Homework # 4

Section 7.4

4) The exact value of the integral is easy to obtain.

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Let's compare this to the approximation obtained with Simpson's rule, tex2html_wrap_inline225 . To subdivide the interval into 2 subintervals, we need 3 equally spaced points tex2html_wrap_inline227 Define h=(b-a)/2.

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As we can see, the approximation given by Simpson's rule is in fact the exact value of the definite integral.

6)

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a) To evaluate tex2html_wrap_inline235 , we need 5 equally spaced points in the interval [a,b]=[0,2]. If tex2html_wrap_inline239 then tex2html_wrap_inline241 .

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b) Theorem 4 in Section 7.4 provides an upper bound for the approximation error

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n is 4 in our case and tex2html_wrap_inline249 is an upper bound for tex2html_wrap_inline251 , which we still need to determine.

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We need to find the largest value of tex2html_wrap_inline255 for tex2html_wrap_inline257 . A graph could be used to determine the smallest and largest values of tex2html_wrap_inline259 . We will instead define tex2html_wrap_inline261 and use the standard techniques of calculus to identify the maxima and minima of g.

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It is easy to see that tex2html_wrap_inline267 because only even powers of x occur. g'(x) > 0 on the interval (0,2] and therefore g is increasing. Notice moreover that tex2html_wrap_inline277 and g increases for the rest of the interval. The largest value of tex2html_wrap_inline281 is therefore attained at x=2. If tex2html_wrap_inline285 then tex2html_wrap_inline249 will be an upper bound. Plugging everything back into our original inequality

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.

e) We need to find a condition on n that will guarantee that tex2html_wrap_inline293 . Consider that

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Using algebra, we see that when tex2html_wrap_inline297 the error is as desired.

9) We have the following inequalities

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where I is the exact value of indefinite integral. These inequalities can be justified with a picture. For each one of the methods, draw the rectangle or trapezoid that is used to estimate the area above a single subinterval tex2html_wrap_inline303 .

Unfortunately, it is impossible to determine where tex2html_wrap_inline305 belongs in this sequence of inequalities. It is clear that because tex2html_wrap_inline307 is a weighted average of tex2html_wrap_inline309 and tex2html_wrap_inline311 ,

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that tex2html_wrap_inline307 belongs in between tex2html_wrap_inline309 and tex2html_wrap_inline311 . Nothing about tex2html_wrap_inline305 can stated with such certainty.

11) In this case h=(b-a)/n=3/4 and f is given at all the points tex2html_wrap_inline327 .

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An upper bound for tex2html_wrap_inline331 is obviously tex2html_wrap_inline333 .

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Section 8.1

4) a) I redrew the curve tex2html_wrap_inline337 using an identical scale for the x and y axis. I then placed a shoelace on top of the curve and measured the length of the string with a ruler. I obtained 72 mm as an estimate for the length. My scale on the bottom of the graph was 1 unit = 50 mm. 72 mm was therefore equivalent to 1.44 units.

b) Using the trapezoid rule with 2 subdivisions, we can give the area under the curve an eyeball estimate of 1.47 units.

c) The only error bound available for the midpoint rule is given in Section 7.4, Theorem 3, as

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where

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For tex2html_wrap_inline349 ,

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where we have made the numerator as large as possible (x=1) and the denominator as small as possible (x=0). Plugging this information into our inequality we obtain

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d) Before we apply identity 35 in the book we will manipulate the integrand in order to put it into a convenient form.

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Section 8.2

1) See Figure 1 (at bottom) for a picture of the solid of revolution. Each cross-section of the solid, at x, is a circle of radius tex2html_wrap_inline363 . We therefore have tex2html_wrap_inline365 . Cross-sections of the volume are taken at each tex2html_wrap_inline367 .

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2) See Figure 2 (at bottom) for a picture of the solid of revolution. Each cross-section of the solid, at x, is a ``washer''. The outer radius of the washer is 1 and the inner radius is tex2html_wrap_inline373 . The area of the washer is therefore given by

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The region bounded is bounded on the left and the right by tex2html_wrap_inline377 respectively. The integration is therefore performed from 0 to 1.

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9) Consider the line tex2html_wrap_inline381 . The graph of this line is given in Figure 3 (at bottom). If the region below the curve and between x=0,x=h is rotated around the x-axis, we obtain the cone mentionned in the question. For tex2html_wrap_inline387 , the cross-section is a circle of radius rx/h and its area is

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17) If at each height, we knew the radius of the pole, r(h), then we could make a picture like Figure 4 (at bottom). This picture shows that we could obtain the volume of the pole as the volume of the solid of revolution about the h-axis for the curve r. Cross-sections at h would be be circles of radius r and their area would be tex2html_wrap_inline405

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This last integral will be approximated with Simpson's rule but first we need to derive an expression for r(h). We only know the circumference, C, at a given height, tex2html_wrap_inline413 . The relationship between radius and circumference of a circle is

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Let's build a new table of values using the right-hand side identity.

height h 0 10 20 30 40 50 60
radius r 2.5465 2.2282 1.5915 0.7958 0.4775 0.3183 0.1592

The interval [0,60] is subdivided into 6 subintervals of length h=10.

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26) Figure 5 (at bottom) is useful to identify the axes. Figure 6 is a sketch of the top half of the intersection of the two full cylinders. A cross-section taken perpendicularly to the z-axis is clearly a square. The top and bottom edges of the square are the intersection of the plane (perpendicular to the z-axis) and the horizontal cylinder. In Figure 7, the dark outline of a rectangle indicates the position of the intersection of this plane with the full cylinder. To calculate the lenght of the vertical edges of the square we will try to obtain the distance between the two horizontal edges. These two horizontal edges are clearly identified in Figure 7 as the edges of the intersection of the plane and the surface of the cylinder. Figure 8 is a cross-section perpendicular to the x-axis of the horizontal cylinder intersecting our plane. The strip has width 2H where, according to Pythagoras's theorem,

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for tex2html_wrap_inline437 .

This shows that one of the sides of the original square cross-section is

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The area of the cross-section is therefore tex2html_wrap_inline441 . To every tex2html_wrap_inline437 there corresponds a unique cross-section and so we must integrate from -R to R.

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