LECTURE 2
System:
We introduce boundaries in our study called the
system and surroundings.
The boundaries are set up in
a way most conducive to understanding the energetics of what we're studying.
Defining the system and surroundings is arbitrary, but it becomes
important when we consider the exchange of energy between the system and
surroundings.
Two types of exchange can
occur between system and surroundings: (1) energy exchange (heat, work,
friction, radiation, etc.) and (2) matter exchange (movement of molecules
across the boundary of the system and surroundings).
Based on the types of exchange which take place or don't take
place, we will define three types of systems:
control volume is
defined as a volume which encloses the matter and the device inside a control
surface.
Every thing external
to the control volume is the surroundings with the separation given by the
control surface.
The surface may be
open or closed to mass flows and it may have flows from energy in terms of heat
transfer and work across it.
The boundaries may be
moveable or stationary.
In the case of a
control surface that is closed to the mass flow, so that no mass can enter or
escape the control volume, it is called a control
mass containing same amount of matter at all times.
In thermodynamics a
property is any characteristic of a system that is associated with the energy
and can be quantitatively evaluated.
The property of a system should have a definite value when the system is
in a particular state.
Thermodynamic property is a point function.
Properties like
volume of a system that depend on the mass of a system are called extensive
properties.
Properties like
pressure or temperature which do not depend on the system mass are called
intensive properties.
The ratio of extensive
property to the mass of the system are called specific properties and therefore
become intensive properties.
Substance can be
found in three states of physical aggregation namely, solid, liquid and vapor
which are called its phases.
If the system consists
of mixture of different phases, the phases are separated from each other by
phase boundary.
The thermodynamic
properties change abruptly at the phase boundary, even though the intensive
properties like temperature and pressure are identical.
When the property of
a system is defined, it is understood that the system is in equilibrium.
If a system is in
thermal equilibrium, the temperature will be same throughout the system.
If a system is in
mechanical equilibrium, there is no tendency for the pressure to change. In a
single phase system, if the concentration is uniform and there is no tendency
for mass transfer or diffusion, the system is said to be in chemical
equilibrium.
A system which is
simultaneously in thermal, mechanical, and chemical equilibrium is said to be
in thermal equilibrium.
Process
A process is path followed
by a system in reaching a given final state of equilibrium state starting from
a specified initial state.
An actual process occurs only when the equilibrium state does not
exist.
An ideal process can be
defined in which the deviation from thermodynamic equilibrium is infinitesimal.
All the states the system
passes through during a quasi-equilibrium process may be considered equilibrium
states.
For non-equilibrium
processes, we are limited to a description of the system before the process
occurs and after the equilibrium is restored.
Several processes are described by the fact that one property
remains constant.
The prefix iso- is used to describe such processes.
A process is said to be
reversible if both the system and its surroundings can be restored to their
respective initial states by reversing the direction of the process.
Mass---------kg.
Mole------ The mole is the amount of
substance that contains as many atoms (or molecules) as there are atoms in
0.012 kg of carbon-12.
Length—m.
Time:
second
SI unit of temperature is Kelvin (abbreviated
as K). The Kelvin is defined as the fraction of 1/273.16 of the thermodynamic
temperature of the triple point of water. The relation between Kelvin and
Celsius temperature is K = C + 273.15 (The triple point of water is at 0.01 C).
Derived
units: Force: 1 N = 1 kg m/s, pressure 1 Pa = 1 N/m2, 1 bar = 10 Pa,
1 atm. = 101325 Pa. In thermodynamics we are concerned with absolute pressure.
Gauge pressure = absolute pressure – atmospheric pressure. Ordinary vacuum gauge pressure = atmospheric
pressure – absolute pressure.