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Find the mass and centroid (center of mass) of the following thin plates, assuming constant density. Sketch the region corresponding to the plate and indicate the location of the center of mass. Use symmetry when possible to simplify your work. The region bounded by \(y=\sin x\) and \(y=1-\sin x\) between \(x=\pi / 4\) and \(x=3 \pi / 4\)

Short Answer

Expert verified
Question: Find the mass and centroid of the thin plate bounded by the curves \(y = \sin x\) and \(y = 1 - \sin x\) on the interval \([\frac{\pi}{4},\frac{3\pi}{4}]\) with constant density \(\delta\). Solution: The mass of the thin plate is \(M=\delta\pi\), and the centroid is located at the point \((\bar{x},\bar{y}) = \left(\frac{\pi}{2},\frac{\pi}{6}\right)\).

Step by step solution

01

Sketch the region

The given region is bounded by two curves: \(y = \sin x\) and \(y = 1 - \sin x\). First, plot these functions over the given interval \([\frac{\pi}{4}, \frac{3\pi}{4}]\), and then draw the region they define. Notice that the region is symmetric with respect to the line \(x=\frac{\pi}{2}\).
02

Set up and compute integrals

Since this plate has a constant density, we will assume a density \(\delta\). Now we need to find the mass of the plate by integrating over the region and multiplying by density. The mass of the plate, \(M\), can be found as follows: $$M = \delta \int_{\pi/4}^{3\pi/4} [(1 - \sin x) - (\sin x)] dx$$ Now, we can find the moments \(M_x\) and \(M_y\). The centroid of the plate will have coordinates \((\bar{x},\bar{y})\) given by \(\bar{x} = \frac{M_x}{M}\) and \(\bar{y} = \frac{M_y}{M}\). To compute the moments, we evaluate the following integrals: $$M_x = \delta \int_{\pi/4}^{3\pi/4} x[(1 - \sin x) - (\sin x)] dx$$ $$M_y = \delta \int_{\pi/4}^{3\pi/4} \frac{1}{2}[(1 - \sin x) + (\sin x)] [(1 - \sin x) - (\sin x)] dx$$
03

Use symmetry and simplify

Observing that the region is symmetric with respect to the line \(x=\frac{\pi}{2}\), we can use this property to simplify the work. Based on symmetry, we know that \(\bar{x} = \frac{\pi}{2}\). Now we only need to compute \(\bar{y}\). To find \(M\): $$M = \delta \int_{\pi/4}^{3\pi/4} (1 - 2\sin x) dx = \delta \left[x - 2\int_{\pi/4}^{3\pi/4} \sin x dx\right]_{\pi/4}^{3\pi/4} = \delta\left(\frac{\pi}{2} - 2\left[\cos x\right]_{\pi/4}^{3\pi/4}\right) = \delta \pi$$ Now, we find \(M_y\): $$M_y = \delta \int_{\pi/4}^{3\pi/4} \frac{1}{2}(1 - 2\sin x)(1-\sin x) dx = \frac{\delta}{2} \int_{\pi/4}^{3\pi/4} (1 - \sin x)^2 dx$$ To solve this integral, use u-substitution with \(u = 1 - \sin x\), giving \(du = -\cos x dx\), and changing the bounds to correspond to \(u\) values. $$M_y = -\frac{\delta}{2} \int_{\sqrt{2}/2}^{1-\sqrt{2}/2} u^2 du = -\frac{\delta}{6}\left[u^3\right]_{\sqrt{2}/2}^{1-\sqrt{2}/2} = \frac{\delta}{6}\left(\frac{\sqrt{2}}{2} - \frac{1-\sqrt{2}}{2}\right) = \frac{\delta\pi}{6}$$ Now we can find the coordinates of the centroid: $$\bar{x} = \frac{M_x}{M} = \frac{\pi}{2}$$ $$\bar{y} = \frac{M_y}{M} = \frac{\pi}{6}$$ The mass and centroid of the thin plate are \(M = \delta\pi\) and \((\bar{x},\bar{y}) = \left(\frac{\pi}{2},\frac{\pi}{6}\right)\), respectively.

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