By V. I. Arnold

ISBN-10: 0387968903

ISBN-13: 9780387968902

During this textual content, the writer constructs the mathematical gear of classical mechanics from the start, reading all of the easy difficulties in dynamics, together with the speculation of oscillations, the idea of inflexible physique movement, and the Hamiltonian formalism. this contemporary process, in line with the speculation of the geometry of manifolds, distinguishes itself from the conventional procedure of normal textbooks. Geometrical issues are emphasised all through and comprise section areas and flows, vector fields, and Lie teams. The paintings encompasses a precise dialogue of qualitative tools of the speculation of dynamical structures and of asymptotic equipment like perturbation innovations, averaging, and adiabatic invariance.

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Additional resources for Mathematical Methods of Classical Mechanics (2nd Edition) (Graduate Texts in Mathematics)

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Line from the north pole of the sphere, say k, through the point r to the place z where the line intersects the complex plane (Fig. 21) Note that points on the equator (ζ = 0) are fixed points of the map, k (ζ = 1) is mapped to the point at infinity, and −k (ζ = −1) is mapped to the origin. The upper hemisphere is mapped outside the unit circle and the lower hemisphere is mapped inside the unit circle. 22) A rotation of R3 induces a single-valued map of the unit sphere into itself and also induces, via the stereographic projection, a map of the complex plane into itself with the same properties.

Then ri = r0 + a + R [(ri − rk ) + (rk − r0 )] = rk + b + R(ri − rk ) where b = r0 − rk + a + R(rk − r0 ) Thus the transformation is again expressed in terms of a translation Tb applied to the new reference point rk and the rotation R which is unchanged by the altered reference point. 4 Rigid Body Transformations Form the Group SE (3) It will now be convenient to take r0 = 0. Then the generic rigid body transformation is r = Rr + a If this is followed by a second rigid body transformation r = Sr + b = SRr + S a + b the result is another rigid body transformation with rotation T = SR and translation c = S a + b.

These circles are mapped to circles in the complex plane (Fig. 8). Note that if the circles are traversed clockwise (seen from the exterior of the sphere) their images will be traversed counterclockwise. 3 Complex Numbers Fig. 8 Rotation of the sphere about n induces, via stereographic projection of the orbits, a map of the complex plane with the fixed point n . the axis of rotation n with the sphere. The details of the argument can be found in the beautifully rendered [11]. We begin by examining the transformation induced by a reflection since any rotation is composed of two reflections.

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Mathematical Methods of Classical Mechanics (2nd Edition) (Graduate Texts in Mathematics) by V. I. Arnold

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