Theory Residence time distribution
an rtd curve reasonably well-mixed reactor
the theory of residence time distributions begins 3 assumptions:
the incompressibility assumption not required, compressible flows more difficult work , less common in chemical processes. further level of complexity required multi-phase reactors, separate rtd describe flow of each phase, example bubbling air through liquid.
the distribution of residence times represented exit age distribution,
e
(
t
)
{\displaystyle e(t)}
. function
e
(
t
)
{\displaystyle e(t)}
has units of time , defined such that
∫
0
∞
e
(
t
)
d
t
=
1
{\displaystyle \int _{0}^{\infty }e(t)\,dt=1}
.
the fraction of fluid spends given duration,
t
{\displaystyle t}
inside reactor given value of
e
(
t
)
d
t
{\displaystyle e(t)dt}
.
the fraction of fluid leaves reactor age less
t
1
{\displaystyle t_{1}}
is
∫
0
t
1
e
(
t
)
d
t
{\displaystyle \int _{0}^{t_{1}}e(t)\,dt}
.
the fraction of fluid leaves reactor age greater
t
1
{\displaystyle t_{1}}
is
∫
t
1
∞
e
(
t
)
d
t
=
1
−
∫
0
t
1
e
(
t
)
d
t
{\displaystyle \int _{t_{1}}^{\infty }e(t)\,dt=1-\int _{0}^{t_{1}}e(t)\,dt}
.
the average residence time given first moment of age distribution:
t
¯
=
∫
0
∞
t
⋅
e
(
t
)
d
t
{\displaystyle {\bar {t}}=\int _{0}^{\infty }t\cdot e(t)\,dt}
.
if there no dead, or stagnant, zones within reactor
t
¯
{\displaystyle {\bar {t}}}
equal
τ
{\displaystyle \tau }
, residence time calculated total reactor volume , volumetric flow rate of fluid:
τ
=
v
v
{\displaystyle \tau ={\frac {v}{v}}}
.
the higher order central moments can provide significant information behavior of function
e
(
t
)
{\displaystyle e(t)}
. example, second central moment indicates variance (
σ
2
{\displaystyle \sigma ^{2}}
), degree of dispersion around mean.
σ
2
=
∫
0
∞
(
t
−
t
¯
)
2
⋅
e
(
t
)
d
t
{\displaystyle \sigma ^{2}=\int _{0}^{\infty }(t-{\bar {t}})^{2}\cdot e(t)\,dt}
the third central moment indicates skewness of rtd , fourth central moment indicates kurtosis (the peakedness ).
one can define internal age distribution
i
(
t
)
{\displaystyle i(t)}
describes reactor contents. function has similar definition
e
(
t
)
{\displaystyle e(t)}
: fraction of fluid within reactor age of
t
{\displaystyle t}
i
(
t
)
d
t
{\displaystyle i(t)dt}
. shown danckwerts, relation between
e
(
t
)
{\displaystyle e(t)}
,
i
(
t
)
{\displaystyle i(t)}
can found mass balance:
i
(
t
)
=
1
τ
(
1
−
∫
0
t
e
(
t
)
d
t
)
e
(
t
)
=
−
τ
d
i
(
t
)
d
t
{\displaystyle i(t)={\frac {1}{\tau }}\left(1-\int _{0}^{t}e(t)\ dt\right)\qquad e(t)=-\tau {\frac {di(t)}{dt}}}
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