Atherosclerosis and Lipoproteins |
From the Atherosclerosis Research Unit, King Gustaf V Research Institute (C.S.-A., A.H., F.K.), and the Department of Emergency and Cardiovascular Medicine (U.d.F., A.H., F.K.), Karolinska Hospital, and Institute of Environmental Medicine, Division of Cardiovascular Epidemiology, Karolinska Institute (U.d.F.), Stockholm, Sweden; and Center for Medical Ultrasound, Division of Vascular Ultrasound Research, Wake Forest University School of Medicine, Winston-Salem, NC (R.T., M.G.B.).
Correspondence to Camilla Skoglund-Andersson, King Gustaf V Research Institute, Karolinska Hospital, S-171 76 Stockholm, Sweden. E-mail camilla{at}instmed.ks.se
| Abstract |
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Key Words: intima-media thickness atherosclerosis low-density lipoprotein subfractions gradient gel electrophoresis apolipoprotein B
| Introduction |
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Cross-sectional studies have consistently demonstrated the importance of LDL heterogeneity in coronary heart disease (CHD).17 18 19 20 21 In addition, results of recent prospective studies indicate that a small LDL particle size predicts CHD.22 23 24 However, the association between LDL particle size and CHD risk has been independent of the plasma triglyceride level only when a quantitative variable has been used to describe LDL particle size distribution.22 24 25
A number of methods have been developed to characterize LDL heterogeneity. Density gradient ultracentrifugation (DGUC) of plasma26 27 or isolated LDL1 8 28 has been commonly used to separate the LDL particle spectrum according to density. An advantage of the ultracentrifugation techniques is the possibility for compositional studies of LDL subfractions. Nondenaturing polyacrylamide gradient gel electrophoresis (GGE), on the other hand, separates LDL according to particle size, is fairly easy to perform, and has been extensively used in clinical studies. GGE has been reported to enable separation of as many as 7 discrete subclasses within the LDL population.29 However, the qualitative nature of the GGE method is a disadvantage in its current application, because a protocol for quantification of LDL subspecies has not been established. Typically, LDL particle size distribution has been categorized into 2 patterns, A and B,30 and the peak particle diameter has been the sole quantitative estimate.
B-mode ultrasound examination of the common carotid artery (CCA) enables measurement of its size and the width of the vascular wall components. An increased CCA intima-media thickness (IMT) is considered a good surrogate marker of early atherosclerosis. Furthermore, it has been shown to correlate significantly with the presence of coronary artery disease (CAD) and to predict coronary events.31 32 33 34 Factors suggested to influence CCA IMT are age, smoking, hypertension, LDL cholesterol concentration, and postprandial lipemia.35 36 37 38 In accordance with its clinical benefit, lipid-lowering treatment also retards progression of CCA IMT.39 40 41 Recently, the common apoE polymorphism was shown to have an effect on carotid atherosclerosis.42 43
The purpose of this study was to investigate the relation between LDL particle size distribution and IMT of the CCA in healthy, 50-year-old men. A 3% to 7.5% polyacrylamide gradient gel in which separation of LDL particles is achieved with high resolution was developed, as was a procedure to quantify the apoB mass of defined LDL subfractions.
| Methods |
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Blood Sampling
Venous blood samples were drawn into precooled sterile tubes
(Vacutainer, Becton Dickinson) containing
Na2-EDTA (final concentration, 4 mmol/L),
and plasma was immediately recovered by low-speed
centrifugation (1.750g, 20 minutes, +1°C).
PMSF (10 mmol/L, dissolved in isopropanol) and aprotinin (1.4
mg/mL; Trasylol, Bayer) were immediately added to the isolated plasma
to final concentrations of 10 µmol/L and 28 mg/mL,
respectively.
Major Plasma Lipoproteins
Fasting plasma concentrations of cholesterol and
triglycerides in VLDL, LDL, and HDL were determined by a
combination of preparative ultracentrifugation,
precipitation of apoB-containing lipoproteins, and lipid
determinations.44 ApoE genotype was determined as
described elsewhere.45 46
Subfractionation of ApoB-Containing Lipoproteins and Determination
of ApoB Content
Large and small VLDL (Svedberg flotation rate, 60 to 400 and 20
to 60, respectively), IDL, and LDL fractions were isolated by
DGUC.47 The content of apoB-100 in the VLDL subfractions
and IDL was determined by analytical SDSpolyacrylamide gel
electrophoresis.47 Total VLDL apoB-100 concentration is
the sum of apoB-100 content in the small and large VLDL subfractions.
LDL for GGE was isolated from plasma by a single-spin DGUC procedure
according to the method of Redgrave and Carlson48 with
modifications. After a 16-hour spin at 40 000 rpm and 15°C (Beckman
SW40), the top 0.5-mL layer was aspirated (VLDL). The tube was then
sliced 57 mm from the top to harvest the fraction (density, 1.006
to 1.061 kg/L) containing both IDL and LDL. The protein concentration
of the isolated fraction was determined according to the method of
Lowry et al49 after addition of SDS to the reagent mixture
to clear turbidity. Aliquots of isolated LDL were then stored at
-80°C after addition of one-fifth of the volume of sucrose (50%
wt/vol), NaCl (0.15 mol/L), and EDTA (0.24 mmol/L, pH
7.4)50 until later GGE analysis.
Nondenaturing Polyacrylamide GGE of LDL
Gel Casting
Polyacrylamide gradient gels were cast using a 2-chamber
gradient mixer (GM-1, Pharmacia-LKB). The gels consisted of a short
3.0% stacking gel (Acrylamide, BioRad Laboratories),
followed by a linear 3.0% to 7.5% acrylamide gradient.
Ammonium persulfate (10% wt/vol) was added to the
acrylamide solutions to attain a polymerization time of 90
minutes. The gel casting cassette (Hoefer Scientific) prepared for 10
gels (1.5-mm spacers, 10-well combs) was filled from the bottom with 20
mL of a 3% acrylamide solution (acrylamide,
29.25 g/L; bisacrylamide, 0.75 g/L; Tris, 0.375 mol/L, pH
8.35; Temed, 0.9 mL/mL; and ammonium persulfate,
0.4 g/L; prepared
on ice). Then, 44 mL of the 3% acrylamide solution and 44
mL of a 7.5% acrylamide solution (acrylamide,
73.125 g/L; bisacrylamide, 1.875 g/L; Tris, 0.375 mol/L, pH
8.35; Temed, 0.6 mL/mL; and ammonium persulfate, 0.2 g/L; prepared on
ice) were poured into the 2 chambers of the gradient mixer. The
acrylamide gradient was formed by allowing the gradient
mixture to fill the gel casting cassette from the bottom by hydrostatic
pressure during 10 to 15 minutes. When the gradient had been formed, 27
mL of 50% (vol/vol) glycerol was added manually, displacing the
gradient upward into the cassette. The glycerol was added slowly with a
syringe, taking extreme care to keep a constant flow and to avoid any
stirring of the gradient. A grain of methyl green was added to the
glycerol solution to observe any perturbation in the interface. Gels
were then left to polymerize at room temperature for at least 2 hours,
after which they could be stored under moist conditions at +4°C for
no longer than 2 weeks.
Electrophoresis
The vertical slab gels were run in the Hoefer Mighty Small II
apparatus equipped with an EPS 500/400 Pharmacia-LKB power
supply. Preelectrophoresis (60 minutes at 50 V) and electrophoresis
were performed by using Tris (180 mmol/L), boric acid (160
mmol/L), and Na2-EDTA (6 mmol/L pH 8.35) as
running buffer with cooling from a thermostatic circulator (Multitemp
II, Pharmacia-LKB) set at 10°C. To avoid smearing, low-melting-point
agarose (final concentration, 0.4% wt/vol) was added to the sample
immediately before application on the gel. A total volume of 25 µL of
sample, containing
3 µg of LDL protein, was applied to each well.
Reference proteins were run in 2 lanes on each gel. Wells closest to
the edges of the gel were not used. Electrophoresis was conducted at 50
V for 60 minutes, followed by 100 V for 20 hours.
Gels were stained for protein (Coomassie) in glass petri dishes using a newly filtered solution of 0.04% Coomassie Brilliant Blue G-250 (Serva) in 3.5% perchloric acid for a minimum of 3 hours. Gels were then destained in 7% acetic acid for 20 hours with 1 change of destaining solution.
Reference Proteins
Four calibration standard size reference proteins or
lipoproteins were used. The largest was a Lp(a) species, which was
isolated by sequential overnight ultracentrifugation at
densities of 1.055 and 1.080 kg/L and 50 000 rpm in a 50.3 Ti rotor
(Beckman Instruments)51 and characterized as follows. The
purity of the fraction was verified by its pre-ß mobility during
agarose gel electrophoresis and subsequent lipid
staining.52 Scanning of the gel showed that >80% of the
stainable material was confined to the pre-ß region, whereas the
remaining stainable material was in the ß region. An isolated LDL
sample was also used as a size reference and as a distribution pattern
reference for rapid estimation of running quality and reproducibility.
The Lp(a)-containing fraction and the isolated LDL sample were dialyzed
against 1% ammonium bicarbonate and thereafter subjected to electron
microscopy (Philips EM 400) using a negative stain (1% phosphotungstic
acid, pH 8.5) at x60 000 magnification. The particle diameter of the
respective fraction was measured in a dehydrated state. The micrograph
was photographically enlarged 5 times. The diameters of 100 particles
were then determined on each micrograph. The calculated mean diameter
of the Lp(a) particles was 25.1±1.9 nm (n=200). For the LDL sample,
115 particles were measured, and mean particle size was 23.5±1.1 nm.
The LDL sample was further characterized by DGUC27 to
establish the LDL density profile. Aliquots of the Lp(a) fraction and
LDL sample were mixed with the sucrose-containing buffer previously
described, kept frozen at -80°C, and thawed immediately before
application on the gel.
The smaller reference proteins were thyroglobulin (Pharmacia-LKB) and its dimer. The hydrated sizes of thyroglobulin and its dimer were calculated to be 17 and 21.4 nm, respectively.53
Densitometry and Determination of LDL Particle Size
Gels were scanned by a laser densitometer (Ultroscan XL,
Pharmacia-LKB) linked to a personal computer, and the area under the
absorbance curve (AUC) was calculated automatically with use of Gelscan
XL software (Pharmacia-LKB). Before scanning, an OH film with a
straight black line was placed on top of the gel to align the line to
the bottom of the wells. The migration distance of each sample was
calculated from the position of the straight line. Every absorbance
value along the distance from the line to a point slightly beyond the
peak of the thyroglobulin monomer corresponded to a migration distance
in millimeters. The AUC was calculated across the LDL particle size
range. On the basis of the linear gradient profile of the gel, a linear
regression analysis was conducted on the relative migration
distance of the reference proteins on the gel and their respective
sizes. The regression line was calculated for each gel and was used to
convert migration distance of the LDL samples into LDL particle
diameter size, to determine major peak size, and to calculate borders
between subfractions. The mean correlation coefficient for the
relationship between the migration distance and size of the standard
references from 10 consecutive runs was 0.998±0.0015.
Definition of LDL Subfractions
After LDL was separated from pooled plasmas by use of an
equilibrium DGUC procedure described by Chapman et al,8
density-defined subfractions were collected and subjected to GGE along
with the standard size reference proteins. The density profile of the
ultracentrifugation gradient was controlled by
replacing LDL with a salt solution (1.040 kg/L). The density-defined
subfractions were then recovered, and the density of each fraction was
determined with use of a precision densitometer (Paar, DMA 60). After
the isolated LDL subfractions were evaluated, the LDL particle sizes of
the respective density subfractions were measured by using the GGE
method. Major peak sizes of the DGUC fractions were plotted against
fraction densities (Figure 1
) and were
thereafter used to convert density cutoffs into LDL particle sizes on
the gel. Boundaries of the total LDL particle size interval were
defined as 21.0 nm>LDL particle diameter>27.0 nm. Size cutoffs were
set at 25.0 nm (corresponding to
1.030 kg/L), 23.5 nm (
1.040
kg/L), and 22.5 nm (
1.050 kg/L). Subsequently, 4 LDL subfractions
were defined: LDL-I (27.0 to 25.0 nm,
1.006 to 1.030 kg/L), LDL-II
(25.0 to 23.5 nm,
1.030 to 1.040 kg/L), LDL-III (23.5 to 22.5 nm,
1.040 to 1.050 kg/L), and LDL-IV (22.5 to 21.0 nm,
1.050 to 1.060
kg/L). The density cutoff for small, dense LDL (1.040 kg/L) was
originally defined by Krauss and Burke2 and has been used
to relate LDL heterogeneity to severity of
CAD.18 LDL particle size distribution was expressed with
use of the defined size cutoffs, and the resulting subfractions were
denoted LDL-I to LDL-IV, from the largest to the smallest particle
size. The relative AUC for stainable material within each LDL
subfraction was calculated by the software. Three different
parameters reflecting LDL particle size distribution were
derived from evaluation of the gel: (1) The major peak size (nm)
denotes the particle size of the predominant peak (corresponds to PPD);
(2) the relative distribution fraction shows the fraction of the total
AUC accounted for by each LDL subfraction; and (3) the plasma LDL
subfraction concentration was quantified by multiplying the total LDL
protein concentration by the relative distribution fraction.
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To examine the stoichiometry for Coomassie binding between different subfractions of LDL, purified subfractions were isolated by DGUC8 and subjected to electrophoresis on the 3% to 7.5% gradient gel. Total AUC (21.0 to 27.0 nm) of the density subfractions, along with cholesterol, triglyceride, and protein content, was measured.
The reproducibility of the GGE procedure was estimated by calculating within-subject variation. LDL samples obtained from 61 subjects on 2 occasions were evaluated, and the difference between measurements was plotted against the subject mean. Absence of correlation between the 2 indicated that the standard deviation was independent of the measurement and therefore that the coefficient of variation (CV) was not an appropriate representation of measurement error. The within-subject standard deviation was 0.033 for the relative distribution of LDL-I, 0.041 for LDL-II, 0.037 for LDL-III, and 0.017 for LDL-IV. The within-subject standard deviation for major peak was 0.14 nm (CV, 0.006).
CCA Ultrasound Examinations
IMT was measured essentially according to the ultrasound
protocol of the European Lacidipine Study on
Atherosclerosis54 and included 2
components, the scanning and reading procedures. Two certified
ultrasonographers performed the scanning, with subjects in the supine
position with the head slightly turned from the sonographer. The
ultrasound device used was a Biosound 2000 II S.A. (Biosound Inc) with
an 8-MHz high-resolution annular array scanner. The far and near walls
of the right and left CCA were scanned in the anterior, lateral, and
posterior angles. Scanning was recorded on S-VHS videotapes, which
were sent to the Center for Medical Ultrasound, Division of Vascular
Ultrasound Research, Wake Forest University, Winston-Salem, NC, for
reading. IMT was estimated by measuring the linear distance,
perpendicular to the luminal axis, between 2 points defined by the
ultrasonic interfaces, which indicate the boundary between the lumen
and intimal surface and the boundary between the medial-adventitial
interface. CCA IMT was calculated as the mean of the right and left CCA
far-wall IMT. Measurements of IMT in the bifurcation and internal
carotid artery were not used in this report. All subjects were
routinely scanned twice on the same occasion by the same sonographer to
evaluate intrasonographer reproducibility. To evaluate intersonographer
reproducibility, the 2 sonographers each scanned, on the same occasion,
all subjects appearing during 1 month at 6-month intervals.
Intrasonographer CVs were 3.8% and 5.1%. The intersonographer CV was
4.7%.
Statistical Analysis
Statistical calculations were performed by using JMP software
(SAS) for Macintosh. Deviation from normality was tested by using the
Shapiro-Wilk W test. If logarithmic transformation did not
normalize the variable, nonparametric tests were used.
Not once did nonparametric test results deviate from those
obtained with log10-transformed variables.
The distribution of continuous variables was
represented by the median and interquartile range.
Associations between parameters were determined by linear
regression analysis, and results are shown as correlation
coefficients (r). Variables showing a statistically
significant univariate association with CCA IMT were
included in the multiple stepwise linear regression analysis.
An F value of 4.0 was entered in the forward stepwise regression
model.
| Results |
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LDL heterogeneity characteristics of the 94 subjects
are described in Table 2
. The
LDL-II subfraction (23.5 to 25.0 nm) comprised
50% of total LDL,
and the major peak was most often found within this subfraction (Table 2
). The greatest
heterogeneity was seen within LDL-III (22.5 to 23.5
nm), which constituted 22% (16% to 33%) of total LDL. Only a small
portion (5%) of the LDL particles were contained in the LDL-IV
subfraction (21.0 to 22.5 nm). Descriptive statistics of the CCA IMT
along with plasma lipids and major lipoproteins are reported in Table 3
.
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Relations Between Major Plasma Lipoproteins and LDL Particle
Size Distribution
Relations between the major plasma lipoproteins and LDL particle
size distribution are shown in Table 4
. As expected, the major peak
size was inversely related to VLDL triglycerides
(r=-0.63, P<0.001) and positively related to
HDL cholesterol (r=0.50, P<0.001).
An inverse correlation was also seen between VLDL
triglycerides and the fraction of total LDL contained in
LDL-II, with a reciprocal positive relation to HDL
cholesterol. These relations were reversed for LDL-III. The
LDL-IV subfraction was not significantly correlated with any major
plasma lipoprotein fraction. When actual plasma concentrations of LDL
subfractions were related to plasma concentrations of major
lipoproteins, the pattern changed slightly. As expected, all LDL
subfractions were now associated with LDL cholesterol.
Plasma concentrations of the LDL subfractions containing
smaller-particle species (LDL-III and -IV) were also strongly and
positively correlated with VLDL triglycerides and inversely
related to HDL cholesterol. In contrast, plasma levels of
LDL subfractions containing larger-particle species (LDL-I and -II)
correlated only with the plasma concentration of LDL
cholesterol.
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Major Plasma Lipoprotein and LDL Subfraction Correlations With
CCA IMT
Linear regression analysis was used to determine the
relations of plasma lipids and lipoprotein lipids to CCA IMT (Table 5
). Of the lipid variables, plasma cholesterol
showed the strongest correlation with CCA IMT (r=0.29,
P<0.01). This correlation was accounted for by the
association between LDL cholesterol and CCA IMT
(r=0.24, P<0.05). Plasma
triglycerides (r=0.25, P<0.05) as
well as VLDL triglycerides (r=0.24,
P<0.05) were also significantly related to the CCA IMT. In
contrast, plasma concentrations of apoB-100 in the VLDL and LDL
fractions were not significantly associated with CCA IMT, whereas IDL
apoB-100 was. Neither BMI, systolic blood pressure (SBP), nor
diastolic blood pressure (DBP) correlated significantly
with CCA IMT.
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Major LDL peak size was strongly inversely related to the IMT of the
CCA, suggesting that a predominance of small LDL particles is
associated with an increased IMT (Table 6
). The relative distribution of
larger-particle LDL species (LDL-I and -II) was negatively related to
IMT, but when the actual plasma concentrations of these LDL
subfractions were considered, only that of LDL-I remained significantly
associated (r=-0.32, P<0.01) with IMT. Of the
smaller-particle LDL species, the major fraction (LDL-III) was strongly
and positively associated with CCA IMT, and this relation persisted
when the plasma concentration of this subfraction was considered
(r=0.42, P<0.001). Relations between quartiles
of LDL-III plasma concentration and CCA IMT are depicted in Figure 4
. The opposite relations of large- and
small-particle LDL to CCA IMT likely explain the relative weakness of
the LDL cholesterol association with IMT.
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Multivariate Analysis
Multiple stepwise linear regression analysis was performed
to identify independent determinants of CCA IMT. Variables that
were significant in univariate analyses were used
as independent variables in multivariate
analyses. These variables included LDL
cholesterol, VLDL triglycerides, IDL apoB-100,
and the plasma concentration of the major LDL subfraction containing
smaller-particle LDL species (LDL-III), which was included as the
single measure of LDL particle size distribution in the
multivariate model. In the multivariate
forward stepwise model (model A, Table 7
), LDL-III was the first
variable to enter, contributing 19% to the variation in CCA IMT.
Once LDL-III had entered, none of the other lipoprotein or
apolipoprotein variables remained significantly related to CCA IMT.
In model B, VLDL triglycerides was first forced to enter
(r2=0.06), and stepwise forward
progression subsequently allowed LDL-III to enter the model
(r2=0.13), followed by LDL
cholesterol. Finally, in model C, VLDL
triglycerides, LDL cholesterol, and IDL
apoB-100 were forced to enter the model. Together they accounted for
10% of the variation in CCA IMT, which indicates a substantial degree
of interaction between these variables. Nevertheless, LDL-III
entered the model and increased the value of
r2 by 0.10. This indicates that the
plasma concentration of LDL-III correlates significantly and
independently with CCA IMT in healthy, middle-aged men. Using total
cholesterol and total triglyceride
concentrations instead of LDL cholesterol and VLDL
triglycerides did not change the outcome of the
multivariate analysis.
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| Discussion |
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Although the metabolic origin of small, dense LDL is not fully understood, the distribution of LDL particle size in human plasma is believed to be the result of the coordinated actions of hepatic and endothelial lipases as well as mediators of neutral lipid exchange. One current hypothesis25 55 is that the large, light LDL particles are direct products of the action of lipoprotein lipase on small VLDL species (VLDL2). In contrast, small, dense LDL particles are believed to arise through the exchange of cholesteryl esters for triglycerides, between LDL and large VLDL (VLDL1), mediated by the cholesteryl ester transfer protein, producing triglyceride-enriched LDL particles, which are then lipolyzed by hepatic lipase. This metabolic relation can, in part, explain the strong correlation between triglyceride levels and the plasma concentration of small, dense LDL particles.
In our study, the strongest correlation with CCA IMT was found for LDL-III. In the multivariate analysis, the plasma concentration of LDL-III accounted for 19% of the variation in CCA IMT, and after LDL cholesterol, VLDL triglycerides, and IDL apoB-100 were forced into the model, this specific LDL subfraction still accounted for 10% of the variation in CCA IMT.
The present method separates LDL particles with high resolution and enables quantification of subtle differences in the LDL particle size distribution pattern between individuals. In the majority of previous clinical studies, evaluation of LDL heterogeneity was based on qualitative classification of LDL particle distribution.21 It is our opinion that the dichotomization of the LDL particle size distribution into subclass patterns A and B limits the information to be gained from studies of the LDL heterogeneity trait.
The most common procedure for separating LDL particles by GGE uses the Pharmacia PAA 2/16 gel. This gel has been useful for obtaining a crude estimate of the LDL particle size distribution pattern. However, because of the steep progression of the polyacrylamide gradient, the resolution of the LDL particle size spectrum is relatively poor in comparison with ultracentrifugation techniques. In this regard, our protocol provides an improved resolution due to the very slow progression of the polyacrylamide gradient. The cutoffs for defining individual LDL particle size subfractions were derived from densitometric analyses of LDL particle distribution.2 Although conversion of the LDL subfraction density to LDL particle size is approximate, the LDL subfractions obtained by this procedure proved to be appropriate.
A couple of points pertaining to determination of LDL particle size require consideration. The commonly used latex beads56 could not be used as a reference marker in our procedure because they either did not enter the gel or failed to focus on the gel. The variation in size of latex beads seems to be too wide for a slowly inclining polyacrylamide gradient. Instead, the particle size of an isolated Lp(a) fraction was determined by electron microscopy, and the Lp(a) sample was then used as the largest reference protein. The advantage of using Lp(a) as a reference marker is its resemblance to LDL in structure and particle size (corresponds to the size of the largest IDL or LDL particles). The disadvantages are difficulties with stability and standardization, which were avoided by freezing large batches of well-defined Lp(a) at a high sucrose concentration.50 We also used a carefully characterized LDL preparation (electron microscopy to establish the size of the most abundant particle and DGUC to establish the LDL density profile of the sample) as a reference marker. This had several advantages. First, the LDL sample constituted a fourth point on the standard curve, which therefore became more stable and reliable. Second, after the lane containing the reference LDL sample was evaluated, the quality and applicability of the run could quickly be determined. Together, these factors, along with standardized procedures for staining, destaining, and evaluation, contributed to the creation of a highly reproducible GGE procedure. Use of a different set of reference markers, isolated samples of Lp(a) and LDL (measured by electron microscopy in a dehydrated state) and the absence of the formerly used latex bead (which is very large, artificial, and incompressible) explain why our estimated lipoprotein diameter sizes are somewhat smaller than those reported from earlier studies based on GGE techniques.2
The results of this study suggest that the plasma concentration of LDL-III (particle size 22.5 to 23.5 nm) is independently related to CCA IMT in a homogenous group of healthy, 50-year-old men with a fairly narrow IMT distribution (0.59 to 1.19 mm). Of the major lipoproteins, only VLDL triglycerides, LDL cholesterol, and IDL apoB-100 related significantly to the CCA IMT and together explained 10% of its variation, which is in agreement with results of an earlier study.57 In our GGE procedure, an LDL sample of density 1.006 to 1.063 kg/L is applied to the gel. Hence, the LDL subfraction containing the largest particles (LDL-I; particle size, 25.0 to 27.0 nm) is likely to contain IDL particles. Results of a recent study58 indicated that IDL is associated with progression of atherosclerosis, measured as an increase in CCA IMT. In our study, the IDL apoB-100 concentration was associated with CCA IMT in univariate analysis but failed to contribute to the variation in IMT independently of LDL cholesterol and VLDL triglycerides.
It is likely that the linear relationship between plasma levels of small LDL particles and CCA IMT would not have been detected if a method with less precision had been used to determine the LDL particle size distribution. GGE methods have been used in several studies to investigate LDL peak particle size in relation to the presence of CAD,17 20 but a graded relationship between LDL particle size and the extent of atherosclerosis assessed by coronary angiography has not been detected. This could be due to the fact that once CAD is present, several mechanisms contribute to the development of the atherosclerotic lesions and that the relative contribution of the small LDL species is difficult to disentangle. An alternative explanation could be that the relation between LDL particle size and CAD depends on the quantity of a particularly atherogenic LDL species and that a more sensitive method of measuring LDL particle size distribution is needed to demonstrate such a relation. However, coronary angiography and ultrasonographic measurement of carotid IMT are 2 principally different methods of measuring vascular lesions and are likely to reflect different stages of the atherosclerotic process.
Our results suggest that the small, dense LDL particle species could play an important role in causing vascular change, leading to atherosclerosis, and indicate that the evaluation of LDL particle size distribution with a high-resolution GGE method may be a valuable approach to estimating the plasma levels of particularly atherogenic LDL species in asymptomatic individuals.
| Acknowledgments |
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Received October 23, 1998; accepted February 17, 1999.
| References |
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