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The work produced by a constant temperature, prpessure-volume thermodynamic process can be computed as: W = f pdV, where W is work, p is pressure, and Vis volume. Using a combination of the trapezoidal rule, Simpson's 1/3 rule, and Simpson's 3/8 rule, use the following data to compute the work in kJ (kJ = kN.m): Pressure (kPa) 336 294.4 266.4 260.8 260.5 249.6 193.6 165.6 Volume (m³) 0.5 2 3 4 6 8 10 11

The work produced by a constant temperature, prpessure-volume thermodynamic process can be computed as: W = f pdV, where W is work, p is pressure, and Vis volume. Using a combination of the trapezoidal rule, Simpson's 1/3 rule, and Simpson's 3/8 rule, use the following data to compute the work in kJ (kJ = kN.m): Pressure (kPa) 336 294.4 266.4 260.8 260.5 249.6 193.6 165.6 Volume (m³) 0.5 2 3 4 6 8 10 11

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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The work produced by a constant temperature, prpessure-volume thermodynamic process can be computed as: W = S p dV, where W is work, p is pressure, and V is volume. Using a combination of the trapezoidal rule, Simpson's 1/3 rule, and Simpson's 3/8 rule, use the following data to compute the work in kJ (kJ = kN.m): Pressure (kPa) 336 294.4 266.4 260.8 260.5 249.6 193.6 165.6 Volume (m) 0.5 2 3 4 6 10 11
Transcribed Image Text:The work produced by a constant temperature, prpessure-volume thermodynamic process can be computed as: W = S p dV, where W is work, p is pressure, and V is volume. Using a combination of the trapezoidal rule, Simpson's 1/3 rule, and Simpson's 3/8 rule, use the following data to compute the work in kJ (kJ = kN.m): Pressure (kPa) 336 294.4 266.4 260.8 260.5 249.6 193.6 165.6 Volume (m) 0.5 2 3 4 6 10 11
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