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225 ⎯ x O C r Shape Area ⎯ x ⎯ x ⎯ x ⎯ y ⎯ y Triangular area Quarter-circular area Semicircular area Quarter-elliptical area Semielliptical area Semiparabolic area Parabolic area Parabolic spandrel General spandrel Circular sector C CC ⎯ y ⎯ y CC ⎯ x ⎯ x CC ⎯ y ⎯ y h 3 bh 2 b 2 b 2 4r 4r 3a 4 3a 8 3h 5 3h 10 2ah 3 3h 5 4ah 3 ah 3 4b 4 4r 2 2 4b 4 4a O O O O O O O O r h 0 a a a a a b y = kx2 h h n + 1 n + 2 a n + 1 4n + 2 h ah n + 1 C 0 0 0 ⎯ x ⎯ y y = kxn h C 3α 2r sin α r2α 3� 3� 3� 3�3 3� r2� r2� ab� ab� � � � Fig. 5.8A Centroids of common shapes of areas. 5.4 First Moments of Areas and Lines bee02286_ch05_218-281.indd Page 225 6/24/11 4:31 PM user-f494bee02286_ch05_218-281.indd Page 225 6/24/11 4:31 PM user-f494 /203/MHDQ294/bee02286_disk1of1/0077402286/bee02286_pagefiles/203/MHDQ294/bee02286_disk1of1/0077402286/bee02286_pagefiles 483 Quarter circle C Rectangle Triangle Circle Semicircle Ellipse b y y' x' x 1 12 ⎯Ix' = bh3 1 12 ⎯Iy' = b3h 1 8 Ix = Iy = r4 1 4 J O = r4 1 4 ⎯Ix =⎯Iy = r 4 1 2 J O = r4 1 36 ⎯Ix' = bh3 1 12 Ix = bh3 1 3 Iy = b3h 1 12 J C = bh(b2 + h2) 1 3 Ix = bh3h b x' x x r O y h C h 3 xO C y r xO C y r x b y a 1 16 Ix = Iy = r4 1 8 J O = r4 1 4 ⎯Ix = ab3 1 4 ⎯Iy = a3b 1 4 J O = ab(a2 + b2) O � � � � � � � � � Fig. 9.12 Moments of inertia of common geometric shapes. determination of moments of inertia is thus a prerequisite to the analysis and design of structural members. It should be noted that the radius of gyration of a composite area is not equal to the sum of the radii of gyration of the component areas. In order to determine the radius of gyration of a composite area, it is first necessary to compute the moment of inertia of the area. 9.7 Moments of Inertia of Composite Areas bee02286_ch09_468-555.indd Page 483 8/29/11 11:18 AM user-f494bee02286_ch09_468-555.indd Page 483 8/29/11 11:18 AM user-f494 /203/MHDQ294/bee02286_disk1of1/0077402286/bee02286_pagefiles/203/MHDQ294/bee02286_disk1of1/0077402286/bee02286_pagefiles
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