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A mathematical model for Modulated Differential Scanning Calorimetry

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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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