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Dr.-Eng. Zayed Al-Hamamre
Multiphase Reacting Systems:
Gas-Solid Systems
Advance Chemical Reaction Engineering
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Content
Introduction
Constant-Size Particle
Shrinking Particle
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Gas-solid reacting systems can be classified as systems in which
o The solid is reacted to another solid or other solids,
Or generally
Introduction
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Such a reaction is frequently encountered in the process industry (e.g., in coal gasification, in
ore processing, iron production in the blast-furnace, and roasting of pyrites.
The rate of such reactions depends on the relative magnitudes of the rate of transport and the
rate of reaction whether or not important gradients inside and around the particle are built up
or not.
Introductiono The solid disappears in forming gaseous product(s).
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Any of the following mass transfer resistances can be important
o Film diffusion: With a fast surface reaction on a nonporous particle, mass transfer
limitations can arise in the fluid phase.
o Pore diffusion: With porous particles, pore diffusion is likely to limit reaction rates at the
internal surface.
o Product layer diffusion: Many fluid-solid reactions generate ash or oxide layers that impede
further reaction.
o Sublimation: Some solids sublime before they react in the gas phase. Heat transfer can be
the rate-limiting step.
The surface reaction itself can be rate limiting.
Introduction
With gas-solid reactions the conditions inside the particle change with time, since the solid
itself is involved in the reaction.
The process is therefore essentially of a non-steady-state nature.
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Geometries Reacting Solids
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Geometries Reacting Solids
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Reaction Rate of Solids The reaction of solids occurs in the monolayer of molecules adsorbed on the surface of the
solid B,
The molecules of the solid react with the gaseous molecules to form a gaseous product and
remove solid molecules.
s
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Since is independent of the conversion of the solid, it is constant as long as any solid is
present.
The concentration of solid B at the surface is constant because new surface is exposed
continuously so that the concentration of exposed solid B, is always one monolayer
Reaction Rate of Solids
s
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A gas reacting with a solid of low porosity to
yield a porous non-reacted layer, often called
"ash" layer.
The reaction then takes place in a narrow zone
that moves progressively from the outer
surface to the center of the particle.
Such a situation is described by the so-called
heterogeneous shrinking-core model
Concentration proms of gas and
solid reactants
Qualitative Analysis
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When the transport rates through the two layers are not
too different and the true rate of reaction is not infinitely
fast,
o The situation is no longer as clear cut, and
o The sharp boundary between reacted and unreacted
zone no longer exists.
Qualitative Analysis
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When the transport through both reacted
and unreacted structures is usually fast
compared with the true reaction rate,
o The reaction rate, is governing the rate
of the overall phenomenon.
o Then there are no gradients whatever
inside the particle.
Qualitative Analysis
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Constant-Size Particle
Assumption
The reacting particle is isothermal.
The particle size remains constant during reaction.
The integrity of the particle is maintained (it doesn’t break apart),
The densities of solid reactant B and solid product (surrounding B) be nearly equal.
The single particle acts as a batch reactor in which conditions change with respect to time t.
The solid does not disappear or appear but rather transforms from one solid phase into another
as the reaction proceeds ,
Any effect of external mass transfer is the same in all cases, regardless of the situation within
the particle
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Constant-Size Particle
In a nonporous solid B,
Reactant A initially reacts with
the exterior surface of B,
As product solid (assumed to be
porous) is formed, A must
diffuse through a progressively
increasing thickness of porous
product to reach a progressively
receding surface of B.
There is a sharp boundary
between the porous outer layer of
product and the nonporous
unreacted or shrinking core of
reactant B
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In a very porous solid B,
Τhere is no internal diffusional resistance, all parts of the interior of B are equally accessible
to A, and reaction occurs uniformly (but not instantaneously) throughout the particle.
Ιn the general case
The reactant and product solids are both relatively porous, the concentration profiles for A and
B with respect to radial position (r) change continuously
is either zero (completely reacted outer layer) or ρBm (unreacted core of
pure B);
Constant-Size Particle
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For an isothermal spherical particle of radius R, a material balance for reactant A(g) around
the thin shell (control volume) of (inner) radius r and thickness dr, taking both reaction and
diffusion into account,
B.C 1
B.C 2
Constant-Size Particle
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the amount of B present in a particle is
The decrease in volume or radius of unreacted core accompanying the disappearance of dNB
moles of solid reactant is
For the reaction
I.C
Constant-Size Particle
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Two idealized models can be used to describe the reaction process
i. Progressive-Conversion Model
ii. Shrinking-Core Model
Uniform reaction model
Reactant gas enters and reacts
throughout the particle at all times,
most likely at different rates at
different locations within the
particle.
Thus, solid reactant is converted
continuously and progressively
throughout the particle
Progressive-Conversion
Model
Constant-Size Particle
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o Step 1: Diffusion of gaseous reactant A
through the film surrounding the particle
to the surface of the solid.
o Step 2: Penetration and diffusion of A
through the blanket of ash to the surface
of the unreacted core.
o Step 3: Reaction of gaseous A with solid
at this reaction surface.
Shrinking-Core ModelShrinking-Core Model
The reaction occurs first at the outer skin
of the particle.
The zone of reaction then moves into the
solid, leaving behind completely converted
material and inert solid (ashes)
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Shrinking-Core Model
Then, the conversion is
o Step 4: Diffusion of gaseous products through the ash back to the exterior surface of the
solid.
o Step 5: Diffusion of gaseous products through the gas film back into the main body of fluid.
Film formation model
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Shrinking-Core Model
There is a sharp boundary (the reaction
surface) between the nonporous
unreacted core of solid B and the
porous outer shell of solid product
(sometimes referred to as the “ash
layer
Outside the particle, there is a gas film
reflecting the resistance to mass
transfer of A from the bulk gas to the
exterior surface of the particle.
As time increases, the reaction surface
moves progressively toward the center
of the particle; that is, the .unreacted
core of B shrinks.
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Shrinking-Core Model To find the time required to reach a fraction of B converted, for a spherical particle of species
B of radius R undergoing reaction with gaseous species A
The material balance across a thin spherical
shell in the ash layer at radial position r and with
a thickness dr,
G/S systems the shrinkage of the unreacted core is
slower than the flow rate of A toward the unreacted
core by a factor of about 1000, which is roughly the
ratio of densities of solid to gas.
Because of this it is reasonable to assume, in
considering the concentration gradient of A in the ash
layer at any time, that the unreacted core is stationary.
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Shrinking-Core Model
B.C 1
B.C 2
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Shrinking-Core Model
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Shrinking-Core Model
and substitution of the resulting expression for
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Shrinking-Core Model
But
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The resistances act in series and are all linear in concentration.
Shrinking-Core Model The time required for complete conversion of the particle
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Diffusion Through Gas Film Controls
Shrinking-Core Model
No gaseous reactant is present at the
particle surface;
The concentration driving force is
constant at all times during reaction of
the particle
Where Sex is the unchanging exterior surface of a particle
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Shrinking-Core Model
The variation of the
unreacted core with time
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Diffusion through Ash Layer Controls
Shrinking-Core Model
Both reactant A and the
boundary of the unreacted
core move inward toward the
center of the particle.
In the ash layer, no reaction
of A take place (inert layer),
The shrinkage of the
unreacted core is slower than
the flow rate of A toward the
unreacted core by a factor of
about 1000,
Constant
The unreacted core is stationary
And
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Thus the rate of reaction of A at any instant is given by its rate of diffusion to the reaction
surface, or
Shrinking-Core Model
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Shrinking-Core Model
The progression of reaction in terms of the time required for complete conversion
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Shrinking-Core Model
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Shrinking-Core Model
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Chemical Reaction Controls
Shrinking-Core Model
The progress of the reaction is unaffected by
the presence of any ash layer,
The rate is proportional to the available
surface of unreacted core
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Shrinking-Core Model
The decrease in radius or increase in fractional conversion of the particle in terms of τ is
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Shrinking (Dissolving) Solid Particle When no ash forms, as in the burning of pure carbon in air, the reacting particle shrinks during
reaction, finally disappearing
o Step 1: Diffusion of reactant A
from the main body of gas
through the gas film to the
surface of the solid.
o Step 2: Reaction on the surface
between reactant A and solid.
o Step 3: Diffusion of reaction
products from the surface of the
solid through the gas film back
into the main body of gas.
There is no product or “ash” layer, and hence no ash-
layer diffusion resistance for A
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Shrinking (Dissolving) Solid Particle
The reacting particle is isothermal.
The particle is nonporous, so that reaction occurs only on the exterior surface.
The surface reaction between gas A and solid B is first-order
Model Assumption
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Shrinking (Dissolving) Solid Particle
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Shrinking (Dissolving) Solid Particle
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But
Shrinking (Dissolving) Solid Particle
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Shrinking (Dissolving) Solid ParticleGas Film Diffusion Controls
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Example
Rearranging
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Example
Rearranging
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Example Cont.
The mass-transfer-limited growth time is much shorter than the reaction-limited growth time,
Therefore, the reaction should be nearly reaction controlled with a reaction time of 2.77 min.