'3 unknowns' diaporamas de présentation

in general, g 1 (x B ,Q 2 ) : dependence on Q 2 (= scaling violations)

h elicity distribution and measurement of N spin. in general, g 1 (x B ,Q 2 ) : dependence on Q 2 (= scaling violations) calculable in perturbative QCD interest in g 1 ( x B ,Q 2 ) is due to its 1 o Mellin moment

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EQUATIONS OF MOTION: GENERAL PLANE MOTION (Section 17.5)

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Chapter 7 Plane Kinetics of Rigid Body

Chapter 7 Plane Kinetics of Rigid Body. y. x. Moment of inertia of a rigid body about an axis. I G is the moment of inertia about G. Example : Moment of inertia of a cylinder about the axis. r. L. d r. a. Parallel axis theorem :. I o = I G + mh 2. Example.

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Back Substitution

Back Substitution. Matrices Solutions. By Dr. Julia Arnold.

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