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Titlebook: Classical Mechanics; B. P. Cowan Book 1984 B. P. Cowan 1984 Aristotle.Hamiltonian mechanics.mechanics.science

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發(fā)表于 2025-3-21 17:41:57 | 只看該作者 |倒序?yàn)g覽 |閱讀模式
書目名稱Classical Mechanics
編輯B. P. Cowan
視頻videohttp://file.papertrans.cn/228/227091/227091.mp4
叢書名稱Student Physics Series
圖書封面Titlebook: Classical Mechanics;  B. P. Cowan Book 1984 B. P. Cowan 1984 Aristotle.Hamiltonian mechanics.mechanics.science
描述The study of mechanics plays a central role in physics for a whole variety of reasons. It was one of the earliest of the quantitative sciences, and had immediate practical applications. These ranged from the study of the motion of projectiles in warfare to the motion of the planets, predicting the seasons, eclipses, etc. At the present time, even though superseded on the very small scale by quantum theory and on the very large scale by the theory of relativity, the mechanics of Newton is perfectly adequate for treating a wide spectrum of problems from the ? ‘"etic theory of gases to the motion of space vehicles. Furthermore, the science of mechanics is regarded by many as the epitome of a good scientific theory and for this reason is studied by philosophers and social scientists alike as an exemplar of the ‘scientific method‘. We shall commence in Chapter 1 with a brief historical outline of the development of mechanics, mentioning the names and dates of the main participants and summarizing their contributions. Preface vii Chapter 1 Newton‘s laws 1. 1 Historical introduction Primitive ideas about mechanics were exemplified by the state- ments of Aristotle (384-322 Be), who asserte
出版日期Book 1984
關(guān)鍵詞Aristotle; Hamiltonian mechanics; mechanics; science
版次1
doihttps://doi.org/10.1007/978-94-010-9171-8
isbn_softcover978-0-7102-0280-2
isbn_ebook978-94-010-9171-8
copyrightB. P. Cowan 1984
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沙發(fā)
發(fā)表于 2025-3-21 21:08:17 | 只看該作者
Student Physics Serieshttp://image.papertrans.cn/c/image/227091.jpg
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發(fā)表于 2025-3-22 11:32:33 | 只看該作者
Dynamics of a single particle,The general problem treated in this chapter is the solution of the dynamics of a single particle once the force field is specified. In most cases, since we shall be dealing with conservative systems, the force will be obtained from a potential energy function.
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發(fā)表于 2025-3-22 14:57:51 | 只看該作者
Many-particle systems,There is a sense in which a body made up of a number of parts (atoms, say) may be regarded as a point mass. We have made such an assumption in previous chapters, even when considering an object as large as the sun! It is the purpose of this section to investigate the extent to which this assumption is valid.
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Reproductive Laws for the 1990sacting with forces that are so’ stiff’ that the separation between any two particles remains constant. From the considerations of the previous chapter we know that these internal forces do not affect the dynamics of the body. What distinguishes a rigid body from a point mass is its extension in spac
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發(fā)表于 2025-3-23 05:47:05 | 只看該作者
Reproductive Laws for the 1990sthe motion at a point to the motion close by. This may be regarded as a . view of the dynamics of the system. By contrast, we now adopt a . view—what can we say about the whole trajectory of our system? In other words, we shall (for the time being) concentrate our attention on the . to the equations
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