Question Number 43145 by rahul 19 last updated on 07/Sep/18 | ||
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$$\int_{\mathrm{0}} ^{\infty} \:\left[\:\mathrm{2e}^{−{x}} \right]{dx}\:=\:?\: \\ $$ $${where}\:\left[.\right]=\:{gif}. \\ $$ | ||
Commented bymaxmathsup by imad last updated on 07/Sep/18 | ||
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$${changement}\:\mathrm{2}\:{e}^{−{x}} \:={t}\:{give}\:{e}^{−{x}} =\frac{{t}}{\mathrm{2}}\:\Rightarrow−{x}={ln}\left(\frac{{t}}{\mathrm{2}}\right)\:\Rightarrow{x}=−{ln}\left(\frac{{t}}{\mathrm{2}}\right)\:{and} \\ $$ $${I}\:=\:\int_{\mathrm{0}} ^{\infty} \:\:\left[\:\mathrm{2}\:{e}^{−{x}} \right]{dx}\:=−\int_{\mathrm{0}} ^{\mathrm{2}} \:\left[{t}\right]\left(−\frac{\mathrm{1}}{{t}}\right){dt}\:=\:\int_{\mathrm{0}} ^{\mathrm{2}} \:\:\frac{\left[{t}\right]}{{t}}{dt} \\ $$ $$=\:\int_{\mathrm{0}} ^{\mathrm{1}} \:\frac{\mathrm{0}}{{t}}{dt}\:+\int_{\mathrm{1}} ^{\mathrm{2}} \:\frac{\mathrm{1}}{{t}}{dt}\:=\:\left[{ln}\mid{t}\mid\right]_{\mathrm{1}} ^{\mathrm{2}} \:\:={ln}\left(\mathrm{2}\right)\:. \\ $$ | ||
Commented bytanmay.chaudhury50@gmail.com last updated on 07/Sep/18 | ||
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Commented byrahul 19 last updated on 08/Sep/18 | ||
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$$\mathrm{thanks}\:\mathrm{prof}\:\mathrm{abdo}. \\ $$ | ||
Commented bymath khazana by abdo last updated on 08/Sep/18 | ||
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$${look}\:{sir}\:{raul}\:{x}=−{ln}\left({t}\right)+{ln}\left(\mathrm{2}\right)\:\Rightarrow{dx}\:=−\frac{{dt}}{{t}} \\ $$ | ||
Answered by tanmay.chaudhury50@gmail.com last updated on 07/Sep/18 | ||
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$$\int_{\mathrm{0}} ^{\mathrm{0}.\mathrm{7}} \left[\mathrm{2}{e}^{−{x}} \right]{dx}+\int_{\mathrm{0}.\mathrm{7}} ^{\infty} \left[\mathrm{2}{e}^{−{x}} \right]{dx} \\ $$ $$=\int_{\mathrm{0}} ^{\mathrm{0}.\mathrm{7}} \mathrm{1}×{dx}+\int_{\mathrm{0}.\mathrm{7}} ^{\infty} \mathrm{0}×{dx} \\ $$ $$=\mathrm{0}.\mathrm{7} \\ $$ $${ln}\mathrm{2}\approx\mathrm{0}.\mathrm{7} \\ $$ | ||
Commented bytanmay.chaudhury50@gmail.com last updated on 07/Sep/18 | ||
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Commented byrahul 19 last updated on 08/Sep/18 | ||
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$$\mathrm{thanks}\:\mathrm{sir}. \\ $$ | ||
Commented byabdo.msup.com last updated on 08/Sep/18 | ||
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$${nevermind}\:{sir}... \\ $$ | ||