Calculus: Early Transcendentals 8th Edition

Published by Cengage Learning
ISBN 10: 1285741552
ISBN 13: 978-1-28574-155-0

Chapter 7 - Section 7.1 - Integration by Parts - 7.1 Exercises - Page 478: 68

Answer

The height of the rocket after one minute is 512375.89 m

Work Step by Step

The height of the rocket as a function of time is just the integral of the velocity function so, we integrate the velocity given $$v(t)=-gt- v_{e}ln{ \frac {m-rt}{m}}$$ The height is $$h(t)= \int{v(t)} dt=\int{-gt- v_{e}ln{ \frac {m-rt}{m}}dt}$$ $$h(t)= \int{v(t)} dt=-\int{gt}dt-\int{ v_{e}ln{ \frac {m-rt}{m}dt}}$$ the first integral is easy it's just $$\int{gt} dt =\frac{1}{2}gt^{2}+c_{1}$$ The second integral could be easier with changing variables $$y= \frac {m-rt}{m}$$ thus $$dy=-\frac {r}{m}dt$$ or $$dt=-\frac {m}{r}dy$$ then the second integral becomes $$-\frac {m}{r} \int\ln{y} dy$$ which can be solved by integration by parts $$u=\ln{y}$$ and $$dk=dy$$ then applying the integration by part formula $$A=uk−∫kdu$$ the second integral is $$A=y\ln{y} -\int{dy} = y\ln{y}-y +C_{2}$$ So the height function is $$h(t)=-\frac{1}{2}gt^{2}-v_{e}\frac {m}{r}( y\ln{y}-y)+C_{1}+C_{2}$$ Changing the new variable back and defining $$C=C_{1}+C_{2}$$ $$h(t)=-\frac{1}{2}gt^{2}-v_{e}\frac {m}{r}( \frac {m-rt}{m}(\ln{(\frac {m-rt}{m})}-1))+C$$ which equal $$h(t)=-\frac{1}{2}gt^{2}-v_{e} \frac {m-rt}{r}(\ln{(\frac {m-rt}{m})}-1)+C$$ since the rocket start the motion at t=0 from the ground then h(0)=0 and $$h(0)=v_{e} \frac {m}{r}(\ln({1})-1)+C=-v_{e} \frac {m}{r}C=0$$ then C=0 and the height function becomes $$h(t)=-\frac{1}{2}gt^{2}-v_{e} \frac {m-rt}{r}(\ln{(\frac {m-rt}{m})}-1)$$ Now we find the height after one minute using the constants given in the problem $$ g=9.8 m/s^{2} ,m=30000 kg , r=160 kg/s ,v_{e}=3000 m/s$$ and $t=60 s$ $h(60)= -\frac{1}{2}9.8*60^{2}-3000 \frac {30000-160*60}{160}(\ln{(\frac {30000-160*60}{30000})}-1)=512375.89 m$
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