Lecture
| The axial moment of resistance is the ratio of the moment of inertia about a given axis to the distance from the axis to the most distant point of the cross section |
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| The polar moment of resistance is the ratio of the polar moment of inertia to the distance from the pole to the most distant point of the cross section |
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| The center of gravity of the cross section of the rod is taken as the pole. |
| Axial moments of resistance for the simplest sections (I xc and I yc are the central moments of inertia of the sections): |
| 1. For a rectangle (fig. 4.10). |
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| 2. For a triangle (Fig. 4.11). |
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| (for upper fibers). |
| Similarly, you can calculate the moments of resistance about the axis of the left and right fibers W St , W pack |
| 3. For the circle (Fig. 4.12). |
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| 4. For the semicircle (Fig.4.13). |
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| 5. For tubular section (Fig. 4.14). |
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| Polar moment of resistance for tubular section. |
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GEOMETRIC CHARACTERISTICS OF FLAT SECTIONS
Terms: GEOMETRIC CHARACTERISTICS OF FLAT SECTIONS