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    Book

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    Chapter

    Centres of mass

    Previously we have considered only the motion of particles, which are defined to be bodies whose size does not influence their motion. In the remaining chapters we shall be concerned with bodies whose size has...

    Tony Bridgeman, P. C. Chatwin, C. Plumpton in Mechanics of Groups of Particles (1984)

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    Chapter

    Coplanar forces acting on a rigid body

    In Chapter 4 we discussed the conditions which ensure that a rigid body is in equilibrium under a set of coplanar forces. In the present chapter we consider sets of coplanar forces acting on a rigid body which...

    Tony Bridgeman, P. C. Chatwin, C. Plumpton in Mechanics of Groups of Particles (1984)

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    Chapter

    Momentum, impact and impulse

    The work in this chapter is again based on Newton’s laws, which are first used to establish the principle of conservation of momentum for systems of particles. We also study how to predict the consequences of ...

    Tony Bridgeman, P. C. Chatwin, C. Plumpton in Mechanics of Groups of Particles (1984)

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    Chapter

    Statics

    The purpose of this chapter is to study the conditions under which particles and rigid bodies can rest in equilibrium, that is without moving. This branch of mechanics is called statics.

    Tony Bridgeman, P. C. Chatwin, C. Plumpton in Mechanics of Groups of Particles (1984)

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    Chapter

    The motion of a rigid body about a fixed axis

    The purpose of this final chapter is to investigate the motion of a rigid body turning about a fixed axis. We shall suppose that the axis is smooth, so that its bearings do not exert any frictional couple and ...

    Tony Bridgeman, P. C. Chatwin, C. Plumpton in Mechanics of Groups of Particles (1984)

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    Chapter

    Energy, work and power

    In order to use mathematics efficiently to deal with the mechanics of groups of particles, including rigid bodies, it is helpful first to use Newton’s laws to derive other principles. In this chapter, Newton’s...

    Tony Bridgeman, P. C. Chatwin, C. Plumpton in Mechanics of Groups of Particles (1984)

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    Book

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    Chapter

    Dimensions and bases

    Again we consider displacements as a particular example of vectors and, in the first instance, restrict ourselves to displacements in a fixed plane.

    Tony Bridgeman, P. C. Chatwin, C. Plumpton in Vectors (1983)

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    Chapter

    Applications of vectors

    The results of the preceding chapters are now used in three different circumstances. The principal application to be discussed in this book is the geometry of real space but some elementary kinematical and phy...

    Tony Bridgeman, P. C. Chatwin, C. Plumpton in Vectors (1983)

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    Chapter

    The vector product

    The vector product (often called the cross product) of two vectors a and b, denoted by a × b, or sometimes ab, is defined to be a vector of magnitude |a| |b| sin θ, where θ is the angle contained between a and...

    Tony Bridgeman, P. C. Chatwin, C. Plumpton in Vectors (1983)

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    Chapter

    An introduction to vectors

    In applying mathematics, particularly in the fields of physics and engineering, we need to be able to associate numbers with quantities that are important.

    Tony Bridgeman, P. C. Chatwin, C. Plumpton in Vectors (1983)

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    Chapter

    The scalar product

    In any triangle ABC, the cosine rule states that (3.1) <math display='block'> <mrow> <msup> <mi>c</mi> <mn>2</mn> <...

    Tony Bridgeman, P. C. Chatwin, C. Plumpton in Vectors (1983)

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    Chapter

    Differentiation and integration of vectors

    We have already met vectors which depend on the value of a scalar variable; for example, if r is the position vector of a point on a straight line ...

    Tony Bridgeman, P. C. Chatwin, C. Plumpton in Vectors (1983)