海洋科学
海洋科學
해양과학
MARINE SCIENCES
2013年
12期
52-61
,共10页
黑潮路径%条件非线性最优扰动(CNOP)%前期征兆%正压出入流模式
黑潮路徑%條件非線性最優擾動(CNOP)%前期徵兆%正壓齣入流模式
흑조로경%조건비선성최우우동(CNOP)%전기정조%정압출입류모식
the Kuroshio path%conditional nonlinear optimal perturbation (CNOP)%optimal precursor%barotropic in-flow-outflow model
基于正压出入流模式,利用条件非线性最优扰动(CNOP)方法研究初始异常的位置与模态对日本南部黑潮路径变异的影响。以模式模拟出的黑潮平直路径的平衡态作为参考态,计算CNOP,考察该扰动随时间的发展,并与随机扰动的发展进行对比。结果表明, CNOP能够导致黑潮弯曲路径发生,随机扰动则不能。因此, CNOP可以作为导致日本南部黑潮路径发生弯曲的一种最优前期征兆。通过分析CNOP和随机扰动的发展过程,可以得出:(1) CNOP使黑潮发展成弯曲路径的过程是一个气旋涡向下游传播并增长的过程。(2)气旋涡的向东传播都是非线性项的作用,也就是涡度平流造成的。(3) CNOP和随机扰动发展过程中所产生的气旋涡均会传播到下游区域,但是 CNOP 产生的气旋涡能够增强,最终导致弯曲路径发生,而随机扰动产生的气旋涡则会减弱,并不能导致弯曲路径发生。分析发现,在CNOP实验中,非线性作用使气旋涡增大;但在随机扰动实验中,非线性作用使气旋涡减弱,所以非线性作用对日本南部黑潮路径发生弯曲有重要影响。(4)底摩擦效应对日本南部黑潮路径变异影响较小。本文揭示的黑潮路径发生弯曲的最优前期征兆及其非线性发展机制,对提高黑潮路径变异的预报技巧具有重要意义。
基于正壓齣入流模式,利用條件非線性最優擾動(CNOP)方法研究初始異常的位置與模態對日本南部黑潮路徑變異的影響。以模式模擬齣的黑潮平直路徑的平衡態作為參攷態,計算CNOP,攷察該擾動隨時間的髮展,併與隨機擾動的髮展進行對比。結果錶明, CNOP能夠導緻黑潮彎麯路徑髮生,隨機擾動則不能。因此, CNOP可以作為導緻日本南部黑潮路徑髮生彎麯的一種最優前期徵兆。通過分析CNOP和隨機擾動的髮展過程,可以得齣:(1) CNOP使黑潮髮展成彎麯路徑的過程是一箇氣鏇渦嚮下遊傳播併增長的過程。(2)氣鏇渦的嚮東傳播都是非線性項的作用,也就是渦度平流造成的。(3) CNOP和隨機擾動髮展過程中所產生的氣鏇渦均會傳播到下遊區域,但是 CNOP 產生的氣鏇渦能夠增彊,最終導緻彎麯路徑髮生,而隨機擾動產生的氣鏇渦則會減弱,併不能導緻彎麯路徑髮生。分析髮現,在CNOP實驗中,非線性作用使氣鏇渦增大;但在隨機擾動實驗中,非線性作用使氣鏇渦減弱,所以非線性作用對日本南部黑潮路徑髮生彎麯有重要影響。(4)底摩抆效應對日本南部黑潮路徑變異影響較小。本文揭示的黑潮路徑髮生彎麯的最優前期徵兆及其非線性髮展機製,對提高黑潮路徑變異的預報技巧具有重要意義。
기우정압출입류모식,이용조건비선성최우우동(CNOP)방법연구초시이상적위치여모태대일본남부흑조로경변이적영향。이모식모의출적흑조평직로경적평형태작위삼고태,계산CNOP,고찰해우동수시간적발전,병여수궤우동적발전진행대비。결과표명, CNOP능구도치흑조만곡로경발생,수궤우동칙불능。인차, CNOP가이작위도치일본남부흑조로경발생만곡적일충최우전기정조。통과분석CNOP화수궤우동적발전과정,가이득출:(1) CNOP사흑조발전성만곡로경적과정시일개기선와향하유전파병증장적과정。(2)기선와적향동전파도시비선성항적작용,야취시와도평류조성적。(3) CNOP화수궤우동발전과정중소산생적기선와균회전파도하유구역,단시 CNOP 산생적기선와능구증강,최종도치만곡로경발생,이수궤우동산생적기선와칙회감약,병불능도치만곡로경발생。분석발현,재CNOP실험중,비선성작용사기선와증대;단재수궤우동실험중,비선성작용사기선와감약,소이비선성작용대일본남부흑조로경발생만곡유중요영향。(4)저마찰효응대일본남부흑조로경변이영향교소。본문게시적흑조로경발생만곡적최우전기정조급기비선성발전궤제,대제고흑조로경변이적예보기교구유중요의의。
The barotropic inflow-outflow model was built to study the impacts of spatial locations and patterns of the initial anomaly on the variability of the Kuroshio path using the conditional nonlinear optimal perturbation (CNOP) method. First, the CNOP was calculated using the equilibrium of the straight path as reference state. Then the CNOP was superimposed on the reference state to investigate its development process, which was compared with the evolutions of random perturbation (RP). We found that the CNOP caused the Kuroshio path to transfer to meander path while the random perturbation did not. In this case, the CNOP could be regarded as the optimal precursor of the Kuroshio meander path. By analyzing the developing processes of the CNOP and the RP, we concluded that: 1) The formation process of the Kuroshio meander path caused by CNOP was the process of a cyclonic eddy advection downstream. 2) The cyclonic eddy was transferred to downstream due to the effect of nonlinear items, which was also the vorticity advection term. 3) The eddies both in the CNOP and RP cases would transport to the downstream, but the eddy in the CNOP case could grow up and develop into meander path while the eddy in the RP case could not. The cyclonic eddy was strengthened by the nonlinear effect in the CNOP case, while it was weakened by the nonlinear effect in the RP case. In conclusion, the nonlinear effect was very important in the processes of the formation of the Kuroshio meander path in the south of Japan. 4) The impact of bottom friction has relatively small effeots on the variability of the Kuroshio path in the south of Japan. This study has revealed the optimal precursor of the occurrence of Kuroshio meander path and its nonlinear evolution mechanism, which is very important for improving the forecast skill of the Kuroshio path variations.