The moment of inertia of a rectangle with base b and height h about an axis through its centroid parallel to the base is
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Rectangle Moment of Inertia. About centroidal axis parallel to base b: \(I_{cx = bh^3 / 12\). About centroidal axis parallel to height h: \(I_{cy = hb^3 / 12\). About base b: \(I_{base = bh^3 / 3\).
The area moment of inertia (\(I\)) measures the resistance of a cross-section to bending. For a rectangular cross-section with base \(b\) and height \(h\), the moment of inertia about an axis passing through its centroid (geometric center) and parallel to the base (let's call this the x-axis, \(I_{cx}\)) is given by the standard formula:
$$ I_{cx} = \frac{bh^3}{12} $$
The moment of inertia about an axis through the centroid parallel to the height (y-axis) would be \(I_{cy} = \frac{hb^3}{12}\). The moment of inertia about the base itself (\(I_{base}\)) can be found using the parallel axis theorem: \(I_{base} = I_{cx} + A d^2 = \frac{bh^3}{12} + (bh)(h/2)^2 = \frac{bh^3}{12} + \frac{bh^3}{4} = \frac{bh^3}{3}\). Option (1) is the MOI about the base, while option (2) is the MOI about the centroidal axis parallel to the base.