Title: GAS TRANSFER
1GAS TRANSFER
2DEFINITION AND TERMS
- Gas transfer ? a physical phenomenon, by which
gas molecules are exchanged between a liquid and
a gas at a gas-liquid interface ? - (1) an increase of the concentration of the
gas(es) in the liquid phase as long as this phase
is not saturated with the gas under the given
conditions of e.g. pressure, temperature
(absorption of gas) - (2) a decrease when the liquid phase is over
saturated (desorption, precipitation or stripping
of gas)
3DEFINITION AND TERMS
- Important natural phenomena of gas transfer ? the
reaeration of surface water - (1) the transfer of oxygen into surface water
- (2) release of oxygen produced by algal
activities up to a concentration above the
saturation concentration - (3) release of taste and odor-producing
substances - (4) release of methane, hydrogen sulfide under
anaerobic conditions of surface water or of the
bottom deposits
4ELEMENTS OF AERATION AND GAS TRANSFER OPERATIONS
- Gas transfer occurs only through the gas-liquid
interface ? has to be carried out as to maximize
the opportunity of interfacial contact between
the two phases. - The engineering goal ? to accomplish the gas
transfer with a minimum expenditure of initial
and operational cost (energy).
5ELEMENTS OF AERATION AND GAS TRANSFER OPERATIONS
- Four different types of aerators
- Gravity aerators
- (a) cascades ? the available difference head is
subdivided into several steps - (b) inclined planes ? eqipped with riffle plates
to break up the sheet of water for surface
renewal - (c) vertical stacks ? droplets fall and updrafts
of air ascend in counter current flow
6ELEMENTS -- CASCADES
7ELEMENTS INCLINED PLANES
8ELEMENTS VERTICAL STACKS
9ELEMENTS VERTICAL STACKS
10ELEMENTS VERTICAL STACKS
11ELEMENTS AMMONIA STRIPPING
12ELEMENTS OF AERATION AND GAS TRANSFER OPERATIONS
- (2) Spray aerators
- ? the water is sprayed in the form of fine
droplets into the air ? creating a large
gas-liquid interface for gas transfer
13ELEMENTS SPRAY AERATORS
14ELEMENTS OF AERATION AND GAS TRANSFER OPERATIONS
- (3) Air diffusers (bubble aeration)
- ? air is injected into water
- (a) through orifices or nozzles in the air
piping system - (b) through spargers
- (c) through porous tubes, plates, boxes or domes
- ? to produce bubbles of various size with
different interfacial areas per m3 of air.
15ELEMENTS AIR DIFFUSERS
16ELEMENTS AIR DIFFUSERS (POROUS TUBES)
17ELEMENTS AIR DIFFUSERS
18ELEMENTS AIR DIFFUSERS
19ELEMENTS AIR DIFFUSERS
20ELEMENTS OF AERATION AND GAS TRANSFER OPERATIONS
- (4) Mechanical aerators
- ? create new gas-liquid interfaces by different
means and constructions ? two types of
construction - (a) various construction of brushes ? a
horizontal revolving shaft with combs, blades or
angles - (b) turbine or cone aerators with vertical shaft
21Boyles Law
22Charles Law
23Gay-Lussacs Law
24Ideal Gas Law
The ideal gas law is a special form of an
equation of state, i.e., an equation relating the
variables that characterize a gas (pressure,
volume, temperature, density, .). The ideal gas
law is applicable to low-density gases.
25Absolute Zero and the Kelvin Scale
The pressure-temperature relation leads to the
design of a constant-volume gas thermometer.
Extrapolation of measurements made using
different gases leads to the concept of absolute
zero, when the pressure (or volume) is zero.
26Kinetic Theory Applications
- Kinetic theory investigates (on a molecular
scale) topics such as - Change of phase (evaporation vapour pressure
latent heat) - Pressure
- Change of shape and volume (elasticity Hooke's
law) - Transport phenomena (diffusion - transport of
mass viscosity - transport of momentum
electrical conduction - transport of electric
charge thermal conduction - transport of heat) - Thermal expansion
- Surface energy and surface tension
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28Kinetic Theory of Gases Basic Assumptions
- The number of molecules is large, and the average
separation between them is large compared with
their dimensions. This means that the molecules
occupy a negligible volume in the container. - The molecules obey Newton's laws of motion, but
as a whole they move randomly. 'Randomly' means
that any molecule can move equally in any
direction. - The molecules undergo elastic collisions with
each other and with the walls of the container.
Thus, in the collisions both kinetic energy and
momentum are constant. - The forces between molecules are negligible
except during a collision. The forces between a
molecule are short-range, so the molecules
interact with each other only during a collision. - The gas is a pure substance. All molecules are
identical.
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31SOLUBILITY OF GASES
- The solubility of gases in water (and also in
other liquids) depends upon - (1) the nature of the gas generally expressed by
a gas specific coefficient ? the distribution
coefficient, kD - (2) the concentration of the respective gas in
the gaseous phase ? related to the partial
pressure of the respective gas in the gas phase - (3) the temperature of the water
- (4) impurities contained in the water
32INFLUENCE OF THE GAS CONCENTRATION ON SOLUBILITY
- The higher the gas concentration in the gaseous
phase ? the greater will be the saturation
concentration in the liquid phase - The relation between the saturation concentration
cs (g/m3) and the gas concentration in the gas
phase cg (g/m3) - cs kD . cg
33INFLUENCE OF THE GAS CONCENTRATION ON SOLUBILITY
- The molar gas concentration in the gas phase
(according to the universal gas law) - (n/V) p / (RT) (moles/m3)
- Hence the corresponding mass concentration cg is
obtained by multiplication with the molecular
weight (MW) of the gas - cg (p . MW)/ (RT) (g/m3)
34INFLUENCE OF THE GAS CONCENTRATION ON SOLUBILITY
- The combination yields
- cs (kD . MW . p)/ (RT)
- Henrys law is generally written as
- cs kH . p
- The relation between distribution coefficient kD
and Henrys constant - kH (kD . MW)/ (RT)
35INFLUENCE OF THE GAS CONCENTRATION ON SOLUBILITY
- Bunsen absorption coefficient, kb ? how much gas
volume (m3), reduced to standard temperature
(0oC) and pressure (101,3 kPa), can be absorbed
per unit volume (m3) of water at a partial
pressure of pO 101,3 kPa of the gas in the gas
phase - cs (m3 STP gas/m3 water) kb
36INFLUENCE OF THE GAS CONCENTRATION ON SOLUBILITY
- And any other partial pressure p
- cs kb . (p/p0) (m3STP/m3)
- Since 1 m3STP contains p0/R.T0 moles of gas and a
mass of gas equal to MW. p0/R.T0 - cs (kb . MW)/(R.T0 ) p (g/m3)
-
37INFLUENCE OF THE GAS CONCENTRATION ON SOLUBILITY
- The relation between kD and kb
- kb kD T0/T
- The interrelationship between the three
coefficients - kD kH .R.T/MW kb .T/T0
38INFLUENCE OF THE GAS CONCENTRATION ON SOLUBILITY
- In the practice of aeration the gas phase will
always be saturated with water vapor exerting a
certain partial pressure pw ? the partial
pressure p of the other gases are reduced ? - p p . (P pw)/P
39INFLUENCE OF TEMPERATURE ON SOLUBILITY
- Gases dissolved in water ? accompanied by
liberation of heat ?H - Le Chatelier principle ? increase of temperature
results in a decrease of solubility ? vant
Hoffs equation - d(ln kD)/dT ?H/(RT2)
- where R universal gas constant
- T absolute temperature K
- ?H change of heat content
accompanying by the absorp- tion of 1 mole
of gas (J/mole)
40INFLUENCE OF TEMPERATURE ON SOLUBILITY
- By integrating between the limits T1 and T2
- ln(kD)2/(kD)1 (?H/R)(T2-T1)/(T1.T2)
- The product T1 .T2 does not change significantly
within the temperature range encountered in gas
transfer operations - (kD)2 (kD)1. econst (T2 T1)
41INFLUENCE OF IMPURITIES ON SOLUBILITY
- Other constituent that may be contained in water
influence the solubility of gases ? expressed by
an activity coefficient ? - cs (kD/?).cg
- For pure water ? 1
- ? ? generally increases as the concentration of
substances dissolved in water rises ? lowering
the solubility
42INFLUENCE OF IMPURITIES ON SOLUBILITY
- The influence of concentration of impurities cimp
on the activity coefficient - for non-electrolytes
- log ? f . Cimp
- for electrolytes
- log ? f . I
- where f a constant depending on the matter
dissolved in water - I ionic strength of electrolyte
43DIFFUSION
- The phenomenon of diffusion ? the tendency any
substance the spread uniformly throughout the
space available to it ? in environmental
engineering ? diffusion phenomena the liquid
phase in gas transfer operations
44DIFFUSION
- For a quiescent body of water of unlimited depth
contacting the gas by an area of A ? the rate of
mass transfer dM/dt as a consequence of diffusion
of the gas molecules in the liquid phase ? Ficks
Law - (dM/dt) -D.A (dc/dx) (g/s)
- where
- D coefficient of molecular diffusion (m2/s)
- x the distance from the interfacial area A
- dx/dt concentration gradient
45DIFFUSION
46DIFFUSION
47DIFFUSION
48DIFFUSION
- The total amount of gas M (g) that has been
absorbed through the surface area A during the
time t ? independent of x ? -
- under conditions of unlimited depth of water body
49DIFFUSION
- If the depth is not too small ? the time of
diffusion is not too long ? diffusion is very
slow process and only very little gas is brought
into deeper layers of the water body
50THE CONCEPT OF GAS TRANSFER COEFFICIENTS
51THE CONCEPT OF GAS TRANSFER COEFFICIENTS
- In accordance with Ficks Law ? the mass
transport per unit time (g/s) is proportional to
the concentration difference - for the gas phase
- for the liquid phase
52THE CONCEPT OF GAS TRANSFER COEFFICIENTS
- where
- kg partial gas transfer coefficient for
the gas phase - kL partial gas transfer coefficient for
the liquid phase - cgi and cLi ? generally not known ?
- cLi kD . cgi
- ?
53THE CONCEPT OF GAS TRANSFER COEFFICIENTS
- The total gas transfer coefficient KL is composed
of both the partial coefficients and the
distribution coefficient -
- then
- m A KL (kDcg cL)
54THE CONCEPT OF GAS TRANSFER COEFFICIENTS
- The value of kD/kg will be very small with
respect to 1/kL ? the influence of the gas
transfer coefficient of the gas phase may be
neglected ? - KL kL
- and consequently
- m A kL (kDcg cL)
55FILM THEORY
56FILM THEORY
57FILM THEORY
58FILM THEORY
59FILM THEORY
60PENETRATION THEORY
- During the time of exposure the gas diffuses into
the fluid element ? penetrates into liquid. - In contrast to the film theory, the penetration
process is described by unsteady diffusion
61PENETRATION THEORY
62PENETRATION THEORY
63PENETRATION THEORY
- During the time of the liquid the interface to
the gas, the gases penetrate into the liquid at a
diminishing rate. The total mass of gas absorbed
during this time
64PENETRATION THEORY
- Hence the average absorption rate m (g/s) during
the time t is defined by - The penetration assumes
- t tc
- for a gas transfer process operated under
steady state condition
65PENETRATION THEORY
- The final form of the rate expression for gas
absorption as proposed by the penetration theory
66PENETRATION THEORY
- According to the penetration theory
-
- stating that the coefficient of gas transfer is
proportional to the root of the coefficient
diffusion.
67PENETRATION THEORY
- Assumption of a constant time of exposure of
fluid elements to the gas phase ? a constant rate
rc (s-1) - Taking rc instead of tc
-
68SURFACE RENEWAL THEORY
- The model underlying the surface renewal theory
is equal to that of the penetration theory ?
unsteady diffusion of the gas into liquid
elements exposed to the gas phase. - However, this theory does not assume that the
time to be constant ? follow a frequency
distribution f(t) with ages of the fluid elements
( time of exposure) ranging from zero to
infinity.
69SURFACE RENEWAL THEORY
- The theory is based on the assumption ? the
fraction of the surface having ages between t and
tdt is given by -
- ? if the surface element of any age always has
chance of s.dt of being replaced ? if each
surface element is being renewed with a frequency
s, independent of its age -
70SURFACE RENEWAL THEORY
- The average rate of gas transfer is
- The surface renewal theory forecasts
71FILM-SURFACE-RENEWAL THEORY
- This theory attempts a combination of the film
theory and the surface renewal theory in
principle ? a combination of steady and unsteady
diffusion. - The gas transfer coefficient as a function of the
rate of surface renewal s and max x dL -
72COMPARISON OF THE THEORIES
73FACTORS AFFECTING THE GAS TRANSFER COEFFICIENTS
- The effects of temperature on the rate gas
transfer (effects on kL and A) - The temperature coefficient ? for oxygenation of
sewage ? in the range of 1,016 to 1,047.
74FACTORS AFFECTING THE GAS TRANSFER COEFFICIENTS
- The influence of hydrophobic constituents and
surface active agents on the rate of gas transfer
? Gibbs adsorption equation -
- c concentration of hydrophobic substance in
the bulk of the solution (g/m3) - S excess concentration of hydrophobic
substance at the surface (g/m3) as compared with
that of the bulk solution - R universal gas constant
- d?/dc rate of increase of surface tension with
increasing the concentration of the
hydrophobic substance -
75FACTORS AFFECTING THE GAS TRANSFER COEFFICIENTS
76FACTORS AFFECTING THE GAS TRANSFER COEFFICIENTS
77THE OVERALL GAS TRANSFER COEFFICIENT OR AERATION
COEFFICIENT
- Under steady state conditions of gas transfer
operation ? the coefficient diffusion and the
time of exposure may be assumed constant - where k2 or kL.a is the overall gas transfer
coefficient. -
78THE OVERALL GAS TRANSFER COEFFICIENT OR AERATION
COEFFICIENT
- The rate of gas transfer can be expressed as the
rate of concentration change -
-
- which integrates with c0 at t0 to
-
- or
79THE OVERALL GAS TRANSFER COEFFICIENT OR AERATION
COEFFICIENT
- The overall gas transfer coefficient k2 can
easily determined experimentally by measuring the
change of concentration as a function of time and
by plotting log (cs-c)/(cs-c0) versus time
80THE EFFICIENCY COEFFICIENT
- With some transfer operations, e.g. cascades,
weir aeration ? difficult or impossible to
determine the parameter time t. - If now a constant time tk is assumed for the
aeration step under steady state conditions
81THE EFFICIENCY COEFFICIENT
82THE EFFICIENCY COEFFICIENT
83THE OXYGENATION CAPACITY
84THE OXYGENATION CAPACITY
85THE OXYGENATION CAPACITY
86AIR STRIPPING
87AIR STRIPPING
88AIR STRIPPING
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