Chapter 2: Q18E (page 77)
Differentiate.
\(h\left( w \right) = \left( {{w^2} + 3w} \right)\left( {{w^{ - 1}} - {w^{ - 4}}} \right)\)
Short Answer
Derivative of the function is \(1 + 2{w^{ - 3}} + 9{w^{ - 4}}\)\(\).
Chapter 2: Q18E (page 77)
Differentiate.
\(h\left( w \right) = \left( {{w^2} + 3w} \right)\left( {{w^{ - 1}} - {w^{ - 4}}} \right)\)
Derivative of the function is \(1 + 2{w^{ - 3}} + 9{w^{ - 4}}\)\(\).
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Get started for free34: Verify, by a geometric argument, that the largest possible choice of \(\delta \) for showing that \(\mathop {\lim }\limits_{x \to 3} {x^2} = 9\) is \(\delta = \sqrt {9 + \varepsilon } - 3\).
Describe the intervals on which each function f is continuous.
38: If H is the Heaviside function defined in section 2.2, prove, using Definition 2, that \(\mathop {\lim }\limits_{t \to 0} H\left( t \right)\) does not exist.
(Hint: Use an indirect proof as follows. Suppose that the limit is L. Take \(\varepsilon = \frac{1}{2}\) in the definition of a limit and try to arrive at a contradiction.)
Each limit represents the derivative of some function f at some number a. State such as an f and a in each case.
\(\mathop {{\bf{lim}}}\limits_{h \to {\bf{0}}} \frac{{{\bf{tan}}\left( {\frac{\pi }{{\bf{4}}} + h} \right) - {\bf{1}}}}{h}\)
The gravitational force exerted by the planet Earth on a unit mass at a distance r from the center of the planet is
\(F\left( r \right) = \left\{ {\begin{array}{*{20}{c}}{\frac{{GMr}}{{{R^{\bf{3}}}}}}&{{\bf{if}}\,\,\,r < R}\\{\frac{{GM}}{{{r^{\bf{2}}}}}}&{{\bf{if}}\,\,\,r \ge R}\end{array}} \right.\)
Where M is the mass of Earth, R is its radius, and G is the gravitational constant. Is F a continuous function of r?
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