Manganese oxide formation by heat treatment of MnCO 3 in air.
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Transcript of Manganese oxide formation by heat treatment of MnCO 3 in air.
Manganese oxide formation by heat treatment of MnCO3 in air.
MnCO3 + ½ O2MnO2+CO2
<500 C Reaction 1
>500 C Reaction 2
2 MnCO3 + ½ O2Mn2O3 + 2 CO2
Note that in reaction 1, there is a net increaseOf ½ mole of gas for each mole of Mn, and for reaction 2 there is a net increase of ¾ of a mole of gas for each mole of Mn. What can you say about the entropy change in each reaction? How does this help explain the temperature dependence between the two reactions?
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0.2 um
As the manganese oxide particles form from the carbonate salt, they begin to grow together, or ‘sinter’. The figure below is a TEM micrograph of neck formation during the
sintering of Mn2O3 particles.
Why do the necks get larger and the pores get smaller as the heat treat time and or temperature increases?
Pore
Neck
Neck
dG S dT V dP
1
m
i
Gi dni
‘Master’ Equation of Thermodynamics
For an isothermal process with no change in composition
dP P 1 P odG G P 1 G P o
dG S dT V dP
1
m
i
Gi dni
where Gi is the chemical potential per atom of type i and dni is the change in number of atoms of
type i. We know that an increase in pressure will increase the chemical potential of the components,i. Consider an incremental increase in pressure from the ambient pressure Po to a Pressure P1. Letthe the free energy at ambient pressure Po be given by G Po . Then using the master equation at
constant volume, temperature and composition in a one component system, we get .
G P 1 G P o V P( )( )
Divide both sides by the number of atoms in the 'system'
V
N
G
NChemicalPotential Gi
where is the atomic volume. Let
dP P1 Po
Substitution and rearrangement relates the chemical potential at two pressures as
Gi P1 Gi P0 P
dG S dT V dP
1
m
i
Gi dni
where Gi is the chemical potential per atom of type i and dni is the change in number of atoms of
type i. We know that an increase in pressure will increase the chemical potential of the components,i. Consider an incremental increase in pressure from the ambient pressure Po to a Pressure P1. Letthe the free energy at ambient pressure Po be given by G Po . Then using the master equation at
constant volume, temperature and composition in a one component system, we get .
G P1 G Po V P( )( )
Divide both sides by the number of atoms in the 'system'
V
N
G
NChemicalPotential G i
where is the atomic volume. Let
dP P1 Po
Substitution and rearrangement relates the chemical potential at two pressures as
Gi P1 Gi P0 P
Divide both sides by the number of atoms in the system=N
G i P 1 G i P o P ΔP=2γ/r for inside a spherical particle.
Positive and Negative CurvatureCorrugated Surface Example (2D)
solid
vapor
ΔP=γ/rPositive Curvature
ΔP=-γ/rNegative Curvature
Atoms move from
high free energy to low.
G i P 1 G i P o P