00:01
In this question it is given that if omega is the region between the curve, y is equals to cos hyperbolic x and the x -axis from x is equal to 0 to x is equal to 1, then we need to find the centroid of the solid generated by revolving omega about the x -axis and about the y -axis.
00:29
Let's see how to solve this question.
00:31
The centroid of the solid generated by revolving omega about x -axis can be calculated as x -bar is equals to integration 0 to 1 pi x cos hyperbolic square x d x upon integration 0 to 1 pi cos hyperbolic square x d x.
01:15
By the integration we can write pi into 1 by 2xxxxxxxx plus half sine hyperbolic 2x minus integration 1 by 2x plus half sine hyperbolic 2x minus integration 1 by 2 x plus half half -syn hyperbolic 2x dx and the limits are 0 to 1 upon the integration of this expression pi cos hyperbolic square x d x will be pi by 2 integration 0 to 1 1 plus cos hyperbolic 2x d x this this will be equal to pi into 1x 2x into x plus half, sine hyperbolic 2x minus half and the integration of this expression will be equals to x square by 2 plus 1 by 4, cos hyperbolic 2x and the limits are 0 to 1 upon the value of this integration will be pi by 2 x plus sine hyperbolic 2x upon 2 and the limits are 0 to 1 this will be equals to pi by 8 3 plus 2 sine hyperbolic 2 minus cos hyperbolic 2 upon pi by 4 2 plus sine hyperbolic 2.
04:03
Therefore, the value of x bar will be equals to 3 plus 2 sine hyperbolic 2 minus cos hyperbolic 2 upon 2 into 2 plus sine hyperbolic 2.
04:30
And when omega is revolved about x -axis, the value of y bar will be equals to 0.
04:39
So these are the centroids.
04:45
Now let's come to part b.
04:55
We need to find the centroid of the solid when omega is revolved about y -axis.
05:03
Hence, the value of x bar will be equals to.
05:07
And we need to find the value of y bar...