In mathematics, engineering, and manufacturing, a solid of revolution is a solid figure obtained by rotating a plane figure around some straight line (the axis) that lies on the same plane.
Assuming that the figure lies entirely on one side of the axis, the solid's volume is equal to the length of the circle described by the figure's barycenter, times the figure's area.
A representative disk is three-dimensional volume element of a solid of revolution. The element is created by rotating a line segment (of length "w") around some axis (located "r" units away); such that, a cylindrical volume, of π∫r2w units, is enclosed.
If one of the bounding curves is actually the x-axis, then we can let in the formula above, and we have:
As above, we can use
if one of the bounding curves is actually the x-axis.
To visualize how this works, consider a function like , on the interval * being revolved about the x-axis. If you imagine looking at the graph from the side (so that you are right behind the y-axis) and see the representative slice being revolved about the x-axis, it would form a circle, the area of which is . Summing up every one of the areas of the circles (i.e. the definite integral) gives you the total volume. This is a special case of the Disc method, where r(x)=0.
To visualize how this works, consider the same function and bounds as before, but this time being revolved about the y-axis. If you look at it from above and revolve the slice around the y-axis, it forms a cylinder with no top or bottom. The lateral surface area of any cylinder is given by , where p is the radius (just keeping it in terms of the formula), and h is the height. Summing up all of the surface areas along the interval (i.e. the definite integral) gives you the total volume.
Rotationskörper | Théorème de Guldin | 回転体 | omwentelingslichaam
This article is licensed under the GNU Free Documentation License.
It uses material from the
"Solid of revolution".
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