| William Woolsey Johnson - 1881 - 228 páginas
...Radii of Gyration about Parallel Axes. 193. The moment of inertia of a body about any axis exceeds its **moment of inertia about a parallel axis passing through the centre of gravity,** by the product of the mass and the square of the distance between the axes. Let h be the distance between... | |
| Sir Edward James Reed - 1885 - 369 páginas
...to the middle ordinate, and having obtained this, the necessary modification in order to determine **the moment of inertia about a parallel axis passing through the centre of gravity** of the water section is readily obtained by deducting from the result the area of the water-plane multiplied... | |
| Frank Castle - 1908 - 594 páginas
...theorem is very simple and may be left to the reader, ie the moment of inertia about any axis is equal to **the moment of inertia about a parallel axis passing through the centre of gravity,** together with the product of the mass and the square of the distance between the axes. 1 ml3 ml3 _=_... | |
| Athole James Murray - 1916 - 400 páginas
...where A is the whole area of surface. It is thus seen that (a) The moment of inertia of a plane area **about any axis is equal to the sum of the moment of inertia about a parallel axis** through the centre of gravity of the area and the product of the area by the square of the distance... | |
| Ashok Kr. Mishra - 2006 - 123 páginas
...the axis of rotation passes through its centre of gravity because the moment of inertia, I of a body **about any axis is equal to the sum of the moment of inertia** lg about a parallel axis passing through its centre of gravity and the product of its mass M to the... | |
| C P Kothandaraman, R Rudramoorthy
...X2 A 3.2.3 or I = Ic + ;c2 A 3.2.4 Similarly Ix = IG + y1 A 3.2.5 The moment of inertia of an area **about any axis is equal to the sum of the moment of inertia about a parallel axis** through the centroid and the product of the area and the square of the distance between this axis and... | |
| Anita Jindal
...Hence /0 = / g + M x Thus, the theorem of parallel axes states that the moment of inertia of a body **about any axis is equal to the sum of the moment of inertia** of the body about a parallel axis passing through the centre of gravity and the product of the mass... | |
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