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Titlebook: Dynamic Analysis of Ocean Structures; Bruce J. Muga,James F. Wilson Book 1970 Springer Science+Business Media New York 1970 earthquake pre

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Nonlinear Response of a Moored Ship to Sea Oscillationsizontal lines, as shown in Figure 13.2. It will be shown that these assumptions lead to a nonlinear differential equation of motion which is a special form of the more general one derived by Wilson (1951).
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s from the growing realization that design on a purely deterministic basis is inadequate for structures sub­ ject to random loads, which are best described by statistical (or probability) methods. This book is an attempt to bridge the gap between present design practices and available analytical tec
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https://doi.org/10.1007/978-3-322-84864-2res for which the wind loadings dominate the loading pattern and second, many of the wind effects are also present in the case of surface water waves and thus a knowledge of the wind effects serve as a proper introduction to surface water wave excitation.
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Politische Konjunkturzyklen und Wahlens, a statistical approach is used to describe the damage accumulation in materials subjected to random type loads and to corrosive environments. Numerical examples are included which illustrate the use of the theory to estimate probable lifetimes of certain ocean structures.
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Dynamic Behavior of Materials in an Environments, a statistical approach is used to describe the damage accumulation in materials subjected to random type loads and to corrosive environments. Numerical examples are included which illustrate the use of the theory to estimate probable lifetimes of certain ocean structures.
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Book 1970 growing realization that design on a purely deterministic basis is inadequate for structures sub­ ject to random loads, which are best described by statistical (or probability) methods. This book is an attempt to bridge the gap between present design practices and available analytical techni­ ques
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Paradoxien der Rückwärtsrechnungurs at the boundary of an ocean current and still water. The end result is a change in the ‘apparent’ wave lengths and direction of the incident waves. The change in wave lengths also appears as a change in wave steepness. For details, the reader is referred to the paper by Johnson (1947).
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