Thermodynamics: An Engineering Approach 8th Edition

Published by McGraw-Hill Education
ISBN 10: 0-07339-817-9
ISBN 13: 978-0-07339-817-4

Chapter 2 - Energy, Energy Transfer, and General Energy Analysis - Problems - Page 99: 2-36

Answer

a) $P=47.01kW$ b) $P=90.14kW$ c) $P=-10.49kW$

Work Step by Step

$h=100m*sin(30^{\circ})=50m$ The work of climb is: $W_{p}=mg\Delta z=1150kg*9.81\frac{m}{s^2}*50m=564.08kJ$ And the power of climb is: $P_{p}=\frac{W_{p}}{t}=\frac{564.08kJ}{12s}=47.01kW$ a) In this case, since velocity is constant the power needed is only the one to climb the uphill road: $P_{t,a}=P_{p}=47.01kW$ b) In this case, the power needed is the sum of the one to climb the uphill road and the one to increase the velocity: $W_{k,b}=\frac{1}{2}m\Delta v^2=\frac{1}{2}*1150kg*((30\frac{m}{s})^2-(0\frac{m}{s})^2)=517.5kJ$ $P_{k,b}=\frac{W_{k,b}}{t}=\frac{517.5kJ}{12s}=43.13kW$ Then the total power needed is: $P_{t,b}=P_{k,b}+P_{p}=43.13kW+47.01kW=90.14kW$ c) In this case, the power needed is the sum of the one to climb the uphill road and the one to reduce the velocity: $W_{k,c}=\frac{1}{2}m\Delta v^2=\frac{1}{2}*1150kg*((5\frac{m}{s})^2-(35\frac{m}{s})^2)=-690kJ$ $P_{k,c}=\frac{W_{k,c}}{t}=\frac{-690kJ}{12s}=-57.5kW$ Then the total power needed is: $P_{t,c}=P_{k,c}+P_{p}=-57.5kW+47.01kW=-10.49kW$
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