An empty beer can has a mass of 50 g, a length of 12 cm, and a
radius of 3.3 cm. Assume that the shell of the can is a perfect
cylinder of uniform density and thickness.
(a) What is the mass of the lid/bottom?
(b) What is the mass of the shell?
(c) Find the moment of inertia of the can about the cylinder's axis
of symmetry.
(a) The mass has three components, M = Mlid + Mshell + Mbottom = 50 g, where the lid and the bottom are identical. Mass is proportional to the surface area for uniform objects. The area of the lid and bottom is that of a circle, Acircle = ?r2 . The surface area of a cylindrical shell is Ashell = 2?rL. So the total area of can is Atotal = 2Acircle + Ashell = 2?rL + 2?r2 = 2?r(r + L). So the mass of the lid or bottom is given by . Thus Mlid = 5.392 g.
(b) Similarly, the mass of the shell is given by . Thus Mshell = 39.216 g.
(c) The total moment of inertia of the beer can is given by the sum of the individual pieces, Itotal = Ilid + Ishell + Ibottom. Since each piece is revolving about its centre of mass, we do not need the parallel axis theorem. Looking up the moments of inertia of a flat solid disk and a thin cylindrical shell, we have Itotal = 2Mlidr2 + Mshellr2 = 4.86
An empty beer can has a mass of 50 g, a length of 12 cm, and a
radius of 3.3 cm. Assume that the shell of the can is a perfect
cylinder of uniform density and thickness.
(a) What is the mass of the lid/bottom?
(b) What is the mass of the shell?
(c) Find the moment of inertia of the can about the cylinder's axis
of symmetry.
(a) The mass has three components, M = Mlid + Mshell + Mbottom = 50 g, where the lid and the bottom are identical. Mass is proportional to the surface area for uniform objects. The area of the lid and bottom is that of a circle, Acircle = ?r2 . The surface area of a cylindrical shell is Ashell = 2?rL. So the total area of can is Atotal = 2Acircle + Ashell = 2?rL + 2?r2 = 2?r(r + L). So the mass of the lid or bottom is given by . Thus Mlid = 5.392 g.
(b) Similarly, the mass of the shell is given by . Thus Mshell = 39.216 g.
(c) The total moment of inertia of the beer can is given by the sum of the individual pieces, Itotal = Ilid + Ishell + Ibottom. Since each piece is revolving about its centre of mass, we do not need the parallel axis theorem. Looking up the moments of inertia of a flat solid disk and a thin cylindrical shell, we have Itotal = 2Mlidr2 + Mshellr2 = 4.86
(a) The mass has three components, M = Mlid + Mshell + Mbottom = 50 g, where the lid and the bottom are identical. Mass is proportional to the surface area for uniform objects. The area of the lid and bottom is that of a circle, Acircle = ?r2 . The surface area of a cylindrical shell is Ashell = 2?rL. So the total area of can is Atotal = 2Acircle + Ashell = 2?rL + 2?r2 = 2?r(r + L). So the mass of the lid or bottom is given by . Thus Mlid = 5.392 g.
(b) Similarly, the mass of the shell is given by . Thus Mshell = 39.216 g.
(c) The total moment of inertia of the beer can is given by the sum of the individual pieces, Itotal = Ilid + Ishell + Ibottom. Since each piece is revolving about its centre of mass, we do not need the parallel axis theorem. Looking up the moments of inertia of a flat solid disk and a thin cylindrical shell, we have Itotal = 2Mlidr2 + Mshellr2 = 4.86
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