Sunday, 28 March 2021
Exact Differetial Theorem
Thermodynamics Definitions
System
A system is any region that occupies a volume and has a boundary. The volume outside of this boundary is referred to as the surroundings of the system. The sum of the system and its surroundings is called the universe. Thermodynamics considers systems only at the macroscopic level. Systems can be divided into three general types:
- Isolated System: A system that does not have any mass and energy exchange with the surroundings. An example includes the universe.
- Closed System: This is a system where only energy in the form of heat and work is exchanged with the surroundings. No mass is exchanged.
- Open System: This is a system where both mass and energy is exchanged with the surroundings.
Since the equations available to analyze closed and open systems differ from one another, it is important to properly define a system.
State
Intensive and Extensive Properties
Thermodynamic properties are considered to be either intensive or extensive. A property is considered to be extensive if it is proportional to the mass of the system e.g., volume, kinetic and potential energy. An intensive property is independent of the systems mass e.g., viscosity, density, temperature, pressure, mole fraction and refractive index.
An easy way to visualize this is to divide a system into two equal parts. Each of the part will have the same value of intensive properties (T , P , ρ) as the original system, but will have half the value of the extensive property (V) as shown in the figure below. In short, extensive properties are additive while intensive properties are not.
Specific properties are extensive properties divided by the total mass or total moles of the system, i.e.,
Note: All specific properties are intensive.
The
Degrees of Freedom are the number of
independent intensive variables needed to specify the state of the system. The
Gibbs phase rule specifies the number of degrees of freedom (F) for a system at
equilibrium and is expressed as follows:
P
+ F = C + 2
where
P is the phase number and C is the number of components.
Thus,
is you are working with a single phase, one component system, you need to
specify two independent intensive properties. Two properties are independent if
one property can be varied while the other is constant. For example,
temperature and density are always independent properties and together they can
fix the state of a single-phase, single-component system.
Equations of State
This
can be defined as any mathematical relationship between the variable T, P and V.
Process
Process is a change of state that can occur in numerous ways. Work and heat can only occur during processes and only across the boundary of the system. The curve describing the process is called a process path. If the final state is the same as initial state, then the overall process is called a cyclic process.
State and Path Functions
State
functions are an important thermodynamic concept. If the magnitude of a
thermodynamic property depends only on the initial and final states and is
independent of the path being followed then its known as a state function.
Otherwise, it’s called a path function. All the thermodynamic variables
are state functions except heat and work.
Some
characteristics of state functions are:
- State functions can be solved using integral and differential calculus.
- If a state function φ, undergoes a cyclic process, its initial and final values are the same (Δφ = 0), and this will be true regardless of the path being used to carry out the cyclic process.
- Cannot be solved using integral and differential calculus
- If a path function φ, undergoes a cyclic process, its initial and final values:
(i). will be different (Δφ ≠ 0),
(ii). will depend on the cyclic path being used,
(iii). will be different for every path.
Steady-state
This
means the dependent variable does not change as a function of time. If the
dependent variable is φ, then:
Uniform
This
means the dependent variable is not a function of position. This means that all
three of the partial derivatives with respect to position be zero, i.e.,
The
variation of a physical quantity with respect to its position is called a gradient.
Thus, the gradient of a quantity must be zero for a uniform condition to exist.
Equilibrium
A
system is considered to be at equilibrium if both steady-state and uniform
conditions are met simultaneously. This means that the systems properties like
temperature, density, pressure are constant at all time. Equilibrium has the
following characteristics:
· No
work is done by a system in equilibrium.
· Its state is completely specified when a given number of independent state functions are specified.
Equilibrium
can be classified into 4 classes that can easily be conceptualized using the
analogy of a ball on a solid surface being acted on by gravity.
In
thermodynamics only systems with stable equilibrium states are considered in
their initial and final stable equilibrium states to determine the heat and work
interactions with its surroundings.
Thursday, 25 March 2021
Process Calculations
Describing
Physical Quantities
Units
the
metric and America engineering systems are the most widely used unit systems in
the industrial world. However, a single worldwide unit system was introduced in
order to solve any problems that may arise when products are traded
internationally from one unit system to another. Hence the Systeme
Internatinale d’Units or SI system was formed.
Some
widely used systems are summarized below
System |
Mass |
Length |
Time |
Temperature |
SI |
kg |
m |
s |
Kelvin |
American |
lbm |
ft |
s |
Fahrenheit |
cgs |
g |
cm |
s |
Celcius |
Conversion
Factors
This
is a relationship expressed by an equation where the entries on each side of
the equation are the same quantity but expressed in a different form of units.
for
example: Convert 3 meters to inches.
Moles
This
is the number of molecules in a compound whose mass in grams is numerically
equal to its molecular weight. can be in the form of gram-mol (gmol),
kilogram-mol (kgmol) or pound-mole (lbmol) depending one your preferred unit
system.
Mixture
Composition
it
is important to find the amount of a particular substance in a mixture using
concentration (c) of the substance. The following relationships can help find
the concentration, mass and mole fractions of a substance, A.
The
above equations ca be manipulated to suit the problem being solved. Depending
on what variables are provided, it is easy to solve for unknowns as follows
(where MW stands for molecular weight of a species):
Dimensional
Consistency
1. Terms
that are added or subtracted together MUST have the same units. For example, in
the equation y = mx + b, the units of mx and b must be the same.
2. Exponents
MUST be unitless, therefore an exponent with multiple terms must have those
terms cancel out.
Equations
that correctly describe a physical phenomenon MUST obey the above rules of
dimensional consistency
Exercise
1. Convert
the following
a) an
acceleration of 1 cm/s2 to km/yr2 (Ans: 9.95 * 109
km/yr2)
b) 1
bar into g/cm-s2 (Ans: 106 g/cm-s2)
c) 10,000
g/cm2-s2 into J (Ans: 0.001 J)
2. Calculate the Pressure at the bottom of a swimming pool with a depth of 2 meters.
3. When
a fluid flows from one location to another under certain circumstances, the
changes in fluid properties can be described by Bernoulli equations:
where α: dimensionless correction factor, ρ: fluid density, P:
fluid pressure, v: fluid velocity, z: fluid elevation
Show that this equation is dimensionally consistent in the SI
system.
4. A
gas mixture has the following mass percentage: 70% N2, 14% O2,
4% CO and 12% CO2. What are the mole percentages of the gases in the
mixture? what is the average molecular weight of the mixture? (MW for N2 =
28g/mol, O2 = 32 g/mol, CO = 28 g/mol and CO2 = 44
g/mol).
Assume
a mass basis of 100 g for the total mixture
components |
mass
fraction |
mass
(g) |
MW
(g/mol) |
Moles |
Mole
fraction |
Mole Percent |
N2 |
0.70 |
70 |
28 |
2.500 |
0.745 |
74.5 |
O2 |
0.14 |
14 |
32 |
0.432 |
0.131 |
13.1 |
CO |
0.04 |
4 |
28 |
0.143 |
0.043 |
4.3 |
CO2 |
0.12 |
12 |
44 |
0.273 |
0.081 |
8.1 |
Total |
1.00 |
100 |
|
3.354 |
1.00 |
100 |
Average
molecular weight
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