{"title":"动力","authors":"M. McCluskey","doi":"10.1201/9780429506437-8","DOIUrl":null,"url":null,"abstract":"A simple, but general, horizontal momentum budget for inviscid (cid:143) ow is developed to understand how the vertical (cid:143) ux of horizontal momentum varies with height in a mountain-forced trapped lee-wave train. Taking a sinusoidal form for the wave (cid:142) eld, from the analytical solution for a two-layer Scorer-parameter atmosphere, the constant Bernoulli functional on a streamline is used to diagnose the momentum (cid:143) ux. It is shown that in an inviscid, steady wave train the magnitude of the momentum (cid:143) ux decreases with height as a sinusoidal function. The present theory clearly shows how this pro(cid:142) le of momentum (cid:143) ux with height is a direct consequence of the exact balance between the vertical derivative of momentum (cid:143) ux and the dynamic pressure difference across the mountain in steady state. The simple analytic pro(cid:142) le of (cid:143) ux with height shows a remarkable qualitative similarity with numerical-model results from idealized case-studies of (cid:143) ow over an isolated mountain ridge.","PeriodicalId":415009,"journal":{"name":"No-Frills Physics","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Momentum\",\"authors\":\"M. McCluskey\",\"doi\":\"10.1201/9780429506437-8\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A simple, but general, horizontal momentum budget for inviscid (cid:143) ow is developed to understand how the vertical (cid:143) ux of horizontal momentum varies with height in a mountain-forced trapped lee-wave train. Taking a sinusoidal form for the wave (cid:142) eld, from the analytical solution for a two-layer Scorer-parameter atmosphere, the constant Bernoulli functional on a streamline is used to diagnose the momentum (cid:143) ux. It is shown that in an inviscid, steady wave train the magnitude of the momentum (cid:143) ux decreases with height as a sinusoidal function. The present theory clearly shows how this pro(cid:142) le of momentum (cid:143) ux with height is a direct consequence of the exact balance between the vertical derivative of momentum (cid:143) ux and the dynamic pressure difference across the mountain in steady state. The simple analytic pro(cid:142) le of (cid:143) ux with height shows a remarkable qualitative similarity with numerical-model results from idealized case-studies of (cid:143) ow over an isolated mountain ridge.\",\"PeriodicalId\":415009,\"journal\":{\"name\":\"No-Frills Physics\",\"volume\":\"1 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-05-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"No-Frills Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1201/9780429506437-8\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"No-Frills Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1201/9780429506437-8","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
A simple, but general, horizontal momentum budget for inviscid (cid:143) ow is developed to understand how the vertical (cid:143) ux of horizontal momentum varies with height in a mountain-forced trapped lee-wave train. Taking a sinusoidal form for the wave (cid:142) eld, from the analytical solution for a two-layer Scorer-parameter atmosphere, the constant Bernoulli functional on a streamline is used to diagnose the momentum (cid:143) ux. It is shown that in an inviscid, steady wave train the magnitude of the momentum (cid:143) ux decreases with height as a sinusoidal function. The present theory clearly shows how this pro(cid:142) le of momentum (cid:143) ux with height is a direct consequence of the exact balance between the vertical derivative of momentum (cid:143) ux and the dynamic pressure difference across the mountain in steady state. The simple analytic pro(cid:142) le of (cid:143) ux with height shows a remarkable qualitative similarity with numerical-model results from idealized case-studies of (cid:143) ow over an isolated mountain ridge.