If a particle of mass m is at a distance r from a given line, then mr2 is called the moment of inertia of the particle about the given line.
MOMENT OF INERTIA If a particle of mass m is at a distance r from a given line, then mr2 is called the moment of inertia of the particle about the given line. This line is refered to as an axis. We extend this concept to a lamina which occupies a region R in the xy-plane with density ρ(x, y) at the point (x, y). We assume ρ(x, y) is continuous. We divide the region R into small rectangles with typical rectangle of area Δx · Δy and element mass ρ(x, y) Δx · Δy. It is also known as polar moment of Inertia. Note that Io = Ix + Iy It is also the M.I of the lamina about an axis perpendicular to the xy-plane. Note: The tendency of the lamina to resist a change in rotational motion about an axis is measured by its moment of inertial about that axis. For example, the M.I of a wheel of a car is what makes it difficult to start or stop the rotation of the wheel. Radius of gyration The radius of gyration of a lamina about an axis is the number R such that MR2 = I, where M is the mass of the lamina and I is the M.I about the axis. Example 1 Find the moment of inertia of a uniform rectangular lamina that occupies the region R in the xy-plane given by 0 ≤ x ≤ a, 0 ≤ y ≤ b about the x-axis, the y-axis and about the origin. Solution Given the rectangular lamina is of constant density ρ. Example 2 Find the moment of inertia of a homogeneous circular disk in the xy-plane with centre origin and radius a about the x-axis and the y-axis. Solution Put y = a sin θ ⸫ dy = acos θ dθ When y = 0, sin θ = 0 ⇒ θ = 0 When y = a, sin θ = 1 ⇒ θ = π/2 Because the region is symmetric about both the axis, Note: So, the M.I of a circular disk of radius a about a diameter is 1/4 Ma2, where M is the mass of the lamina. M.I is circular disk of radius a about an axis through the centre and perpendicular to it is 1/2 Ma2. Example 3 Find Ix, Iy, Iz of the lamina occupying the region R in the xy-plane, where R = {(x,y)|1≤x≤3,1≤ y ≤4} and ρ(x, y) = ky2 Solution Given the lamina occupies a rectangular region in the xy-plane. Example 4 A thin plate covers the triangular region bounded by the x-axis and the lenis x = 1 and y = 2x in the first quadrant. The plate's density at the point (x, y) is ρ(x, y) = 6x + 6y + 6. Find the M.I of the plate about the x-axis, about the y-axis and about the origin. Solution Example 5 Find the moment of inertia about the x-axis of a thin plate bounded by the parabola x = y - y2 and the line x + y = 0 if the density ρ(x, y) = x + y. Solution Example 6 Find the M.I of a uniform elliptic lamina about its major axis and minor axis. Solution Given a uniform elliptic lamina in the xy-plane. Equation of the boundary of the region is the ellipse Its centre is the origin, major and minor axes are the x-axis and the y-axis. That is, M.I about an axis perpendicular to the lamina through its centre is For a solid region, the element mass at the point, P (x, y, z) is ρΔx Δy Δz, where ρ(x,y,z) is the density at P. It may be a constant in some case. We assume ρ(x,y,z) is continuous. Example 1 A solid cube in the first octant is bounded by the coordinate planes and the planes x = 1, y = 1, z = 1. The density of the cube is ρ (x,y,z) = x + y + z + 1. Find the moments of inertia about the coordinate axes. Solution Given a solid cube bounded by the planes x = 0, x = 1, y = 0, y = 1, z = 0, z = 1. Given the density at any point (x, y, z) is ρ (x, y, z) = x + y + z + 1. Example 2 Find Iz for the solid cylinder x2 + y2 ≤ a2, 0 ≤ z ≤ h with constant density ρ. Solution Given a solid cylinder Base circle is x2 + y2 = a2 and height is h. Density ρ is a constant We shall evaluate using cylindrical polar coordinates Note: M.I of a solid cylinder of base radius a about the axis of the cylinder = M/2 a2 Example 3 Find the M.I of a solid sphere of radius a about a diameter. Solution We shall use the basic method of slicing to sphere into circular disks perpendicular to the diameter l and use Riemann sum idea. Consider a typical disk at a distance x from centre O and thickness Δx. ⸫ M.I of the solid sphere about the diameter l is Example 4 Find the M.I of a solid right circular cone about its axis. Solution Consider a solid right circular cone of height h and base circle of radius a choose the vertex of the cone as the origin and its axis as the z-axis as in Fig. 5.105. We shall use basic Riemann sum idea. Divide the solid cone into circular disks perpendicular to the axis. i.e., the z-axis. Take a typical disk at a distance z from O and thickness Δz. ⸫ M.I of the disk about an axis perpendicular to it is The following theorems are useful in finding M.I if the M.I of a body is required about an axis other than the principal axis. Theorem 1 Parallel axis theorem (Steiner's Theorem) If the M.I of a body of mass M about an axis through the centre of gravity is I, then the M.I of the body I' about a parallel axis at a distance d from the first axis is given by I' = I + Md2 Theorem 2 Perpendicular axis theorem If Ix and Iy be the M.I of a plane lamina about two perpendicular axes ox, oy in its plane, then the M.I of the lamina about an axis oz through O and perpendicular to its plane is Iz = Ix + Iy Note: The perpendicular axis theorem is valid only for a plane lamina whereas the parallel axis theorem is valid for any rigid body. Example 5 Find the M.I of a solid right circular cone having base radius a and height h about (i) its axis (ii) an axis through the vertex and perpendicular to its axis (iii) a diameter of its base. Solution Refer Fig. 5.105 in example 4 (i) By example 4, M.I of the cone about the axis of the cone (z-axis) is = 3/10 Ma2 (ii) An axis through the vertex and perpendicular to it is the y-axis (of course the x-axis also) A diameter of the disk is parallel to the y-axis. Since the diameter of base is parallel to the diameter of the disk, by parallel axis theorem, we get ⸫ M.I of the cone about the diameter of the base 1. Find the M.I about the x-axis and the y-axis of the part of the disk x2 + y2 ≤ a2 in the first quadrant and with constant density ρ. 2. Find the M.I, Ix, Iy, Io for an isosceles right triangle with equal sides a if the density at any point is proportional to the square of the distance from the vertex opposite to hypotenuse. [Hint: vertex at right angle as origin as in the figure] 3. Find the M.I about the x-axis of the area enclosed by the line x = 0, y = 0, 4. Find the M.I about the x-axis of a thin plate of density 1 bounded by the circle x2 + y2 = 4. Then use this result to find Iy and Io for the plate. 5. Find the M.I about the y-axis of a thin plate bounded by the x-axis, the lines x = ± 1 and the parabola y = x2 if p(x, y) = 7y + 1. 6. Find the moment of inertia about the z-axis of a homogeneous tetrahedron bounded by the planes x = 0, y = 0, z = x + y and z = 1. 7. Find the M.I of an octant of the ellipsoid 1. Moment of Inertia of a Lamina
WORKED EXAMPLES
2. Moment of Inertia of a Solid in Space
WORKED EXAMPLES
WORKED EXAMPLES
EXERCISE
about the x-axis.
ANSWERS TO EXERCISE
Matrices and Calculus: Unit V: Multiple Integrals : Tag: : Worked Examples, Exercise with Answers - Integrals: Moment of Inertia
Matrices and Calculus
MA3151 1st semester | 2021 Regulation | 1st Semester Common to all Dept 2021 Regulation