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3.5.2. VLDL and LDL trigtyceride simulation studies
This
section describes results derivedfrom
simulation studies whichpredict
plasmaVLDL, and LDL, triglyceride specific radioactivity
curvesfollowing the
reinjectionof labelled VlDl-triglyceride. The
shapeof
thepredicted specific radioactivity curves is model
dependent.This
sectionexamines
the
predictedtriglyceride specific
radioactivity functions generated using the Zechet al
(1979) model and the model developedin
Section 3.4.4. ln addition, LDL-triglyceride simulation studiesare
presented.Simulated functions can
be
derivedby
assumingthat at time f a
labelledprecursor of VLDL triglyceride is
administered.As this precursor
isincorporated
into VLDL
triglyceridethe
specific radioactivityof
triglyceridein the VLDL
fraction increases, and then decreases asthe
labelled precursor is depletedand as a
functionof the
metabolismand
hydrolysisof VLDL.
Atdifferent times
throughoutthe
courseof the rise and fall of the
VLDLtriglyceride specific radioactivity function
it is
possibleto
determine, using amodel, the
amountof
radioactivity presentwithin with
each compartment.Taking the radioactivity values of the different
compartmentsat
specifictimes, such
as 1.5 hrs, it is
possibleto
producea
simulated function which wouldbe
producedif
labelledVlDl-triglyceride
had been isolatedat a
specifictime and then reinjected into a donor subject. If
experimentscan
beperformed
which result in functions similar to those
predictedby
thesimulation then
the
modelis
validated.The early
VLDL
triglyceride reinjection studiesof
Farquharet al
(1965)showed
that the
decay curveof
reinjected labelledVLDL
triglyceride was slowrelative
to
the riseof
theVLDL
curve after the injectionof
labelled glycerol orpalmitate.
On the
basisof this
observationthey
assumedthat the
turnover ofthe liver
triglyceride compartment was faster thanthat of VLDL,
and that theturnover
rate of the VLDL
triglyceride compartment was equalto the fall
ofthe
triglyceride curveafter a
bolus injectionof
labelled glycerolor
palmitate.Based upon
this
information ttre Zechet al
(1979) model was developed. Usingthe Zech model (Figure
2) a fit
was obtainedto
the YLDL2 triglyceride specificradioactivity data
of
subjectK
(Figure 52). Includedin this figure
are threeother panels (1.5, 3.0 and 8.0 hrs) which describe the simulated decay curves of reinjected labelled
VLDL
triglyceride isolatedat
1.5, 3.0 and 8.0 hours after theinjection of labelled glycerol. These times were
selected because theycorresponded
to the
pre-T6ax, Tmax and post-TmaxVLDL2
triglyceride specific radioactivity valuesof
subjectK.
Clearlythis
figure shows that, irrespective of whenthe VLDL
triglyceridewas
collectedfor
reinjection,the
slopeof
theVLDL
decay curye was the same as the terminal slopeof
theVLDL
triglyceridespecific radioactivity curve after injection of glycerol, reflecting
theturnover
rate of the
plasmaVLDL
triglyceride moiety. Usingthe
new modelhowever
a fit
was obtainedto the
same data (Figure53)
and, simulated decaycurves were obtained
for
reinjectedVLDL
triglyceride collectedrf
1.5,3.0
and8.0
hours.It is
clearfrom this
figure that the triglyceride decay curveof
thereinjected
VLDL
containsa rapidly falling
component,the
slopeof
which isequivalent
to the
function describingthe
turnoverrate of the N level
VLDL compartments.In
the new model (Figure 51), unlike thatof
Zechet al
(1979), itis
assumedthat the liver
triglyceride compaftmentis rate limiting
and thatwithin the VLDL
pool there are particles whichturn
over rapidly.In
subject Kthe
turnover ratesof the liver
precursor,N level
andR level
compartmentswere
0.110,
1.246and
0.089 ¡-I
respectively.The terminal
slopesof
thereinjected
VLDL
triglyceride curves werethe
same as thatof the
falling VLDLcurve after
glycerol.The
slopesof
these curves (k=0.089 h-1)
describe theturnover rate of the R level
compartmentsrather than the more
rapidlyturning over liver
precursor.In
addition,it is
importantto
observe thatalthough
the VLDL was
collectedbefore, during and after the
maximumtriglyceride specific radioactivity
was
reachedall
reinjectedVLDL
triglceride decay curves displayeda rapidly falling
component.At the later
times theproportion
of slowly
turningover
particles increasedfrom
about lOToaÍ
1.5hours to
30%oat 8 hours reflecting the
movementof label, and
henceconversion
of
particles,from the
more rapidlyN level to
slowly turning overR level
compartments.Clearly if VLDL were isolated after 10
hours andreinjected
it would be difficult to
observea rapid
componentin the
decaycurv e
Gtv 1.5 hrs
A
a
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Èît Ëd
rtêc
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lÊ.E
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10
lo
3.0 hrs 8.0 hrs
0 10 {0 50 30 ll
Hours Hours
Figure
52.Fit of
Zechet al
(1979) (Figure2)
modelto
YLDL2 triglyceride spécific radioactivity dataof
subjectK (Gly).
The other panels show simulatedVlOl
triglyceride decay curyesof
reinjectedVLDL
isolatedat
1.5, 3.0 and 8.0hours after the injection of
labelled glycerol. Triglyceride decay curves of reinjectedVLDL
arethe
same asthe
terminal slopeof the falling
partof
theVLDL
curve after glycerol.Glv
3.0 hrs
l-.5 hrs
8.0 hrs
ú
EÈ
€ ',
Ëc rt6
ú
lÉ Io
<ttÀ
€o Èo I à¡
ts{
Hours Hours
Figure 53. Fit of new model
(Figure51) to VLDLZ
triglyceride specific radioactivity dataof
subjectK (Gly).
The other panels show simulated VLDL triglyceride decay curvesof
reinjectedVLDL
isolatedat
1.5,3.0
and 8.0 hoursaftei the
injectionof
labelled glycerol. Triglyceride decay curvesof
reinjectedVLDL show
presenceof a rapidly turning over
componentin the
VLDLfraction. The
turnover rateof this fast
component correspondsto the
rapid riseof
theVLDL
curve after glycerol.Malmendier and Berman (1973) examined the kinetics
of LDL
apoB
andtriglyceride
simultaneouslyin normal and hyperlipidemic
subjects.
In additionto
showingthat the FCR for
apoB
and triglyceridein LDL
were differentthey
observed, althoughdidn't
discuss,a
complex decay function for reinjectedLDL
triglyceride.Using the LDL
modelin Figure 52 a fit
wasobtained
to
subjectK's LDL
triglyceride specific radioactivity data (Figure 54).G
E ÉÈ
€ uc rto
úc
'EI oÀ
(t)
€0 .E oI d L Er
Glv
15.5 hrs
30
3.0 hrs
30.0 hrs
Hours Hours
Figure 54. Fit of new model (Figure 51) to LDL triglyceride
specificradioactivity data
of
subjectK (Gly). The
other panels show simulated LDL triglyceride decay curvesof
reinjectedLDL
isolatedat 3.0,
15.0 and 30.0 hoursafter the
injectionof
labelled glycerol.Included
in this figure are
simulated curves describingthe
decayof
thereinjected
LDL
triglyceride moiety isolatedat
3.0, 15.5 and 30.0 hours, following injectionof
tabelled glycerol.At
each time (3.0, 15.5 and 30.0 hours) the decaycurve was monoexponential and
its
slope wasthe
same asthat of the
slowlyturning over
LDL R level
compartment (turnover rate=
0.045 h-1). In
subjectH
howeverthe
decay curveof
reinjectedLDL
triglyceride was biexponential in shape(Figure 55). This
biexponential shape \ryasa result of the
markeddifferences
in
the tumover ratesof
theN
andR
levelLDL
compartments (0.187 and 0.040h-l
respectively). The slopeof the
reinjectedLDL
triglyceride curvedecreased between 3.0 and 30.0 hours as label moved from the
N
levelto
moreslowly turning over
R level
compartments.In
additionto the
transferof
labelfrom the N to R level
compartments,label
waslost from the LDL N
levelcompartments as
a
resultof
hydrolysisof
triglyceride. Curve peelingof the
3.0 hourLDL
triglyceride decay curve function would resultin two
functions, thefaster of which
representsthe
summerof the N level LDL
compartments.Unlike
the
turnover ratesof the VLDL N
level compartments,the
turnover rateof the LDL N level
compartments were similarto
thoseof the liver
precursorcompartment.
Gtv 3.0 hrs
1(
3(
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10 15 20 2a 5
0
L5.5 hrs 30.0 hrs
1C
10 15 20
IIours
2a 3( 5 10 15 20 23 3(
Ilours