Introduction The objective of evaporation is to concentrate a solution consisting of a nonvolatile solute and a volatile solvent In the overwhelming majority of evaporations the solvent is water ID: 624734
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Slide1
EvaporationSlide2
Introduction
The objective of evaporation is to concentrate a solution consisting of
a nonvolatile
solute and a volatile solvent. In the overwhelming majority of
evaporations the
solvent is water.
When the liquid
phase is agitated, mass-transfer in the liquid phase
is sufficiently
rapid that the rate of evaporation of solvent
can be
determined by the rate of heat transfer from the
heating medium
, usually condensing steam, to the
solution.
Evaporation differs from
drying in that the residue is a liquid-sometimes a highly viscous
one-rather than
a
solid.
it
differs from distillation in that the vapor usually is a
single component
, and even when the vapor is a mixture, no attempt is made in
the evaporation
step to separate the vapor into
fractions.
Mineral-bearing
water often is evaporated to give a solid-free product
for boiler
feed, for special process requirements, or for human consumption.
This technique
is often
called
water distillation, but technically it is evaporation.Slide3
Liquid characteristics
Concentration
The density
and viscosity
increase with solid content until either the solution becomes
saturated or
the liquor becomes too viscous for adequate heat transfer
.
continued boiling of
a saturated solution causes crystals to form; these must be removed or the
tubes clog.
The
boiling point of the solution may also rise considerably as the
solid content
increases, so that the boiling temperature of a concentrated solution
may be
much higher than that of water at the same pressure
.
2. Foaming
A
stable foam accompanies the vapor out of the evaporator, causing
heavy entrainment
. In extreme cases the entire mass of liquid may boil over into
the vapor
outlet and be lost
.
3.
Temperature
sensitivity
4. Scale
رسوب
5. Materials
of
construction
6. Toxicity,
explosion hazards, radioactivity, and
necessity for
sterile
operationSlide4
Once-through circulation evaporators
These evaporators are
well adapted to multiple-effect
operation
Agitated-film
evaporators are
always operated
once
through
Falling-film
and climbing-film evaporators can also
be operated
in this
way
Useful
for heat-sensitive
materials, By
operating under high vacuum, the temperature of the liquid can be kept
low
With a single rapid passage through the tubes the thick liquor is at the
evaporation
Temperature
but a short time and can be quickly cooled as soon as it leaves
the evaporatorSlide5
Circulation evaporators
Although the average residence time of the liquid in the heating
zone may
be short, part of the liquid is retained in the evaporator for a
considerable time
. Prolonged heating of even a small part of a heat-sensitive material like
a food
can ruin the entire
product.
Climbing-film
evaporators are
usually
circulation
units.Slide6
Continuous flow evaporators
1. Horizontal-tube
evaporator.
inside of which
steam condenses and outside of which the
solution to
be concentrated boils
.
Agitation is provided
only by the movement of the
bubbles formed
. Therefore, this type of unit is only suitable for low-viscosity solutions that do not deposit scale on the heat-transfer surfaces.Slide7
Continuous flow evaporators
2. Short-vertical-tube
evaporator.
solution
inside the tubes and
steam condensing
outside.
Boiling inside
the tube causes the solution to circulate,
thus providing
additional
agitation
not
suitable for very viscous solutions.Slide8
Continuous flow evaporators
3. Long-vertical-tube evaporator
Higher
tube-entering liquid velocity
Higher
heat-transfer
coefficient
For liquids
that tend to foam.Slide9
Continuous flow evaporators
4. Forced-circulation evaporator
Very
viscous solutions
A
pump is used to force the
solution upward
Through relatively short tubes
Because
of the high velocities in a
forced-circulation evaporator
, the residence time of the liquid in the tubes is short-about 1
to 3 s-so that moderately heat-sensitive liquids can be concentrated in them.
Salting
liquors or those that tend to foam.Slide10
Continuous flow evaporators
5. Falling-
f
ilm evaporator
heat-sensitive
solutions such as
fruit juices
The flows
as a
film inside
walls of the
tubesThe concentrate and
the vapor produced are separated at the bottomSlide11
Continuous flow evaporators
6
. AGITATED-FILM EVAPORATOR
The principal resistance to overall heat
transfer from
the steam to the boiling liquid in an evaporator is on the liquid side.
One way
of reducing this resistance, especially with viscous liquids, is by
mechanical agitation
of the liquid
film.
This is a modified falling-film evaporator with a single jacketed tube containing an internal agitator.
High rates of heat transfer with viscous liquids
Viscous
heat-sensitive products as gelatin, rubber latex, antibiotics, and fruit juices.Slide12
Performance of tubular evaporators
Capacity is defined as the number of
kilograms
of
water vaporized per hour.
Economy
is the number of kilograms vaporized
per
kilogram
of steam fed to the
unit.
In a single-effect evaporator the economy is nearly always less than 1, but in multiple-effect equipment it may be considerably greater.
The steam consumption, in kilograms per hour, is also important. It equals the capacity divided by the economy.
The
rate of heat transfer
q through the heating surface of an
evaporator
is
the
product of
three factors: the area of the heat-transfer surface
A, the overall
heat-transfer
coefficient
U, and the overall temperature drop
Δ
T.
q = UA
Δ
TSlide13
Evaporator
Economy
Influencing factor
1. Number of effects
By
proper design the enthalpy of vaporization of the steam to the
first effect
can be used one or more times, depending on the number of effects.
2. Temperature
of the
feedSlide14
Effect of the feed state on the capacity
If the feed to the evaporator is at the boiling temperature corresponding
to the absolute
pressure in the vapor space, all the heat transferred through
the heating
surface is available for evaporation and the capacity is proportional to
q
.
If the feed is cold, the heat required to heat it to its boiling point may be
quite large
and the capacity for a given value of
q is reduced accordingly, as heat used to heat the feed is not available for
evaporation.if the feed is at
a temperature
above the boiling point in the vapor space, a portion of the
feed
evaporates spontaneously by adiabatic equilibration with the vapor-space
pressure and
the capacity is greater than that corresponding to
q. This process is called
flash evaporation.Slide15
Boiling-point elevation
(BPE
)
For a given pressure in the vapor space
of
an evaporator, the boiling temperature of an aqueous solution will be equal to that of pure water if the solute is not dissolved in
the
water
but rather consists of small, insoluble, colloidal material
.
If the solute is soluble, the boiling temperature will
be greater than that of pure water by an amount known as
the boiling-point elevation of the solution.
In
actual evaporators, however, the
boiling point
of a solution is affected by two factors, boiling-point elevation and
liquid head
.
If, as is usually
the case
, the solute has little or no vapor pressure, the
evaporator
pressure is equal to the partial pressure of the water in
the solution
. Then, by a modified
Raoult's
law:Slide16
Diihring
chart for aqueous solutions of
sodium hydroxide
.Slide17
Nomograph
for
boiling-point
elevation of
aqueous
solutionsSlide18Slide19
Effect of liquid head and friction on temperature drop
If
the depth
of liquid in an evaporator is appreciable, the boiling point
corresponding to
the pressure in the vapor space is the boiling point of the surface layer of
liquid only
.
The average boiling point of the liquid in the tubes is higher than the boiling point corresponding to the pressure in the vapor because:
pressure
of the vapor
space head of Z meters or feet
of liquid frictional loss in the tubes increases the average pressure of the
liquid (large liquid velocity).
This increase in boiling point lowers the average temperature drop
between the
steam and the liquid and reduces the
capacity.
The
amount of reduction
cannot be
estimated quantitatively with precision, but the qualitative effect of liquid
head, especially
with high liquor levels and high liquid velocities, should not be
ignored.
The
temperature drop is fixed by the
properties of
the steam and the boiling liquid and
except for
the effect of hydrostatic
head is
not a function of the evaporator construction.Slide20
Heat transfer coefficients
The overall coefficient, on
the other
hand, is strongly influenced by the design and method of operation of
the evaporator.
the overall resistance to heat
transfer between
the steam and the boiling liquid is the sum of five individual resistances:
The steam-film resistance (not important, the presence of non-condensable gas seriously reduces the steam-film coefficient)
Inside
and outside the
tubesThe tube-wall resistance (not important)
The resistance from the boiling liquid.Slide21
The liquid-side coefficient
The liquid-side coefficient depends to a large extent
on the
velocity of the liquid over the heated surface. In most evaporators,
and especially
those handling viscous materials, the resistance of the liquid side
controls the
overall rate of heat transfer to the boiling liquid
.
Forced circulation gives high liquid-side coefficients even though
boiling inside
the tubes is suppressed by the high static head.
The formation of scale on the tubes of an evaporator adds a thermal resistance equivalent to a fouling factor.Slide22
single-effect evaporation
When a single evaporator is used, the vapor from the boiling liquid
is condensed
and discarded
.
This method is called
single-effect evaporation,
and
although
it is simple, it utilizes steam ineffectively
.
To evaporate 1 kg of water from a solution calls for from 1 to 1.3 kg of steam.Slide23
weight-fraction solute:
wf
mass
flow
rate:
mf
1. The thin-liquor feed has only one volatile
component, e.g
., water.
2. Only the latent heat of the heating steam at T, is
available for
heating and vaporizing the solution in the evaporator.3. The boiling action on the heat-exchanger surfaces
agitates the solution, in the evaporator, sufficiently to achieve perfect mixing Te= Tp
and
Tv
= Tp.
4. Driving force for heat
transfer =
Δ
T
= Ts -
Tp
5. The
Δ
T
is high enough to
achieve nucleate
boiling and not so
high as
to cause film
boiling
6. No
heat loss from the
evaporator
Continuous-flow, steady-state model evaporatorSlide24
Continuous-flow, steady-state model evaporatorSlide25
Enthalpy-concentration diagram for sodium hydroxide-water system
.Slide26
Multiple-Effect Evaporator
Systems
When condensing steam is used to evaporate water
from an
aqueous solution, the heat of condensation of the
higher temperature condensing
steam is less than the heat of
vaporization of
the lower-temperature boiling
water. consequently, less
than 1 kilogram of vapor is produced
per kilogram condensation of heating steam. This ratio is called the economy.
To reduce the amount of steam required and, thereby, increase the economy, a series of evaporators, called effects, can be
used.
The
increased economy is achieved by operating the
effects
at different pressures, and thus at different boiling
temperatures, so
that vapor produced in one effect can be
condensed to
supply the heat in another effect.Slide27
Multiple-Effect Evaporator
Systems
1. Forward-feed,
triple-effectSlide28
Multiple-Effect Evaporator
Systems
1. Forward-feed,
triple-effect
This pattern of liquid flow is the simplest.
One-third
of
the total
evaporation occurs in each effect
.
To achieve a temperature-driving force for
heat transfer in the second effect, the pressure of the second effect, P2, is lower than that of the first effect. This
procedure is repeated in the third effect.For three effects, the flow
rate of
steam entering the first is only about one-third of
the amount
of steam that would be required if only one
effect were used.
the
temperature-driving force in
each of
the three effects is only about one-third of that in a
single effect.
Therefore
, the heat transfer area of each of the
three evaporators
in a triple-effect system is approximately
the same
as for the one evaporator in a single-effect
unit.
It
requires a pump for
feeding
dilute solution to the first
effect, since
this effect is often at about atmospheric pressure, and a pump to
remove thick
liquor from the last effect. The transfer from effect to effect, however, can
be done
without pumps, since the flow is in the direction of decreasing pressure,
and control
valves in the transfer line are all that is required
.Slide29
Multiple-Effect Evaporator Systems
2. Backward-feed,
triple-effectSlide30
Backward-feed, triple-effect
When the temperature of the fresh feed is
significantly below
its saturation temperature corresponding to the
pressure in
the first effect,
backward-feed operation is
desirable.
Th
e
cold fresh feed is sent to
the third effect, which operates at the lowest pressure and, therefore, the lowest temperature.
Unlike the forward-feed system, pumps
are required to move the concentrate from
one effect
to the next because
PI >
P
2
> P3.
Backward
feed often gives a higher capacity than forward feed when the
thick liquor
is viscous, but it may give a lower economy than forward feed when
the feed
liquor is cold.Slide31
Multiple-Effect Evaporator Systems
3.
mixed
feedSlide32
Multiple-Effect Evaporator Systems
4.
parallel feedSlide33
CAPACITY AND ECONOMY OF MULTIPLE-EFFECT
EVAPORATORS
The total capacity of a multiple-effect evaporator is usually no
greater than
that of a single-effect evaporator having a heating surface equal to one
of the
effects and operating under the same terminal conditions, and, when there
is an
appreciable boiling-point elevation, is often considerably smaller
.
When
the boiling-point elevation is negligible, the effective overall ΔT
equals the sum of the ΔT's in each effect, and the amount of water evaporated per unit area of surface
in
an
N-effect multiple-effect evaporator is approximately
1/Nth
that in the
single effect
. Slide34
Effect of boiling-point elevation on capacity of evaporatorsSlide35
Effect of boiling-point elevation on capacity of evaporators
Consider an evaporator that is concentrating a solution with a
large boiling-point
elevation. The vapor coming from this boiling solution is at
the solution
temperature and is therefore superheated by the amount of the
boiling point elevation.
Superheated steam is
essentially equivalent to saturated steam at the same pressure when used as
a heating
medium.
The temperature drop in any effect, therefore, is calculated from the temperature of saturated steam at the pressure of the steam chest, and
not from the temperature of the boiling liquid in the previous effect. This means that the boiling-point elevation in any effect is lost from the total available
temperature drop
. This loss occurs in every effect of a multiple-effect evaporator, and
the resulting
loss of capacity is often important
.
The boiling-point elevation tends
to make
the capacity of a multiple-effect evaporator less than that of the
corresponding single
effect
.
In a single-effect unit producing 50 percent
NaOH
,
for example
, the overall coefficient
U for this viscous liquid would be small. In
a
triple-effect
unit, the coefficient in the final effect would be the same as that in
the single
effect, but in the other effects, where the
NaOH
concentration is much
lower than
50 percent, the coefficients would be greater. Thus the average coefficient
for the
triple-effect evaporator would be greater than that for the single effect
.Slide36
The
economy of a
multiple effect
evaporator
depends on heat-balance considerations and not on the rate
of heat
transfer.
The
capacity
is reduced by the
boiling-point
elevation.The capacity, on the other hand, is reduced by the
boiling-point elevation. The capacity of a double-effect evaporator concentrating a solution with a boiling-point elevation is generally less than half the capacity of two single
effects, each
operating with the same overall temperature drop. The capacity of a
triple effect
is generally less than one-third that of three single effects with the
same terminal
temperatures
.
The optimum number of effects must be
found from
an economic balance between the savings in steam obtained by
multiple-effect operation
and the added investment required.Slide37