this 70-min period the ionospheric segment moved at least 38° eastward relative to magnetic midnight.     

南极中山站极光亚暴期间的I(557.7nm)/I(427.8nm)比值变化分析

对1999年4月8日南极中山站极光亚暴期间不同谱线的极光强度比值进行讨论,并据此讨论亚暴期间沉降粒子能量随时间变化的情况.得出I(557.7 nm)/I(427.8 nm)和I(630.0 nm)/I(427.8 nm)比值在平静时期分别在5-22和1-2.76之间变化,该变化不是由原子氧浓度空间分布变化所引起,而可能...     

极光全天空图象移动速度的一种计算方法

用随机变形图案分析法计算极光全天空图象的移动速度。与过去直观估计方法不同的是,这样得到的是极光的整体移动速度或整个极光图象的平均速度,而不是个别部分（如最亮部分、边缘或某条亮射线等）的速度。对１９９７年６月２３日一段持续１００秒的平静带状极光记录进行了具体分析,得到极光东西向移动的最大速度为２．８ｋｍ ／ｓ。     

An investigation of the causes of abnormal quiet days in Sq (H)

Summary. From a study of 'abnormal quiet days' (AQDs) along the 0° meridian between 14 and 60° N, it was found (Butcher & Brown) that the minimum in H at stations on the poleward side of the Sq ( H ) focus was formed by a small negative substorm event when the normal Sq ( H ) amplitude was reduced by a superposed northward field.
In this paper we consider both the AQD event and the superposed northward field as a function of longitude and also consider in more detail the latitude variation of the superposed northward field. From such a study it is concluded that: (1) the AQD event is definitely due to a small magnetospheric substorm event; (2) the superposed northward field varies smoothly with longitude falling to zero some 110° from the longitude of its maximum amplitude; (3) the superposed northward field has a variation with geomagnetic latitude tending to zero near 20° and 70°N with a maximum near 55° N in summer and 35° N in winter; (4) there is some evidence that the effect of the IMF penetrates into the mid-latitude E-region and its effect is latitude-dependent. Although the evidence supports the suggestion that the currents responsible for the superposed northward field flow in the E-region no suggestion as to the origin of the driving force of the currents is forthcoming.     

Magnetometer array study in a tectonically active region of Quebec, Canada

Summary. An array of 26 magnetometers deployed in a tectonically active area of Quebec has mapped a boundary in terrestrial electrical conductivity for 200 km along strike. The contrast in conductivity across the boundary, from previous magnetotelluric soundings, is about one order of magnitude. Anomalous variation fields associated with electric currents flowing along the boundary are readily detected at pulsation periods only when the horizontal field is polarized transverse to the structure (the E -polarization case). The anomaly is hardly visible in transfer functions from substorms, for a number of reasons: a predominant H -polarization orientation of the substorm fields, the single order-of-magnitude contrast in conductivity, and the probably small depth extent of the structure. Attempts were made to estimate the response of a one-dimensional earth via the inductive scale length with gradients evaluated from polynomial surfaces fitted to the smoothly varying substorm fields. The results were inconsistent, owing to vertical fields with strong external components and to horizontal fields with scale lengths too small relative to their penetration distances.     

塔里木盆地绿洲农田土壤水盐运动动力学模式研究

本文采用改进型Ｐｉｃａｒｄ迭代差分法求解土壤水分运动的混鸽ｉｃｈａｒｄｓ方程,避免了采用Ｐｉｃａｒｄ迭代求解ｈ型Ｒｉｃｈａｒｄｓ方程所现的质量平衡误差问题。