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Saturated steam at 99.63°C condenses on the outside of a 5-m long, 6- cm-diameter thin horizontal copper tube by cooling liquid water whose density is 997 kg/m3 that enters the tube at 20°C at an average velocity of 4 m/s and leaves at 50°C. Liquid water density is 997 kg/m2, cp of iquid water is 4.18 kJ/kg°C. The rate of heat transfer to water in kW is O 314.22 O 3,142.2 O 1,413.99 O 1,767.49

Saturated steam at 99.63°C condenses on the outside of a 5-m long, 6- cm-diameter thin horizontal copper tube by cooling liquid water whose density is 997 kg/m3 that enters the tube at 20°C at an average velocity of 4 m/s and leaves at 50°C. Liquid water density is 997 kg/m2, cp of iquid water is 4.18 kJ/kg°C. The rate of heat transfer to water in kW is O 314.22 O 3,142.2 O 1,413.99 O 1,767.49

Introduction to Chemical Engineering Thermodynamics
Introduction to Chemical Engineering Thermodynamics
8th Edition
ISBN:9781259696527
Author:J.M. Smith Termodinamica en ingenieria quimica, Hendrick C Van Ness, Michael Abbott, Mark Swihart
Publisher:J.M. Smith Termodinamica en ingenieria quimica, Hendrick C Van Ness, Michael Abbott, Mark Swihart
Chapter1: Introduction
Section: Chapter Questions
Problem 1.1P
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Condensing steam Q This situation pertains to the transfer of heat from higher T (steam) to lower T (cooling liquid water). The heat transfer phenomena causes the increase of temperature of the cooling liquid water. We can also clearly see that thermodynamic property can also be divided by time that gives rise to what we call rate. Saturated steam at 99.63°C condenses on the outside of a 5-m long, 6- cm-diameter thin horizontal copper tube by cooling liquid water whose density is 997 kg/m° that enters the tube at 20°C at an average velocity of 4 m/s and leaves at 50°C. Liquid water density is 997 kg/m3, cp of liquid water is 4.18 kJ/kg®C. The rate of heat transfer to water in kW is O 314.22 O 3,142.2 O 1,413.99 O 1,767.49
Transcribed Image Text:Condensing steam Q This situation pertains to the transfer of heat from higher T (steam) to lower T (cooling liquid water). The heat transfer phenomena causes the increase of temperature of the cooling liquid water. We can also clearly see that thermodynamic property can also be divided by time that gives rise to what we call rate. Saturated steam at 99.63°C condenses on the outside of a 5-m long, 6- cm-diameter thin horizontal copper tube by cooling liquid water whose density is 997 kg/m° that enters the tube at 20°C at an average velocity of 4 m/s and leaves at 50°C. Liquid water density is 997 kg/m3, cp of liquid water is 4.18 kJ/kg®C. The rate of heat transfer to water in kW is O 314.22 O 3,142.2 O 1,413.99 O 1,767.49
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