云凝结物平流输送对降水云系发展影响的数值模拟研究

大气动力学中"平流输送"是非常重要的宏观动力学过程,云凝结物的平流输送与降水云系的发展演变密切相关,它把宏观动力过程与各种云凝结物粒子的时空演变联系起来,云凝结物的平流输送可以增加或减少局地大气中云凝结物的含量,改变云凝结物的空间分布状况,影响云凝结物的微观物理过程,进而促进或抑制降水云系的发展演变.本文在数值模拟研究中.通过改变云凝结物平流输送的状况来研究宏观动力过程对云微观物理过程的影响,因而利用ARPS模式开展3个分别排除云凝结物水平平流输送、垂直平流输送和三维平流输送的敏感试验,进行关于云凝结物平流输送对降水云系发展演变影响的敏感性数值模拟研究.结果表明,云凝结物的平流输送对水汽比湿的影响很小.云凝结物的三维平流输送有利于增加降水云系中雪和霰的混合比含量,抑制云水、雨水和云冰混合比含量的增长.云凝结物的水平平流输送可以降低降水云系中云水和雨水的混合比含量,增加云冰和雪的混合比含量;云凝结物垂直平流输送的作用是增加降水云系中雨水、雪和霰的混合比含量,减少云与冰混合比含量.云凝结物三维平流输送效应的分析表明,云凝结物的三维平流输送主要通过调整云凝结物的微物理过程源汇项以及降水粒子(雨水、雪和霰)的下落末速项来改变降水云系中云凝结物的垂直结构;另外,雪的三维平流输送对雪本身的分布也有一定影响.     

1998年夏季风爆发前后南海地区的水汽输送和水汽收支

利用NCEP逐日再分析资料、Micaps系统提供的气象观测资料及局地经向环流线性诊断模式，定量分析了2003年夏季东亚地区局地经向环流的演变情况。结果表明：(1)东亚地区夏季雨带的移动与局地经向环流的演变紧密联系。当淮河流域发生强降水时，在淮河流域上升和华南地区下沉的副热带季风环流圈尤为显著，该环流圈主要由潜热加热、热量垂直输送、温度平流和西风动量经向输送等物理因子所驱动；(2)潜热加热主要影响副热带季风环流上升支的强度，反映了梅雨锋对流系统的重要作用；(3)热量垂直输送、温度平流及西风动量经向输送则主要影响副热带季风环流上升支的北移，其中热量垂直输送、与强(弱)斜压槽活动有关的经向温度平流和涡动西风动量经向输送(纬向温度平流和平均西风动量经向输送)对上升支北移的作用在华南地区汛期后期(在其余夏季降水阶段)较突出。以上这些物理因子具有预报东亚地区局地经向环流演变和雨带移动的参考价值。     

全球海洋环流模式中氚分布的模拟

氚（3H）作为一种重要的被动示踪物,经常被用于研究海洋中的物理过程及评估海洋环流模式的模拟性能。使用一个全球海洋环流模式（LICOM）来研究氚在海洋中的分布、存储和输送。模拟的全球氚通量表明,1975年之前氚主要由海气交换输入海洋,特别是在1963年,氚的气体交换输入约为降水输入的2.5倍,1975年之后两种方式的氚输入通量都大幅减少。比对GEOSECS（Geochemical Ocean Sections Study,1972～1978年）和WOCE （World Ocean Circulation Experiment,1989～1995年）大洋观测计划期间的观测资料发现,我们的模式很好地模拟出了氚的海表分布、水柱总量、经向分布以及次表层的高值信号,主要缺点在于模拟的氚向深层的穿透不足,特别是在全球的两个副热带地区,表现尤为明显,氚输入函数的不确定性和模式物理场描述的不足可能是造成误差的主要原因。模式给出的海洋中氚储存总量的结果与基于观测得到的结果比较吻合,如北太平洋海区：1973～1974年模拟结果约为20.4 kg,相同期间观测估计值为21.1±4.7 kg,1989～1995年模拟结果为20.7 kg,相同期间观测估计值为23.4±2.0 kg。氚在等密度面上高低纬的侧向通风明显,模式成功模拟出氚从中高纬的海表进入,沿等密度面向低纬的次表层输送,又经大洋环流和扩散分别向南半球和高纬输送的过程。     

二维平流辐射雾的数值模拟

本文采用二维非定常数值模式,模拟了大气边界层内辐射雾、平流辐射雾和在海陆交界处的平流辐射雾的形成、演变规律。研究了雾发展过程中湍流-辐射作用及风场、水汽平流和海陆风环流对雾发展影响的特点。模拟计算结果得出湍流-辐射作用是雾发展变化的主要物理因子。大气边界层风场及风场环流和水汽的平流输送对在不同地点,时刻雾的发展和强度变化也有重要的影响。     

一次强沙尘暴和雪暴天气过程的诊断及模拟分析

利用基本气象资料和T213数值预报产品资料,对发生在内蒙古大部分地区的一次强风、强沙尘暴、强雪暴和强降温天气过程进行了动力诊断和模拟分析。结果表明,强冷空气活动是造成多种灾害的主要动力,高空急流是强风的动量来源,蒙古气旋强烈发展造成的气压梯度风加剧了地面大风和沙尘暴。强烈的冷、暖平流空间配置使大风、沙尘暴和降温更为剧烈。散度场的空间配置有利于沙尘暴、暴风雪的发展。高空西风急流对低空西南急流具有耦合和触发作用,低空西南急流的建立和长距离的水汽输送与辐合,成为内蒙古东部产生暴雪的重要条件,低层东风切变带中的正涡度平流的输送,叠加到了较好的水汽输送及辐合区域,加大了降雪。后期低层西北急流的形成,是产生暴风雪的重要原因。数值模拟结果表明,模拟高压、低压中心位置和强度与实况较为吻合,气旋的气压梯度强度与实况较为接近;冷暖平流在分布区域、输送方向、强中心位置上也与实况具有较相似的特征,但是温度平流模拟的结果在量值上略大于实况。     

闪电产生氮氧化物(LNOX)及其输送过程的模式计算

利用三维强风暴动力电耦合模式,模拟分析了一次雷暴过程中放电活动特征及平流和湍流对LNOX的输送特征。结果表明,在中部负电荷区域的上边缘,对应上升气流区外围、水平流场中心部位的区域,因为放电传输距离较长,所以强放电区主要落在这些部位,且向上传输。在负电荷中心区也有少数放电点,但传输距离较短。闪电产生的氮氧化物逸出闪道后,被云中平流和湍流输送,最后在弱流场区域内形成LNOX浓度中心,峰值达9×10-9。LNOX的输送主要以平流为主,但在云底层及雷暴消散阶段,湍流输送也起重要作用。在雷暴云消亡期,LNOX的峰值为2.7×10-9,比晴天值大1个量级。     

热带太平洋-印度洋海温异常综合模的数值模拟

通过数值模拟及结果的合成分析,对热带太平洋-印度洋异常海温综合模态的三维热力结构、动力结构及其发生发展的可能机制进行了研究.数值模拟结果的分析表明,太平洋、印度洋海温异常的综合模态在表层、次表层的表现都很明显,即在赤道西印度洋、中东太平洋的海温偏高(低)时,赤道西太平洋、东印度洋的海温偏低(高),该模态还存在着显著的年变化特征、年际变化特征以及年代际变化特征.数值模拟的合成分析结果表明,异常的海表风应力引起表层洋流异常,表层洋流异常及由其引起的海表高度异常可导致次表层海水环流的异常,海洋环流异常导致的平流热输送异常是海温形成异常综合模态的主要原因之一,垂直输送是形成次表层海温综合模态的主要原因.平流热输送过程对海表温度变异的贡献是:在事件发生到盛期阶段促进了次表层海温异常综合模态的形成,在盛期到消亡阶段次表层的平流过程阻碍其进一步发展;短波辐射是海洋的主要热力来源,海表面异常的净短波辐射通量、潜热通量是表层海温形成异常模态的主要热力学原因,异常的海表面净短波辐射通量、潜热通量、感热通量在到达盛期阶段后抑制其进一步发展.     

数值剖析0411号热带气旋位置不连续变化和强度突变

为探究竟0411号热带气旋(TC0411)出现数小时内向北"走"了300多公里且急剧加强的异常现象,根据TC0411经向环流特征(辐合抬升ω<0的水汽多来自偏南风v>0)及其与第2类条件不稳定(CISK)机制的密切关系,运用反映南海经向环流的线性诊断模式(包含边界效应、各稳定度及17个内力因子),对TC0411进行定量诊断。结果表明:南海东北部深厚强盛的偏南风急流及其造成的弱惯性稳定度为TC0411发生发展(向北不连续位移)提供了有利水汽输送和抬升(驱动)条件。其中,对偏南风有突出正贡献的边界效应与5°N西南夏季风和西太平洋东南风的辐合有关;驱动地转南风的气压梯度力与中南半岛季风槽、西太平洋高压和高层东风扰动有关。驱动非地转南风的内力因子主要是与斜压不稳定有关的平均经向温度平流、与西南风急流切变场有关的涡动西风动量经向输送、与夏季风环流和高层东风扰动相互作用有关的平均西风动量纬向输送及与非对称动力热力场有关的涡动温度平流。TC0411向北不连续位移实质为22.7°N附近生成新热带低压(TD)和19°N附近TD消亡的结果。2004年7月26日20时—27日02时激发22.7°N附近上升运动(19°N附近下沉运动)的主要因子是平均经向温度平流和涡动西风动量水平输送(平均西风动量纬向输送和涡动温度平流)。27日02—14时使新TD加强为热带风暴(TS)并维持的主要因子是潜热加热和平均经向温度平流。根据以上分析,建议业务预报应着眼于深厚强盛西南风急流和温度平流的共同作用。     

2009年河南一次大暴雨过程的涡度方程诊断分析

利用NCEP/NCAR再分析格点资料、常规气象资料及中尺度WRF模式,对2009年8月28-30日发生在河南南部的一次暴雨过程进行中尺度数值模拟及诊断分析。结果表明,WRF模式对此次暴雨过程模拟效果较好,模拟物理量能够较好地反映暴雨的实际特征,模拟暴雨强度及落区与实况较一致。高空槽、副热带高压、超低空东风急流及低层风切变是此次暴雨的主要影响系统。利用涡度方程对暴雨过程进行诊断分析发现,涡度方程各项收支中,涡度平流作用与辐合辐散作用对涡度局地变化的贡献最大,垂直输送项与扭转项对涡度局地变化的贡献较弱。涡度平流项对中低层涡度局地变化表现出正反馈作用,垂直输送项、扭转项及辐合辐散项起着负反馈作用。涡度平流作用使得中低层气旋式环流加强,有利于中低层辐合加强,局地涡度增加。垂直输送项、扭转项及辐合辐散项使得低层辐合减弱,气旋性涡度减小。此外,利用垂直螺旋度等模拟产品对暴雨诊断分析发现,暴雨落区与垂直螺旋度大值中心、水汽通量散度负值中心等相对应,此次暴雨正是在良好的动力、水汽及热力条件下产生的。     

2009年河南一次大暴雨过程的涡度方程诊断分析

利用NCEP／NCAR再分析格点资料、常规气象资料及中尺度WRF模式,对2009年8月28—30日发生在河南南部的一次暴雨过程进行中尺度数值模拟及诊断分析。结果表明,WRF模式对此次暴雨过程模拟效果较好,模拟物理量能够较好地反映暴雨的实际特征,模拟暴雨强度及落区与实况较一致。高空槽、副热带高压、超低空东风急流及低层风切变是此次暴雨的主要影响系统。利用涡度方程对暴雨过程进行诊断分析发现,涡度方程各项收支中,涡度平流作用与辐合辐散作用对涡度局地变化的贡献最大,垂直输送项与扭转项对涡度局地变化的贡献较弱。涡度平流项对中低层涡度局地变化表现出正反馈作用,垂直输送项、扭转项及辐合辐散项起着负反馈作用。涡度平流作用使得中低层气旋武环流加强,有利于中低层辐合加强,局地涡度增加。垂直输送项、扭转项及辐合辐散项使得低层辐合减弱,气旋性涡度减小。此外,利用垂直螺旋度等模拟产品对暴雨诊断分析发现,暴雨落区与垂直螺旋度大值中心、水汽通量散度负值中心等相对应,此次暴雨正是在良好的动力、水汽及热力条件下产生的。     

Influences of Climate Change on the Uptake and Storage of Anthropogenic CO2 in the Global Ocean

A global ocean general circulation model, called LASG/IAP Climate system ocean model (LICOM), is employed to study the influence of climate change on the uptake and storage of anthropogenic CO 2 in the global ocean. Two simulations were made: the control run (RUN1) with the climatological daily mean forcing data, and the climate change run (RUN2) with the interannually varying daily mean forcing data from the NCEP (National Centers for Environmental Prediction) of the US. The results show that the simulated distributions and storages of anthropogenic dissolved inorganic carbon (anDIC) from both runs are consistent with the data-based results. Compared with the data-based results, the simulations generate higher anDIC concentrations in the upper layer and lower storage amount of anDIC between the subsurface and 1000-m depth, especially in RUN1. A comparison of the two runs shows that the interannually varying forcing can enhance the transport of main water masses, so the rate of interior transport of anDIC is increased. The higher transfer rate of anDIC in RUN2 decreases its high concentration in the upper layer and increases its storage amount below the subsurface, which leads to closer distributions of anDIC in RUN2 to the data-based results than in RUN1. The higher transfer rate in RUN2 also induces larger exchange flux than in RUN1. It is estimated that the global oceanic anthropogenic CO 2 uptake was 1.83 and 2.16 Pg C yr 1 in the two runs in 1995, respectively, and as of 1994, the global ocean contained 99 Pg C in RUN1 and 107 Pg C in RUN2 of anDIC, indicating that the model under the interannually varying forcing could take up 8.1% more anthropogenic carbon than the model under the climatological forcing. These values are within the range of other estimates based on observation and model simulation, while the estimates in RUN1 are near the low bound of other works. It is estimated that the variability of root mean square of the global air-sea anthropogenic carbon flux from the simulated monthly mean results of RUN2 with its seasonal cycle and long-term trend removed is 0.1 Pg C yr 1 . The most distinct anomalies appear to be in the tropical Pacific Ocean and the Southern Ocean.     

Interannual and interdecadal variabilities in the Pacific in an MRI coupled GCM

Interannual and interdecadal variabilities in the Pacific are investigated with a coupled atmosphere-ocean GCM developed at MRI, Japan. The model is run for 70 years with flux adjustments. The model shows interannual variability in the tropical Pacific which has several typical characteristics shared with the observed ENSO. A basin-scale feature of the principal SST variation for the ENSO time scale shows negative correlation in the central North Pacific with the tropical SST, similar to that of the observed one. Associated variation of the model atmosphere indicates an intensification of the Aleutian Low and a PNA-like teleconnection pattern as a response to the tropical warm SST anomaly. The ENSO time scale variability in the midlatitude ocean consists of the westward propagation of the subsurface temperature signal and the temperature variation within the shallow mixed layer forced by the anomalous atmospheric heat fluxes. For the interdecadal time scale, variation of the SST is simulated realistically with a geographical pattern similar to that for the ENSO time scale, but it has a larger relative amplitude in the northern Pacific. For the atmosphere, spatial structure of the variation in the interdecadal time scale is also similar to that in the ENSO time scale, but has smaller amplitude in the northern Pacific. Long oceanic spin-up time (>∼10 y) in the mid-high latitude, however, makes oceanic response in the interdecadal time scale larger than that in the ENSO time scale. The lagged-regression analysis for the ocean temperature variation relative to the wind stress variation indicates that interdecadal variation of the ocean subsurface at the mid-high latitudes is considered as enhanced ocean gyre spin-up process in response to the atmospheric circulation change at the mid-high latitudes, remotely forced by the interdecadal variation of the tropical SST. Received: 6 November 1995 / Accepted: 19 April 1996     

The Asymmetry of Subsurface Temperature Anomalies Associated with ENSO in the Equatorial Western Pacific

The phenomenon of ENSO asymmetry has been recognized for many years, but most studies have focused on the asymmetry of surface temperature anomalies in the equatorial eastern Pacific. Here, the authors investigate the temperature asymmetry associated with ENSO in the subsurface of the western Pacific through analysis of observations and numerical experiments with an ocean GCM. Both the observation and simulation exhibit significant ENSO asymmetry, characterized by negative temperature skewness in the equatorial western Pacific and positive skewness in the eastern Pacific. Heat budget analysis reveals that nonlinear dynamical heating results in the positive temperature asymmetry in the equatorial eastern Pacific, but tends to weaken the negative temperature asymmetry in the equatorial western Pacific. The climatological meridional current transports the temperature anomalies and corresponding negative asymmetry from the off-equator region to the equator in the subsurface of the western Pacific. Through a sensitivity experiment with reversed wind stress forcing, the authors suggest that the skewness of the wind stress anomalies does not contribute to the negative temperature asymmetry in the western Pacific in the first-order approximation, while the internal nonlinear dynamics does play a key role. The study suggests that, as a result of nonlinear processes, the oceanic responses to anomalous wind stress are nonlinear and asymmetric in the tropical Pacific.     

CMIP5模式对拉尼娜生命史模拟能力的评估

利用19个CMIP5模式输出资料,评估模式对于拉尼娜事件特殊生命史发展过程的模拟能力。评估结果显示,仅有少数模式可以很好地再现拉尼娜事件缓慢衰减并再次增强的生命史发展过程,而多数模式中拉尼娜事件持续衰减直至消亡。观测分析结果表明,一个可能导致拉尼娜再次增强的原因是风场强迫作用下的海洋赤道波动过程。模拟能力较好的模式可以建立起"SST—对流—风场"正反馈过程,使得拉尼娜事件再次发展。而模拟能力较弱的模式中正反馈过程无法建立,因此拉尼娜事件最终消亡。另一个可能导致拉尼娜事件再次增强的原因是海洋平均经圈环流的作用。模拟能力较好的模式可以很好地模拟出气候态海洋经圈环流强度,因此海洋平均经向冷平流会帮助赤道地区负海温距平再次增强。而模拟能力较弱的模式中海洋经圈环流强度较弱,因此赤道地区负海温距平持续衰减,最终回归到气候态。     

Response of Southern Ocean circulation to global warming may enhance basal ice shelf melting around Antarctica

We investigate the large-scale oceanic features determining the future ice shelf–ocean interaction by analyzing global warming experiments in a coarse resolution climate model with a comprehensive ocean component. Heat and freshwater fluxes from basal ice shelf melting (ISM) are parameterized following Beckmann and Goosse [Ocean Model 5(2):157–170, 2003]. Melting sensitivities to the oceanic temperature outside of the ice shelf cavities are varied from linear to quadratic (Holland et al. in J Clim 21, 2008). In 1% per year CO₂-increase experiments the total freshwater flux from ISM triples to 0.09 Sv in the linear case and more than quadruples to 0.15 Sv in the quadratic case after 140 years at which 4 × 280 ppm = 1,120 ppm was reached. Due to the long response time of subsurface temperature anomalies, ISM thereafter increases drastically, if CO₂ concentrations are kept constant at 1,120 ppm. Varying strength of the Antarctic circumpolar current (ACC) is crucial for ISM increase, because southward advection of heat dominates the warming along the Antarctic coast. On centennial timescales the ACC accelerates due to deep ocean warming north of the current, caused by mixing of heat along isopycnals in the Southern Ocean (SO) outcropping regions. In contrast to previous studies we find an initial weakening of the ACC during the first 150 years of warming. This purely baroclinic effect is due to a freshening in the SO which is consistent with present observations. Comparison with simulations with diagnosed ISM but without its influence on the ocean circulation reveal a number of ISM-related feedbacks, of which a negative ISM-feedback, due to the ISM-related local oceanic cooling, is the dominant one.     

Interannual Salinity Variability in the Tropical Pacific in CMIP5 Simulations

Salinity variability and its causes in the tropical Pacific are analyzed using observations, reanalysis products and model simulations. The mixed-layer salinity(MLS) budget analyses from observations and reanalysis products indicate that its interannual evolution is closely related to ENSO and is predominantly governed by surface forcing and surface advection in the western-central equatorial Pacific. It is found that the observed MLS tendency leads Nin?o3.4 by about 12 months due to the effect of negative freshwater flux(evaporation minus precipitation). These observation-based analyses are used to evaluate the corresponding simulation using GFDL-ESM2 M. It is evident that the model can simulate the spatiotemporal variations of MLS with some discrepancies compared to observations. In the warm pool of the equatorial Pacific the MLS tendency in the model is sensitive to ocean dynamics, however model biases cause the tendency to be underestimated. In particular, the freshwater flux is overestimated while the ocean surface zonal current and vertical velocity at the base of the mixed layer are underestimated. Due to model biases in representing the related physics, the effects of surface forcing on the simulated MLS budget are overestimated and those of subsurface and surface advection are relatively weak. Due to weaker surface advection and subsurface forcing than observed, the simulated compensations for surface forcing are suppressed, and the simulated MLS tendency that leads Nin?o3.4 by 8–10 months, which is shorter than the observed lead time. These results are useful for the interpretation of observational analyses and other model simulations in the tropical Pacific.     

大气环流模式降水的模拟对水汽方程差分方案的敏感性试验

分别采用3种应用比较广泛的水汽方程差分方案:多维正定平流传输方案(MPDATA)、通量修正传输方案(FCT)和两步保形平流方案(TSPAS),对大气物理所9层大气环流模式(IAP 9L AGCM)的降水模拟作敏感性试验,分析比较3种方案下模式降水气候平均场的差异,从而揭示模式降水对水汽方程差分方案的敏感性.试验结果显示,不同的水汽方程差分方案对大气环流模式降水的气候模拟有较大影响,并由此从3种差分方案中为IAP 9L AGCM寻找出一种较好的水汽计算方案.     

The role of atmospheric internal variability on the prediction skill of interannual North Pacific sea-surface temperatures

The sensitivity of the sea-surface temperature (SST) prediction skill to the atmospheric internal variability (weather noise) in the North Pacific (20^°–60^°N;120^°E–80^°W) on decadal timescales is examined using state-of-the-art Climate Forecasting System model version 2 (CFS) and a variation of CFS in an Interactive Ensemble approach (CFSIE), wherein six copies of atmospheric components with different perturbed initial states of CFS are coupled with the same ocean model by exchanging heat, momentum and fresh water fluxes dynamically at the air-sea interface throughout the model integrations. The CFSIE experiments are designed to reduce weather noise and using a few ten-year long forecasts this study shows that reduction in weather noise leads to lower SST forecast skill. To understand the pathways that cause the reduced SST prediction skill, two twenty-year long forecasts produced with CFS and CFSIE for 1980-2000 are analyzed for the ocean subsurface characteristics that influence SST due to the reduction in weather noise in the North Pacific. The heat budget analysis in the oceanic mixed layer across the North Pacific reveals that weather noise significantly impacts the heat transport in the oceanic mixed layer. In the CFSIE forecasts, the reduced weather noise leads to increased variations in heat content due to shallower mixed layer, diminished heat storage and enhanced horizontal heat advection. The enhancement of the heat advection spans from the active Kuroshio regions of the east coast of Japan to the west coast of continental United States and significantly diffuses the basin-wide SST anomaly (SSTA) contrasts and leads to reduction in the SST prediction skill in decadal forecasts.     

热带太平洋-印度洋海温联合模及其气候影响

本文基于观测资料和LICOM2.0模拟结果的分析研究,简要介绍讨论了太平洋—印度洋海温(异常)联合模(PIOAM)的存在、特征、演变及其影响等问题。热带太平洋—印度洋区域乃至全球范围的海表温度异常(SSTA)资料进行EOF分解,都清楚表明其第一分量在热带太平洋—印度洋的空间形态与太平洋—印度洋海温(异常)联合模(PIOAM)非常相似,说明PIOAM是热带太平洋—印度洋实实在在存在的一种海温异常模态。对应PIOAM的正、负位相,热带印度洋和西太平洋地区的夏季(JJA)850 hPa距平风场有近乎相反的异常流场形势;对流层低层的Walker环流支和亚洲夏季风都出现了不同特征的(近乎相反)异常;在PIOAM正(负)位相将使得100 hPa的南亚高压位置偏东(西)。对热带太平洋和印度洋温跃层曲面上的海温异常(为了方便将其称为SOTA)进行EOF分解,发现其第一模态也是一个三极子模态,即当赤道中西印度洋大部分海域与赤道中东太平洋大部分海域偏暖(偏冷)时,赤道东印度洋和赤道西太平洋大部分海域则偏冷(偏暖);它与太平洋—印度洋表层的PIOAM十分类似,也表明PIOAM在海洋次表层也是存在的。高分辨海洋环流模式LICOM2.0的模拟结果,无论是对太平洋—印度洋表层还是次表层的PIOAM的特征和演变都刻画得很好,这从另一个角度进一步说明PIOAM是热带太平洋—印度洋实际存在的一种海温变化模态。PIOAM正、负位相不仅对亚洲及西太平洋地区的天气气候有非常不一样的影响(不少地方有反向的特征),还会对南北美洲和非洲一些地区产生不同影响;而且其影响与单独的厄尔尼诺(El Ni?o)及印度洋偶极子(IOD)都不尽相同。