ciascuno dei volumi richiesti è dato da un integrale definito del tipo \(\pi \int\limits_{a}^{b}{{{\left( f\left( x \right) \right)}^{2}}dx}\): \[\text{1) }V=\pi \int\limits_{0}^{1}{\frac{{{x}^{2}}}{{{\left( 2-x \right)}^{2}}}dx}=\pi \int\limits_{1}^{2}{\frac{{{\left( 2-t \right)}^{2}}}{{{t}^{2}}}dt}=\pi \left[ -\frac{4}{t}+t-4\ln t \right]_{1}^{2}=\pi \left( 3-4\ln 2 \right)\quad .\] \[\text{2) }V=\pi \int\limits_{0}^{\pi /4}{\frac{1}{{{\cos }^{2}}x}dx}=\pi \left[ \tan x \right]_{0}^{\pi /4}=\pi \quad .\]\[\text{3) }V=\pi \int\limits_{-5}^{-4}{\frac{x+4}{x}dx}=\pi \left[ x+4\ln \left| x \right|
\right]_{-5}^{-4}=\pi \left( 1-4\ln \frac{5}{4} \right)\quad .\]\[\text{4) }V=\pi \int\limits_{0}^{1}{{{e}^{3x}}dx}=\pi \left[ \frac{{{e}^{3x}}}{3} \right]_{0}^{1}=\frac{\pi }{3}\left( {{e}^{3}}-1 \right)\quad .\]
Massimo Bergamini
