Chapter 8: Problem 3
Explain geometrically how the Trapezoid Rule is used to approximate a definite integral.
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Chapter 8: Problem 3
Explain geometrically how the Trapezoid Rule is used to approximate a definite integral.
These are the key concepts you need to understand to accurately answer the question.
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Exact Simpson's Rule a. Use Simpson's Rule to approximate \(\int_{0}^{4} x^{3} d x\) using two subintervals \((n=2) ;\) compare the approximation to the value of the integral. b. Use Simpson's Rule to approximate \(\int_{0}^{4} x^{3} d x\) using four subintervals \((n=4) ;\) compare the approximation to the value of the integral. c. Use the error bound associated with Simpson's Rule given in Theorem 8.1 to explain why the approximations in parts (a) and (b) give the exact value of the integral. d. Use Theorem 8.1 to explain why a Simpson's Rule approximation using any (even) number of subintervals gives the exact value of \(\int_{a}^{b} f(x) d x,\) where \(f(x)\) is a polynomial of degree 3 or less.
Evaluate the following integrals. $$\int \cot ^{5} 3 x d x$$
Use numerical methods or a calculator to approximate the following integrals as closely as possible. The exact value of each integral is given. $$\int_{0}^{\pi / 2} \ln (\sin x) d x=\int_{0}^{\pi / 2} \ln (\cos x) d x=-\frac{\pi \ln 2}{2}$$
Maximum path length of a projectile (Adapted from Putnam Exam 1940) A projectile is launched from the ground with an initial speed \(V\) at an angle \(\theta\) from the horizontal. Assume the \(x\) -axis is the horizontal ground and \(y\) is the height above the ground. Neglecting air resistance and letting \(g\) be the acceleration due to gravity, it can be shown that the trajectory of the projectile is given by $$ \begin{array}{l} y=-\frac{1}{2} k x^{2}+y_{\max }, \quad \text { where } k=\frac{g}{(V \cos \theta)^{2}} \\ \text { and } y_{\max }=\frac{(V \sin \theta)^{2}}{2 g} \end{array} $$ a. Note that the high point of the trajectory occurs at \(\left(0, y_{\max }\right)\) If the projectile is on the ground at \((-a, 0)\) and \((a, 0)\) what is \(a ?\) b. Show that the length of the trajectory (arc length) is $$ 2 \int_{0}^{a} \sqrt{1+k^{2} x^{2}} d x $$ c. Evaluate the arc length integral and express your result in terms of \(V, g,\) and \(\theta\) d. For a fixed value of \(V\) and \(g,\) show that the launch angle \(\theta\) that maximizes the length of the trajectory satisfies \((\sin \theta) \ln (\sec \theta+\tan \theta)=1\) e. Use a graphing utility to approximate the optimal launch angle.
The gamma function is defined by \(\Gamma(p)=\int_{0}^{\infty} x^{p-1} e^{-x} d x,\) for \(p\) not equal to zero or a negative integer. a. Use the reduction formula $$\int_{0}^{\infty} x^{p} e^{-x} d x=p \int_{0}^{\infty} x^{p-1} e^{-x} d x \quad \text { for } p=1,2,3, \ldots$$ to show that \(\Gamma(p+1)=p !(p\) factorial). b. Use the substitution \(x=u^{2}\) and the fact that \(\int_{0}^{\infty} e^{-u^{2}} d u=\frac{\sqrt{\pi}}{2}\) to show that \(\Gamma\left(\frac{1}{2}\right)=\sqrt{\pi}\).
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