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Mathematical Methods for Physics and Engineering - Matematica.NET

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6.3 APPLICATIONS OF MULTIPLE INTEGRALSThe coordinates of the centre of mass of a solid or laminar body may also bewritten as multiple integrals. The centre of mass of a body has coordinates ¯x, ȳ,¯z given by the three equations∫¯x∫∫dM =∫xdMȳ dM = ydM∫ ∫¯z dM = zdM,where again dM is an element of mass as described above, x, y, z are thecoordinates of the centre of mass of the element dM <strong>and</strong> the integrals are takenover the entire body. Obviously, <strong>for</strong> any body that lies entirely in, or is symmetricalabout, the xy-plane (say), we immediately have ¯z = 0. For completeness, we notethat the three equations above can be written as the single vector equation (seechapter 7)¯r = 1 ∫r dM,Mwhere ¯r is the position vector of the body’s centre of mass with respect to theorigin, r is the position vector of the centre of mass of the element dM <strong>and</strong>M = ∫ dM is the total mass of the body. As previously, we may divide the bodyinto the most convenient mass elements <strong>for</strong> evaluating the necessary integrals,provided each mass element is of constant density.We further note that the coordinates of the centroid of a body are defined asthose of its centre of mass if the body had uni<strong>for</strong>m density.◮Find the centre of mass of the solid hemisphere bounded by the surfaces x 2 + y 2 + z 2 = a 2<strong>and</strong> the xy-plane, assuming that it has a uni<strong>for</strong>m density ρ.Referring to figure 6.5, we know from symmetry that the centre of mass must lie onthe z-axis. Let us divide the hemisphere into volume elements that are circular slabs ofthickness dz parallel to the xy-plane. For a slab at a height z, the mass of the element isdM = ρdV = ρπ(a 2 − z 2 ) dz. Integrating over z, we find that the z-coordinate of the centreof mass of the hemisphere is given by¯z∫ a0ρπ(a 2 − z 2 ) dz =∫ a0zρπ(a 2 − z 2 ) dz.The integrals are easily evaluated <strong>and</strong> give ¯z =3a/8. Since the hemisphere is of uni<strong>for</strong>mdensity, this is also the position of its centroid. ◭6.3.3 Pappus’ theoremsThe theorems of Pappus (which are about seventeen centuries old) relate centroidsto volumes of revolution <strong>and</strong> areas of surfaces, discussed in chapter 2, <strong>and</strong> may beuseful <strong>for</strong> finding one quantity given another that can be calculated more easily.195

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