Fundamentals of Physics Extended (10th Edition)

Published by Wiley
ISBN 10: 1-11823-072-8
ISBN 13: 978-1-11823-072-5

Chapter 43 - Energy from the Nucleus - Problems - Page 1333: 47c

Answer

$t=1.46 \times 10^3 \mathrm{y} $

Work Step by Step

If the Sun were composed of the appropriate mixture of carbon and oxygen, the number of combustion events that could occur before the Sun burns out would be $ \left(2.0 \times 10^{30} \mathrm{~kg}\right) /\left(7.31 \times 10^{-26} \mathrm{~kg}\right)=2.74 \times 10^{55} . $ The total energy released would be $ E=\left(2.74 \times 10^{55}\right)\left(6.58 \times 10^{-19} \mathrm{~J}\right)=1.80 \times 10^{37} \mathrm{~J} . $ If $P$ is the power output of the Sun, the burn time would be $ t=\frac{E}{P}=\frac{1.80 \times 10^{37} \mathrm{~J}}{3.9 \times 10^{26} \mathrm{~W}}=4.62 \times 10^{10} \mathrm{~s}=1.46 \times 10^3 \mathrm{y}, $ or $1.5 \times 10^3 \mathrm{y}$, to two significant figures.
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