'Exact differentials' presentation slideshows

Chapter 4

Chapter 4. Work and Heat. 4.1 WORK. From a macroscopic point of view, Work is done by a system if the sole effect on the surroundings (everything external to the system) could be the raising of a weight. Work is a form of energy in transit. Work Crossing Boundary of a System.

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SECTION-A(ii)

SECTION-A(ii). Basics of thermodynamics. Syllabus (ME-101-F). Section-A Introduction to machine tools Basic Concepts of thermodynamics Properties of steam & steam generators Section-B Refrigeration & Air conditioning. Hydraulic turbines & pumps. Section-C

628 views • 34 slides

ERT 206/4 THERMODYNAMICS SEM 1 (2012/2013)

ERT 206/4 THERMODYNAMICS SEM 1 (2012/2013). Chapter 12: THERMODYNAMIC PROPERTY RELATIONS. Dr. Hayder Kh. Q. Ali hayderali@unimap.edu.my. Objectives.

485 views • 33 slides

Section 2.9: Quasi-Static Processes

Section 2.9: Quasi-Static Processes. The discussion so far has been general concerning 2 systems A & A ' interacting with each other. Now, consider a Simpler (Ideal) Special Case Definition : Quasi-Static Process.

314 views • 27 slides

Physical Chemistry I

783 views • 24 slides

Thermodynamic Potentials

Thermodynamic Potentials. Why are thermodynamic potentials useful. Consider U=U(T,V). Complete knowledge of equilibrium properties of a simple thermodynamic System requires in addition. P=P(T,V). equation of state. U=U(T,V) and P=P(T,V). complete knowledge of equilibrium properties.

585 views • 22 slides

5.1 Definition of the partial derivative

Chapter 5 Partial differentiation. 5.1 Definition of the partial derivative. the partial derivative of f(x,y) with respect to x and y are. for general n-variable. second partial derivatives of two-variable function f(x,y). Chapter 5 Partial differentiation.

1.7k views • 21 slides

One of the most important examples is to have the system of interest be a gas and to look at the

Section 2.10: Quasi-Static Work Done by Pressure. One of the most important examples is to have the system of interest be a gas and to look at the Quasi-Static Work done by Pressure on the gas.

200 views • 12 slides

0. Essential Background In Thermodynamics

0. Essential Background In Thermodynamics. The First Law The Second Law And The Entropy Thermodynamic Potentials The Third Law. 0.1. The First Law. ? = inexact differential. state variables state space function of state equation of state extensive / intensive variables.

92 views • 9 slides