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The van der Waals equation of state for a real gas is n?a V – nb = nRT In this equation, the van der Waals constant, a, represents a correction for O a positive deviation in the measured value of P from that for an ideal gas due to the finite mass of the molecules of a real gas. O a positive deviation in the measured value of P from that for an ideal gas due to the finite volume of space occupied by molecules of a real gas. O a negative deviation in the measured value of P from that for an ideal gas due to the finite volume of space occupied by molecules of a real gas. O a negative deviation in the measured value of P from that for an ideal gas due to the attractive forces between the molecules of a real gas. O a positive deviation in the measured value of P from that for an ideal gas due to the attractive forces between the molecules of a real gas. uthool O HModio

The van der Waals equation of state for a real gas is n?a V – nb = nRT In this equation, the van der Waals constant, a, represents a correction for O a positive deviation in the measured value of P from that for an ideal gas due to the finite mass of the molecules of a real gas. O a positive deviation in the measured value of P from that for an ideal gas due to the finite volume of space occupied by molecules of a real gas. O a negative deviation in the measured value of P from that for an ideal gas due to the finite volume of space occupied by molecules of a real gas. O a negative deviation in the measured value of P from that for an ideal gas due to the attractive forces between the molecules of a real gas. O a positive deviation in the measured value of P from that for an ideal gas due to the attractive forces between the molecules of a real gas. uthool O HModio

General Chemistry - Standalone book (MindTap Course List)
General Chemistry - Standalone book (MindTap Course List)
11th Edition
ISBN:9781305580343
Author:Steven D. Gammon, Ebbing, Darrell Ebbing, Steven D., Darrell; Gammon, Darrell Ebbing; Steven D. Gammon, Darrell D.; Gammon, Ebbing; Steven D. Gammon; Darrell
Publisher:Steven D. Gammon, Ebbing, Darrell Ebbing, Steven D., Darrell; Gammon, Darrell Ebbing; Steven D. Gammon, Darrell D.; Gammon, Ebbing; Steven D. Gammon; Darrell
Chapter5: The Gaseous State
Section: Chapter Questions
Problem 5.127QP: A 1.000-g sample of an unknown gas at 0C gives the following data: P(atm) V (L) 0.2500 3.1908 0.5000...
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The van der Waals equation of state for a real gas is n²a' V - nb = nRT In this equation, the van der Waals constant, a, represents a correction for O a positive deviation in the measured value of P from that for an ideal gas due to the finite mass of the molecules of a real gas. O a positive deviation in the measured value of P from that for an ideal gas due to the finite volume of space occupied by molecules of a real gas. O a negative deviation in the measured value of P from that for an ideal gas due to the finite volume of space occupied by molecules of a real gas. O a negative deviation in the measured value of P from that for an ideal gas due to the attractive forces between the molecules of a real gas. O a positive deviation in the measured value of P from that for an ideal gas due to the attractive forces between the molecules of a real gas. Tovth aak dModio
Transcribed Image Text:The van der Waals equation of state for a real gas is n²a' V - nb = nRT In this equation, the van der Waals constant, a, represents a correction for O a positive deviation in the measured value of P from that for an ideal gas due to the finite mass of the molecules of a real gas. O a positive deviation in the measured value of P from that for an ideal gas due to the finite volume of space occupied by molecules of a real gas. O a negative deviation in the measured value of P from that for an ideal gas due to the finite volume of space occupied by molecules of a real gas. O a negative deviation in the measured value of P from that for an ideal gas due to the attractive forces between the molecules of a real gas. O a positive deviation in the measured value of P from that for an ideal gas due to the attractive forces between the molecules of a real gas. Tovth aak dModio
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