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 105: 2-108

Answer

a)$P_{p,full-counterweight}=4.71kW$ $P_{p,full-nocounterweight}=9.42kW$ b)$P_{p,empty}=2.94kW$ $P_{p,friction-empty}=3.90kW$

Work Step by Step

Here we are working with potential energy: The potential work is: $W_{p}=mgh$ And the potential power is: $P_{p}=\frac{W_{p}}{t}=\frac{mgh}{t}=mgV$ The potential power at full load is: $P_{p,full-counterweight}=(800-400)kg*9.81\frac{m}{s^2}*1.2\frac{m}{s}=4.71kW$ The potential power with the cabin empty: $P_{p,empty}=(400-150)kg*9.81\frac{m}{s^2}*1.2\frac{m}{s}=2.94kW$ The potential power at full load if no counterweight were used is: $P_{p,full-nocounterweight}=800kg*9.81\frac{m}{s^2}*1.2\frac{m}{s}=9.42kW$ If there were friction the power to overcome the friction will be: $P_{friction}=\frac{F_{f}z}{t}=F_{f}V=800N*1.2\frac{m}{s}=0.96kW$ Then the power required with the cabin empty taking in count friction will be: $P_{p,friction-empty}=P_{p,empty}+P_{friction}=2.94kW+0.96kW=3.90kW$
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