Abstract
Reading and co-workers introduced a new technique a few years ago called Modulated Differential Scanning Calorimetry or MDSC. Here the first part of a theoretical analysis for this technique is given. A simple mathematical model for modulated differential scanning calorimetry in the form of an ordinary differential equation is derived. The model is analysed to find the effect of a kinetic event in the form of a chemical reaction. Some possible sources of error are discussed. A more sophisticated version of the model allowing for spatial variation in a calorimeter is developed and it is seen how it can be reduced to the earlier model. Some preliminary work on a phase change is also presented.
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Abbreviations
- a :
-
(remaining) mass fraction of reactant or crystalline material
- a 0 :
-
initial mass fraction
- b :
-
temperature ramp
- c :
-
specific heat capacity
- f :
-
rate of heat intake by a kinetic process within the sample
- g :
-
temperature-dependence function of a reaction rate
- h :
-
distribution function for molecular weights
- k :
-
thermal conductivity
- K a :
-
function appearing in the Avrami equation
- l :
-
length scale of a (one-dimensional) calorimeter
- l s :
-
half-width of a sample
- m :
-
complex spatial-decay rate of modulated temperature
- m j :
-
coefficients in a power series for α1 (j=1,2,...)
- n :
-
outward normal
- n j :
-
coefficients in a power series for α2 (j=1, 2,...)
- p :
-
order of a reaction
- q, q j :
-
coefficients appearing in expressions for\(\mathop \Delta \limits^ \sim \) T(j=C, S, D, 1, 2, 3, 4)
- r :
-
reaction rate
- r′ :
-
temperature derivative of reaction rate
- s :
-
time used in integrations
- s d :
-
dimensionless position of a free boundary
- s f :
-
position of a free boundary
- t :
-
time
- t 2 :
-
time scale of melting
- u :
-
real part ofw
- v :
-
imaginary part ofw
- w=wR, ws,W F :
-
functions of position determiningT
- W j :
-
coefficients in power seriesw (j=0, 1, 2...)
- x :
-
position within calorimeter or sample
- y :
-
dimensionless position
- zo,zR,zs:
-
functions of position determining¯T
- A :
-
pre-exponentional rate constant
- A * :
-
adjusted pre-exponential rate constant
- A + :
-
scaled pre-exponential rate constant
- A j :
-
coefficients appearing in expressions of cyclic temperature in regionj (j=1, 2, 3)
- B :
-
amplitude of modulation of temperature
- B :
-
complex amplitude of temperature (a complex multiple ofB)
- B j :
-
complex amplitude ofT j (j=F, R, S, RM or SM)
- C(T):
-
heat capacity of the sample when it depends up on temperature
- CR,CS:
-
heat capacities of pan and sample
- C j :
-
coefficients appearing in expressions of cyclic temperature in regionj(j=1, 2, 3)
- ¯C s :
-
value of sample's heat capacity given by underlying “measurement”
- C s :
-
value of sample's heat capacity given by cyclic “measurement”
- D :
-
heat capacity of sample regarding it as a function ofσ
- E :
-
activation energy
- F, G :
-
functions of time appearing in a nearly periodic signal
- FM,¯GM,GM:
-
“measured” versions ofF, G
- G a :
-
function appearing in the Avrami equation
- H :
-
heat of reaction
- I :
-
function of time appearing in a nearly periodic signal
- ĪM,ĪM:
-
“measured” versions ofI
- K :
-
effective heat-transfer coefficients
- Kt,K0,K1,K2:
-
internal heat-transfer coefficients
- L :
-
latent heat
- M :
-
mass of sample
- M j :
-
coefficients in expressions for\(\mathop \Delta \limits^ \sim \) T(j=1,2,3,4)
- N :
-
exponent appearing in the Avrami equation
- P :
-
coefficient appearing an\(\mathop \Delta \limits^ \sim \) T
- QR,Qs:
-
heat contents of reference pan, sample pan plus sample
- R :
-
gas constant
- S :
-
a surface
- S b :
-
cross-sectional area of a bar
- S c :
-
cross-sectional area of a sample
- S F :
-
external surfaces of calorimeter
- SR,Ss:
-
surfaces of reference and sample pans
- T :
-
temperature
- T :
-
scaled complex amplitude of modulated temperature
- Ti(x):
-
temperature on initiation of melting
- T c :
-
melting temperature
- T e :
-
external temperature
- TF,T R ,TS:
-
temperatures of furnace, reference, sample
- TRM,TSM:
-
temperatures measured for reference and sample
- T o :
-
initial temperature
- Ta,T1,T2:
-
typical temperatures
- T oj :
-
initial values ofT j(j=F, R, S, RM, SM)
- Toj,Tlj:
-
coefficients appearing in expressions for underlying temperature in regionj of a one-dimensional calorimeter (j=1,2,3)
- ΔT :
-
temperature difference,T R-T S
- ΔT j :
-
coefficients in a power series ofΔT (j= 0,1, 2,...)
- U :
-
dimensionless temperature based on reaction rate
- W :
-
molecular weight
- Z(W):
-
mass fraction with molecular weight ≤W
- α:
-
scaled amount of reactant
- αj :
-
surface integrals of normal derivatives ofw's (j=1,2,3)
- β:
-
spatial decay rate of modulated temperature
- γj :
-
surface integrals of normal derivatives of z's (j=1,2,3)
- δ:
-
dimensionless temperature over whichC(T) varies
- ɛ:
-
1/dimensionless activation energy
- ɛm :
-
Stefan number
- η:
-
error in measurement of temperatures due to location of thermo-couples
- λ:
-
degree of bias
- ρ:
-
density
- σ:
-
rescaled dimensionless temperature
- τ:
-
dimensionless time
- ϕ:
-
phase lag
- ϕb, ϕc :
-
baseline and corrected phase lags
- ϕs :
-
phase of alternative “reference” signal, e.g. furnace modulation
- ψ:
-
ratio indicating importance of ωC R compared withK (“departure from perfection”)
- θ:
-
dimensionless temperature
- θi :
-
dimensionless temperature on initiation of melting
- ω:
-
angular frequency of modulation of temperature
- Ω:
-
rescaled angular frequency
- -:
-
underlying part (notC's,F's,G's,I's)
- ∼:
-
cyclic part (notC's,F's,G's,I's)
- ':
-
derivative with respect to argument (notr)
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Dedicated to Prof. Menachem Steinberg on the occasion of his 65th birthday
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Lacey, A.A., Nikolopoulos, C. & Reading, M. A mathematical model for Modulated Differential Scanning Calorimetry. Journal of Thermal Analysis 50, 279–333 (1997). https://doi.org/10.1007/BF01979568
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DOI: https://doi.org/10.1007/BF01979568