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a
b
c
k
d
Fig. 6.2a-d
Plots used to obtain the kinetic equations.
Δ
T =
Δ
T (
ω
, t ) ( a ), T = T (
ω
, t ) ( b ),
η
=
η(ω , t ) ( c ), ˙
η = ˙
η(ω , t ) ( d )
line
η k = const yields i points with abscissas t 1 , t 2 , t i . Each abscissa t i corre-
sponds to one value of T i and ˙
η
=
η i (Fig. 6.2b, d). Thus one obtains a locus of points
in the ˙
η
T coordinates that form a plot of ˙
η i against T . Since each value of
η 1 ,
η 2 ,
η k corresponds to the curve ˙
η
( T ), one obtains a set of k curves ˙
η
= ˙
η
( T ) at
η
= const representing the graphical form of ˙
η
= ˙
η
( T ,
η
) (Fig. 6.3a). The number
of experimental points on the ˙
η
( T ) curve at
η
= const equals the number of exper-
iments i for various heating rates
ω i . For processes that comprise one stage overall,
data (Fig. 6.3a) can be presented as an Arrhenius anamorphosis in ln ˙
T 1 ( K 1 )
η
coordinates at
η
= const (Fig. 6.3b). The temperature interval for the dependence
˙
= ˙
η
η
( T ,
η
) can be widened by extrapolation (dotted lines in Fig. 6.3b).
 
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