Chapter 7: Problem 31
Find the general solution of the following equations. $$\frac{d y}{d t}=\frac{3 t^{2}}{y}$$
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Chapter 7: Problem 31
Find the general solution of the following equations. $$\frac{d y}{d t}=\frac{3 t^{2}}{y}$$
These are the key concepts you need to understand to accurately answer the question.
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Apply Simpson's Rule to the following integrals. It is easiest to obtain the Simpson's Rule approximations from the Trapezoid Rule approximations, as in Example \(7 .\) Make \(a\) table similar to Table 7.8 showing the approximations and errors for \(n=4,8,16,\) and \(32 .\) The exact values of the integrals are given for computing the error. \(\int_{0}^{\pi} e^{-t} \sin t d t=\frac{1}{2}\left(e^{-\pi}+1\right)\)
Given a Midpoint Rule approximation \(M(n)\) and a Trapezoid Rule approximation \(T(n)\) for a continuous function on \([a, b]\) with \(n\) subintervals, show that \(T(2 n)=(T(n)+M(n)) / 2\).
Bob and Bruce bake bagels (shaped like tori). They both make bagels that have an inner radius of 0.5 in and an outer radius of 2.5 in. Bob plans to increase the volume of his bagels by decreasing the inner radius by \(20 \%\) (leaving the outer radius unchanged). Bruce plans to increase the volume of his bagels by increasing the outer radius by \(20 \%\) (leaving the inner radius unchanged). Whose new bagels will have the greater volume? Does this result depend on the size of the original bagels? Explain.
Sociologists model thespread of rumors using logistic equations. The key
assumption is that at any given time, a fraction \(y\) of the population, where
\(0 \leq y \leq 1,\) knows the rumor, while the remaining fraction \(1-y\) does
not. Furthermore, the rumor spreads by interactions between those who know the
rumor and those who do not. The number of such interactions is proportional to
\(y(1-y) .\) Therefore, the equation that models the spread of the rumor is
\(y^{\prime}(t)=k y(1-y)\), where \(k\) is a positive real number. The fraction of
people who initially know the rumor is \(y(0)=y_{0},\) where \(0
The nucleus of an atom is positively charged because it consists of positively charged protons and uncharged neutrons. To bring a free proton toward a nucleus, a repulsive force \(F(r)=k q Q / r^{2}\) must be overcome, where \(q=1.6 \times 10^{-19} \mathrm{C}\) (coulombs) is the charge on the proton, \(k=9 \times 10^{9} \mathrm{N}-\mathrm{m}^{2} / \mathrm{C}^{2}, Q\) is the charge on the nucleus, and \(r\) is the distance between the center of the nucleus and the proton. Find the work required to bring a free proton (assumed to be a point mass) from a large distance \((r \rightarrow \infty)\) to the edge of a nucleus that has a charge \(Q=50 q\) and a radius of \(6 \times 10^{-11} \mathrm{m}\)
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