Pure Substances Thermodynamics Professor Lee Carkner Lecture 5
PAL # 4 First Law Pumping water uphill and then running it back to produce energy Rate of power imparted to water = W’ water = (1000)(2)(9.8)(40) = But the pump and the turbine are only 75% efficient pump = W’ water /W’ pump W’ pump = 785/0.75 = Cost per year = (1046)(10)(0.03)(365) = $ turbine = W’ turbine /W’ water W’ turbine = (785)(0.75) = Revenue per year = (785)(10)(0.08)(365) = $ Net Yearly Profit =
PAL # 4 First Law Should you build it? No
Pure Substances A pure substance consists of either a single type of atom or molecule or a homogeneous mixture Can exist as a mixture of phases Gas Liquid Solid Strong intermolecular forces, high density, fixed molecular position
Types of Phases Compressed liquid Saturated liquid Saturated Vapor Saturated liquid and vapor can coexist together Superheated vapor
Saturation A substance changes phase when it is at the saturation temperature for a given pressure Can be compiled in tables for reference T sat increases with P sat Need more internal energy to become vapor at higher pressure
Change of T sat with P sat
Enthalpy Defined as: h = u + Pv H = U +PV Very useful for flow systems such as turbines
Specific Volume and Quality Mass of saturated liquid = m f Mass of saturated vapor = m g Since both phases often co-exist we define the quality, x: The quality is the relative fraction of the mixture in the vapor phase
Quality Relations The total volume of a mixture is: the volume occupied by each phase is: We can use these relationships to write an expression for the combined specific volume of the mixture: v avg = v f +xv fg x = (v avg –v f )/v fg
Property Diagrams We will plot three key variables P, T, and v as: Each region of the diagram represents a phase or mixture of phases
Pv Diagram
Pv Diagram Properties Saturation curves define boundaries of liquid- vapor mixture region Critical point is on the critical isotherm Densities of both are the same Above the critical point, no amount of pressure can condense the vapor to a liquid
Regions on a Pv Diagram
PT Diagram Three curves can be drawn on the PT diagram Fusion curve Vaporization curve Sublimation curve The curves bound three distinct regions, one for each phase Juncture of the three curves is the triple point where all three coexist
PT Diagram
Other PT Features An isobar at standard atmospheric pressure intersects the normal boiling and melting points The critical point is on the vaporization curve Gas above critical T is called “gas”, below it is called “vapor”
PvT Diagram for Water
PVT Diagram P, V and T relations can be formed to create a three dimensional diagram The PT and PV diagrams are formed by projection
Next Time Read: Homework: Ch 3, P: 48, 54, 75, 86