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pappus theorem is explained with exapmles in this lecture note, it is used in MATH-II class.
Typology: Lecture notes
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Proof We draw the axis of revolution as the x-axis with the region R in the first quadrant (Figure 6.5 6). We let L(y) denote the length of the cross-section of R perpendicular to the y-axis at y. We assume L(y) to be continuous. By the method of cylindrical shells, the volume of the solid generated by revolving the region about the x-axis is
(10)
The y-coordinate of R’s centroid is
so that
Substituting for the last integral in Equation (10) gives With equal to we have
disk of radius a about an axis in its plane at a distance from its center (Figure 6.57). Solution We apply Pappus’s Theorem for volumes. The centroid of a disk is located at its center, the area is is the distance from the centroid to the axis of revolution (see Figure 6.57). Substituting these values into Equation (9), we find the volume of the torus to be
The next example shows how we can use Equation (9) in Pappus’s Theorem to find one of the coordinates of the centroid of a plane region of known area A when we also know the volume V of the solid generated by revolving the region about the other coordinate axis. That is, if is the coordinate we want to find, we revolve the region around the x-axis so that is the distance from the centroid to the axis of revolution. The idea is that the rotation generates a solid of revolution whose volume V is an already known quantity. Then we can solve Equation (9) for which is the value of the centroid’s coordinate
Solution We consider the region between the semicircle (Figure 6.58) and the x-axis and imagine revolving the region about the x-axis to generate a solid sphere. By symmetry, the x-coordinate of the centroid is With in Equation (9), we have
y = V 2 pA
s 4 > 3 dpa^3 2 ps 1 > 2 dpa^2
3 p a.
x = 0. y = r
y = 2 a^2 - x^2
r, y.
y = r
y
V = 2 psbdspa^2 d = 2 p^2 ba^2.
A = pa^2 , and r = b
b Ú a
V = 2 prA.
Ay V = 2 pyA. r y,
d
c
y Ls yd dy = Ay.
y = L^ ' y= y, dA = L( y) dy
d
c
y
dA
A
d
c
y Ls yd dy
A
d
c
2 psshell radiusdsshell heightd dy = 2 p L
d
c
y Ls yd dy.
If a plane region is revolved once about a line in the plane that does not cut through the region’s interior, then the volume of the solid it generates is equal to the region’s area times the distance traveled by the region’s centroid during the revolution. If is the distance from the axis of revolution to the centroid, then V = 2 prA. (9)
r
x
y
d
y
c
0
L ( y )
R
Centroid
FIGURE 6.56 The region R is to be revolved (once) about the x-axis to generate a solid. A 1700-year-old theorem says that the solid’s volume can be calculated by multiplying the region’s area by the distance traveled by its centroid during the revolution.
Area: pa^2 Circumference: 2 pa
Distance from axis of revolution to centroid
a
b
y
z
x
FIGURE 6.57 With Pappus’s first theorem, we can find the volume of a torus without having to integrate (Example 6).
Centroid
a
a x
y
3
4
FIGURE 6.58 With Pappus’s first theorem, we can locate the centroid of a semicircular region without having to integrate (Example 7).
If an arc of a smooth plane curve is revolved once about a line in the plane that does not cut through the arc’s interior, then the area of the surface generated by the arc equals the length L of the arc times the distance traveled by the arc’s centroid during the revolution. If is the distance from the axis of revolution to the centroid, then S = 2 prL. (11)
r
The proof we give assumes that we can model the axis of revolution as the x-axis and the arc as the graph of a continuously differentiable function of x.
Proof We draw the axis of revolution as the x-axis with the arc extending from to in the first quadrant (Figure 6.59). The area of the surface generated by the arc is
(12)
The y-coordinate of the arc’s centroid is
Hence
Substituting for the last integral in Equation (12) gives With equal to we have
Solution From Figure 6.57, the surface of the torus is generated by revolving a circle of radius a about the z-axis, and is the distance from the centroid to the axis of revolu- tion. The arc length of the smooth curve generating this surface of revolution is the cir- cumference of the circle, so Substituting these values into Equation (11), we find the surface area of the torus to be
S = 2 psbds 2 pad = 4 p^2 ba.
L = 2 pa.
b Ú a
S = 2 prL.
yL S = 2 pyL. r y,
x = b
x = a
y ds = yL.
y = L
x = b
x = a
y
ds
x = b
x = a
ds
x = b
x = a
y ds
L
x = b
x = a
2 py ds = 2 p L
x = b
x = a
y ds.
x = b
x = a
is the arc’s length and ' y= y.
L = 1 ds
0
x
y ds
y
a
b
~
Arc
FIGURE 6.59 Figure for proving Pappus’s Theorem for surface area. The arc length differential ds is given by Equation (6) in Section 6.3.
Thin Plates with Constant Density In Exercises 1–14, find the center of mass of a thin plate of constant density covering the given region.
1. The region bounded by the parabola and the line 2. The region bounded by the parabola and the x-axis 3. The region bounded by the parabola and the line 4. The region enclosed by the parabolas y = x^2 - 3 and y = - 2 x^2
y = -x
y = x - x^2
y = 25 - x^2
y = x^2 y = 4
d
5. The region bounded by the y-axis and the curve 6. The region bounded by the parabola and the line 7. The region bounded by the x-axis and the curve 8. The region between the curve and the x-axis
y = sec^2 x,-p> 4 … x … p> 4
y = cos x,
x = y^2 - y y = x
0 … y … 1
x = y - y^3 ,