Calculus (3rd Edition)

Published by W. H. Freeman
ISBN 10: 1464125260
ISBN 13: 978-1-46412-526-3

Chapter 3 - Differentiation - 3.7 The Chain Rule - Exercises - Page 147: 94

Answer

$\dfrac{dR}{dt}=0.257023221$ The unit of the derivative is joules per square meter per second per kelvin.

Work Step by Step

The Stefan–Boltzmann Law gives $R = σT^4$. To find $\dfrac{dR}{dt}$ use chain rule. That is, $\dfrac{dR}{dt}=\dfrac{dR}{dT}\times\dfrac{dT}{dt}$ Now, to find $\dfrac{dR}{dT}$. Derivate $R = σT^4$ with respect to temperature $T$. We get, $\dfrac{dR}{dT}=\dfrac{d}{dT}(σT^4)$ Now, use the power rule to solve further. $\dfrac{dR}{dT}=4σT^3$ Now substitute $\dfrac{dR}{dT}=4σT^3$ and $\dfrac{dT}{dt}= 0.05 K/year$ in $\dfrac{dR}{dt}=\dfrac{dR}{dT}\times\dfrac{dT}{dt}$. $\dfrac{dR}{dt}=4\sigma T^{3}\times 0.05$ Substitute $\sigma = 5.67 ×10^{−8} Js^{−1}m^{−2}K^{−4}$ and $T = 283$ We get, $\dfrac{dR}{dt}=4\times5.67 ×10^{−8}\times283^{3}\times0.05=0.257023221$ Since the unit of $R$ is in joules per square meter per second and the unit of $T$ is in kelvins. The unit of the derivative is the quotient of the units of $R$ and $T$. That is, joules per square meter per second per kelvin.
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