標(biāo)題: Titlebook: Electromagnetic Wave Propagation in Turbulence; Evaluation and Appli Richard J. Sasiela Book 1994 Springer-Verlag Berlin Heidelberg 1994 In [打印本頁] 作者: T-Lymphocyte 時(shí)間: 2025-3-21 18:53
書目名稱Electromagnetic Wave Propagation in Turbulence影響因子(影響力)
書目名稱Electromagnetic Wave Propagation in Turbulence影響因子(影響力)學(xué)科排名
書目名稱Electromagnetic Wave Propagation in Turbulence網(wǎng)絡(luò)公開度
書目名稱Electromagnetic Wave Propagation in Turbulence網(wǎng)絡(luò)公開度學(xué)科排名
書目名稱Electromagnetic Wave Propagation in Turbulence被引頻次
書目名稱Electromagnetic Wave Propagation in Turbulence被引頻次學(xué)科排名
書目名稱Electromagnetic Wave Propagation in Turbulence年度引用
書目名稱Electromagnetic Wave Propagation in Turbulence年度引用學(xué)科排名
書目名稱Electromagnetic Wave Propagation in Turbulence讀者反饋
書目名稱Electromagnetic Wave Propagation in Turbulence讀者反饋學(xué)科排名
作者: 反復(fù)無常 時(shí)間: 2025-3-21 21:20
Introduction,t the results as parametric curves. Many cases are run to develop some insight into how a quantity of interest varies with parameters. Becoming an expert in this field requires a great deal of time to become familiar with these graphical results so that one has some insight into various effects.作者: intrude 時(shí)間: 2025-3-22 03:32
Other Applications of Mellin Transforms,ing (. and . 1975), in summing series and in probability theory (. and . 1988), and by using the scale-invariant property of Mellin transforms to do optical processing of images (. and . 1976a, 1976b; . and . 1983). Some of these applications are considered in this chapter.作者: inventory 時(shí)間: 2025-3-22 07:06
Examples with a Single Complex Parameter,se. To express results as integrals, the approach in Chap. 2 is followed to the point where the propagation parameter γ was assumed to be real. Here γ must be complex to handle beams of finite extent. I derive the filter function for two counterpropa-gating or copropagating waves.作者: indifferent 時(shí)間: 2025-3-22 09:59
Basic Equations for Wave Propagation in Turbulence,dered in this book. This equation is used to find phase and log-amplitude variances. These expressions are modified to obtain expressions for the power spectral density, given in (2.101), beam profile given in (2.109), and Strehl ratio, which is the ratio of on-axis intensity to that of a diffraction-limited wave, in (2.111).作者: creditor 時(shí)間: 2025-3-22 14:50 作者: creditor 時(shí)間: 2025-3-22 19:03 作者: 神化怪物 時(shí)間: 2025-3-23 00:02
Book 1994s. Ample examples of application are outlined and solutions for many problems in turbulence theory are given. The method itself relates to asymptotic results that are applicable to a broad class of problems for which many asymptotic methods had to be employed previously.作者: ELUC 時(shí)間: 2025-3-23 01:53
0931-7252 gral tables. Ample examples of application are outlined and solutions for many problems in turbulence theory are given. The method itself relates to asymptotic results that are applicable to a broad class of problems for which many asymptotic methods had to be employed previously.978-3-642-85072-1978-3-642-85070-7Series ISSN 0931-7252 作者: colloquial 時(shí)間: 2025-3-23 07:00
APPROXIMATE SOLUTIONS: THE INTEGRAL METHOD,ing (. and . 1975), in summing series and in probability theory (. and . 1988), and by using the scale-invariant property of Mellin transforms to do optical processing of images (. and . 1976a, 1976b; . and . 1983). Some of these applications are considered in this chapter.作者: Armory 時(shí)間: 2025-3-23 13:27 作者: PON 時(shí)間: 2025-3-23 15:20 作者: intimate 時(shí)間: 2025-3-23 20:03
dered in this book. This equation is used to find phase and log-amplitude variances. These expressions are modified to obtain expressions for the power spectral density, given in (2.101), beam profile given in (2.109), and Strehl ratio, which is the ratio of on-axis intensity to that of a diffraction-limited wave, in (2.111).作者: outset 時(shí)間: 2025-3-23 23:36 作者: ATOPY 時(shí)間: 2025-3-24 05:34
https://doi.org/10.1007/978-3-319-29841-2eam profile after propagating through uncorrected turbulence, or through a medium with turbulence-induced beam jitter present, or with anisoplanatic effects can all be represented as special cases of a general integral. Results from evaluating the general integral are used to find the average beam profiles for the three specific cases.作者: 編輯才信任 時(shí)間: 2025-3-24 07:02 作者: CHIDE 時(shí)間: 2025-3-24 12:00 作者: GRIN 時(shí)間: 2025-3-24 16:35
Book 1994tion in turbulence. In a systematic way the monograph presents the Mellin transforms to evaluate analytically integrals that are not in integral tables. Ample examples of application are outlined and solutions for many problems in turbulence theory are given. The method itself relates to asymptotic 作者: 膠狀 時(shí)間: 2025-3-24 20:54
Liqiu Wang,Xuesheng Zhou,Xiaohao Wei scale, into a Taylor series, and integrated term by term. Since the integral over each term of the power series converges absolutely, this method is valid. Tatarski expressed the resulting power series as a hypergeometric function. His approach does not always work with zero inner scale and restric作者: allude 時(shí)間: 2025-3-24 23:09
Latif M. Jiji,Amir H. Danesh-Yazdiequencies. I show that finite size sources and apertures can significantly reduce scintillation. Characteristic sizes for the source and aperture at which the reduction is significant are found. Inner scale is found to reduce the scintillation for typical inner-scale sizes. Scintillation of a beam c作者: annexation 時(shí)間: 2025-3-25 07:20 作者: 人類的發(fā)源 時(shí)間: 2025-3-25 07:51 作者: 打谷工具 時(shí)間: 2025-3-25 11:49 作者: 婚姻生活 時(shí)間: 2025-3-25 18:05
Mellin Transforms in , Complex Planes,al transform coordinate in which there are two or more parameters in the integrand is addressed in this chapter. I show that it can be evaluated to give a series solution. The remaining integration over the propagation path can be performed term by term in most cases. For some cases the infinite ser作者: investigate 時(shí)間: 2025-3-25 22:32 作者: occurrence 時(shí)間: 2025-3-26 01:19
Basic Equations for Wave Propagation in Turbulence,uations are solved with the Rytov approximation, and the main result is given in (2.85), which is the starting point for all turbulence problems considered in this book. This equation is used to find phase and log-amplitude variances. These expressions are modified to obtain expressions for the powe作者: acrimony 時(shí)間: 2025-3-26 08:20 作者: Palpate 時(shí)間: 2025-3-26 10:06 作者: 嘲弄 時(shí)間: 2025-3-26 13:26
Integral Evaluation with Mellin Transforms,rmalization, the wavenumber (.) integration can be expressed in a standard form depending only on zero, one, or more parameters. If no parameters are present, the integration is performed simply by table lookup as was done in the last chapter. The one parameter case requires a transformation of the 作者: novelty 時(shí)間: 2025-3-26 19:38 作者: 憤怒歷史 時(shí)間: 2025-3-26 22:36
Examples with a Single Positive Parameter,uter scale with both von Kármán and Greenwood models for outer scale effects. It is shown that outer scale significantly affects tilt even if the diameter is much smaller than the outer scale. It is shown that inner scale limits the maximum tilt that can be measured on an aperture. Tilt is calculate作者: MURKY 時(shí)間: 2025-3-27 01:13 作者: 因無茶而冷淡 時(shí)間: 2025-3-27 05:40
Mellin Transforms with a Complex Parameter,teepest-descent contribution to an asymptotic solution. In some problems, the spatial filter functions contain a decaying exponential times a function that grows exponentially when γ is complex. Consequently, the Mellin convolution relation must be generalized to allow for convergent integrals that 作者: Dna262 時(shí)間: 2025-3-27 11:09 作者: Glutinous 時(shí)間: 2025-3-27 16:02 作者: 誘騙 時(shí)間: 2025-3-27 19:15 作者: Monocle 時(shí)間: 2025-3-28 00:41
978-3-642-85072-1Springer-Verlag Berlin Heidelberg 1994作者: Humble 時(shí)間: 2025-3-28 03:08
Electromagnetic Wave Propagation in Turbulence978-3-642-85070-7Series ISSN 0931-7252 作者: Synapse 時(shí)間: 2025-3-28 09:59
https://doi.org/10.1007/978-3-642-85070-7Integrals; Mellin Transforms; Turbulance; adaptive optics; asymptotic series; electromagnetic wave; optics作者: TOXIN 時(shí)間: 2025-3-28 12:40
https://doi.org/10.1007/978-3-030-05882-1The mathematical technique developed in the last chapter is used to find analytical solutions to seven problems. The first three are purely mathematical problems, and the last four are problems related to turbulence.作者: adequate-intake 時(shí)間: 2025-3-28 16:45 作者: 打擊 時(shí)間: 2025-3-28 20:58
J. R. T. C. Roelandt,M. Pozzolihapter explicit filter functions are derived for many cases of interest. First, those needed to calculate variances of any Zernike mode on an unobscured circular aperture are found. Next, expressions to find piston and tilt on an annular aperture are derived.作者: saturated-fat 時(shí)間: 2025-3-29 01:38 作者: 帽子 時(shí)間: 2025-3-29 03:51 作者: 粗糙濫制 時(shí)間: 2025-3-29 07:59 作者: 排斥 時(shí)間: 2025-3-29 13:49 作者: follicle 時(shí)間: 2025-3-29 16:55 作者: organism 時(shí)間: 2025-3-29 22:58
uations are solved with the Rytov approximation, and the main result is given in (2.85), which is the starting point for all turbulence problems considered in this book. This equation is used to find phase and log-amplitude variances. These expressions are modified to obtain expressions for the powe作者: Expand 時(shí)間: 2025-3-30 02:07 作者: 人充滿活力 時(shí)間: 2025-3-30 06:40
Heartbeat Sensor Projects with PulseSensoros as integrals. Different cases differ only in the appearance of different filter functions. In the last chapter explicit filter functions were derived for a variety of problems. With the use of these filter functions, integrands contain the following functions: sin (.), cos (.), sin. (.), cos. (.)作者: Adulate 時(shí)間: 2025-3-30 11:57 作者: 高射炮 時(shí)間: 2025-3-30 13:00
APPROXIMATE SOLUTIONS: THE INTEGRAL METHOD,a spherical magnet (. et al. 1975), for Doppler signal processing (. and . 1976), in transient propagation (. 1987), to analyze mammalian hearin (. 1978), for quantum field theory (. and . 1975; . and . 1987), for nonlinear systems (. 1970), in chaos theory (. et al. 1987), in digital signal process作者: 使增至最大 時(shí)間: 2025-3-30 16:32
