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Departments of
1
Clinical Chemistry and
2
Endocrinology, Research Institute for Endocrinology, Reproduction and Metabolism, Academic Hospital Vrije Universiteit, P.O. Box 7057, 1007 MB Amsterdam, The Netherlands.
a Author for correspondence. Fax 31-20-4443895.
| Abstract |
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| Introduction |
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Several mechanisms have been postulated to explain the increased atherogenicity of small LDL. Studies on the interaction of LDL with cultured human fibroblasts indicate that small LDL has a reduced affinity for the LDL receptor compared with LDL of normal size, leading to an increased residence time in plasma (11)(12)(13). This could lead to an enhanced interaction of small LDL with the arterial wall. Oxidation of LDL in the subendothelial space of the arterial wall is thought to play a key role in the pathogenesis of atherosclerosis (14)(15). Recent studies have indicated that small, dense LDL is more readily oxidized than larger buoyant LDL (16)(17). In addition, small LDL may more easily penetrate the arterial wall (18)(19) and has been shown to have increased interaction with arterial wall proteoglycans (20).
A widely used technique for the measurement of LDL size is gradient gel electrophoresis (GGE) (21)(22). However, this method is rather laborious. Ultracentrifugation (23), dynamic light scattering (24), and electron microscopy (EM) (25) can also be used for characterization of LDL particles by size and shape. These techniques are less suitable for larger series. To realize a high throughput of samples, an automated procedure is desirable.
Several reports discuss the use of gel-filtration chromatography to separate lipoprotein particles according to their size (26)(27)(28)(29)(30)(31)(32). The column effluent is collected in fractions for subsequent cholesterol and TG measurements (28)(31)(32), or lipoproteins are detected on-line after postcolumn derivatization with cholesterol reagent (29)(30). Lipoprotein classes can thus be quantified.
Here we report on a procedure for LDL size measurement by high-performance gel-filtration chromatography (HPGC) after LDL isolation by ultracentrifugation. LDL was isolated from the plasma of 60 NIDDM patients with plasma TG in the range of 0.55.6 mmol/L. LDL particle diameter obtained by HPGC was compared with values obtained by polyacrylamide GGE. In addition, we present data on the relation between size and composition of the LDL particle.
| Materials and Methods |
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Plasma total cholesterol (TC), HDL cholesterol, and TG were determined on fresh samples. Plasma aliquots, containing sucrose (final concentration 6 g/L) as cryoprotectant, were stored at -70 °C for LDL size and composition measurements.
chemicals
Thyroglobulin (T-1126), apoferritin (A-3641), and dithiothreitol
(D-0632) were purchased from Sigma. Bovine serum albumin was from
Pierce. All chemicals used in solvents and buffers were from Merck and
were analytical grade.
ldl isolation
Ultracentrifugation was carried out in a Beckman Optima-TLX
preparative ultracentrifuge with a fixed-angle type 100.4 rotor.
Acceleration mode 6 and deceleration mode 6 were used. LDL was isolated
from plasma between d 1.019 and 1.063 kg/L on the basis of
the method described by Havel et al. (35) with some
modifications. Briefly, the density of 0.9 mL of plasma was adjusted to
d = 1.019 kg/L by the addition of concentrated salt
solution. Then 2.2 mL of salt solution at d = 1.019 kg/L was
gently layered on top of the density-adjusted plasma by use of a
low-speed peristaltic pump (Pharmacia). After ultracentrifugation at
100 000 rpm (417 000gav) for 1 h 40 min
at 15 °C, the top layer containing VLDL and IDL was discarded. The
infranatant was adjusted at d = 1.063 kg/L and
ultracentifuged at 417 000gav for 5 h at
15 °C. Subsequently, the LDL-containing top layer (~1 mL) was
recovered and stored at 4 °C in the dark.
analytical methods, lipoprotein composition
Samples were analyzed for TC, free cholesterol (FC), TG, and
phospholipids (PL) in enzymatic, colorimetric assays with test kits
from Boehringer Mannheim (cat. nos. 1489232, 310328, 816370, and
691844, respectively). The cholesterol ester (CE) concentration in LDL
was calculated as the difference between TC and FC. Serum HDL
cholesterol was measured after precipitation of the apolipoprotein
B-100-containing lipoproteins with phosphotungstic acid/magnesium
chloride. LDL protein was estimated by the method of Lowry et al.
(36) with some modifications to simplify protein
determination in lipoproteins samples (37). Bovine serum
albumin was used for calibration. The above-mentioned methods were
adapted to the ELAN analyzer.
Lipoprotein(a) [Lp(a)] was measured by rate nephelometry with Beckman reagent (cat. no. 465360) on an Array analyzer.
ldl size calibration samples
Measurement of the LDL particle size was carried out by comparing
the migration distance (GGE) or retention time (HPGC) with two LDL
calibration samples whose molecular diameters were determined by GGE.
In addition, the sizes of the LDL calibrators were confirmed by EM.
LDL calibrator A (large, buoyant) was isolated by ultracentrifugation from the plasma of a young healthy female volunteer with normal plasma TG (0.6 mmol/L), and calibrator B (small, dense) was isolated from the plasma of a male NIDDM patient with increased plasma TG (5.8 mmol/L). Calibrators A and B were stored in aliquots at -70 °C, after the addition of sucrose and EDTA (final concentrations 6 g/L and 0.2 mmol/L, respectively).
The average particle diameters of the calibrator LDL samples were estimated by GGE from a linear calibration curve of the logarithm of the diameter vs the migration distance, with apoferritin (12.2 nm), thyroglobulin (17.0 nm), and thyroglobulin dimer (23.6 nm) as calibrators of known diameter. LDL calibrator A was estimated by GGE at 26.2 ± 0.2 nm and calibrator B at 24.0 ± 0.2 nm.
For EM measurements, LDL calibrators A and B were dialyzed against 10 g/L ammonium acetate buffer containing 0.1 mmol/L EDTA (pH 7.4), negatively stained with methylamine tungstate on copper mesh grids, and examined with a Philips CM 100 Bio electron microscope at a magnification of 135 000 (25). Several enlarged monitor images (final magnification 275 000) of electron micrographs were used to measure the diameter of at least 50 LDL particles. Aggregated particles and particles of abnormal shape were excluded. The diameter was calculated from the measured (by computer) circumference of the LDL particles. LDL calibrator A was estimated by EM at 26.2 nm (0.5 SE) and calibrator B at 23.9 nm (0.3 SE).
hpgc
The HPLC system consisted of a Model 616 pump, Model 486 UV
detector, and Model 717 autosampler from Waters. To avoid deterioration
of LDL samples, the sample compartment of the autosampler was cooled at
7 °C, and sample vials were capped. Millennium 2010 software
(version 2.15) from Waters was used for instrument control and data
acquisition and processing. The mobile phase was continually degassed
with a Degasys Model DG2410 on-line degasser from Uniflows. Separations
were performed on a Superose 6 column (30 x 1 cm) from Pharmacia.
LDL (50 µL) was injected and eluted with phosphate-buffered saline
(PBS; 0.1 mol/L
NaH2PO4 · H2O, 0.2
mol/L NaCl, and 0.1 mmol/L disodium EDTA, adjusted to pH 7.4) at a flow
rate of 0.5 mL/min. The pressure of the HPLC system was ~1725 kPa.
Before use, PBS was filtered through a 0.45-µm filter. The pump was
run in the SILK-mode to smooth the eluent flow by eliminating pressure
pulses and surges. The effluent was monitored at 280 nm at a sampling
rate of 2 Hz for data acquisition. LDL eluted between 20 and 26 min,
and the total run time was 60 min. LDL calibrators A and B were assayed
in each sample set. The retention time of the unknown LDL samples was
used to calculate the LDL particle diameter by linear interpolation.
Some LDL samples were slightly larger than calibrator A or smaller than
calibrator B. The sizes of these LDL samples were calculated by linear
extrapolation. A QC LDL sample stored at -70 °C was also included
in every series of samples. After analysis of a series of samples the
Superose column was washed with 0.1 mL/L Tween and stored in 200 mL/L
ethanol.
gge
Electrophoresis equipment and chemicals were obtained from
Bio-Rad. LDL size was determined by electrophoresis as originally
described by Krauss and Burke (21) and Nichols et al.
(22). Nondenaturing 210% polyacrylamide gradient gels,
10 lanes per gel, were cast in our laboratory according to the method
of Lahdenperä et al. (38) with some modifications.
The MiniProtean II multicasting chamber was used to cast eight
1-mm-thick gels simultaneously. The solutions were made immediately
before casting the gradient. The light monomer solution consisted of
23.5 mL of water, 8.3 mL of 1.5 mol/L Tris-HCl (pH 8.3), 1.8 mL of 40%
acrylamide/bisacrylamide (19:1), 47 µL of 6.6 mol/L
tetramethylethylenediamine, and 135 µL of 50 g/L ammonium persulfate,
and the heavy monomer solution contained 10.7 mL of water, 7.1 mL of
Tris-HCl (pH 8.3), 7.3 mL of acrylamide/bisacrylamide, 25 µL of
tetramethylethylenediamine, 70 µL of ammonium persulfate, and 3.7 mL
of 400 g/L sucrose. Tetramethylethylenediamine and fresh ammonium
persulfate were added immediately before pouring. We used 5 mL of the
light solution as stacking gel. The gradient was generated within 10
min with a Model 385 gradient-former by use of a peristaltic pump. The
gels were left undisturbed for 3 h for polymerization. For
storage, the gels were moistened with TBE buffer (90 mmol/L Tris,
80 mmol/L boric acid, and 3 mmol/L EDTA, adjusted to pH 8.35) and kept
in a tightly sealed container at 4 °C.
The gels were equilibrated in precooled TBE buffer at 100 V for 30 min in a cold room. LDL (30 µL) was mixed with 50 µL of sample buffer [4 mL of 1.5 mol/L Tris-HCl (pH 8.3), 0.5 mL of 1 g/L bromphenol blue, and 2 mL of glycerol], and 20 µL of 1 g/L thyroglobulin was added as internal reference. After a 10-min incubation at room temperature, 10 µL of this suspension (containing ~2 µg of LDL protein) was loaded on the gels. The two outer lanes were not used. LDL calibrators A and B were run on each gel to calibrate for particle size. A QC LDL sample stored at -70 °C was also included in every run.
Electrophoresis was performed by applying voltage to the chamber in the following sequence: 15 V for 15 min, 70 V for 20 min, and 125 V for 24 h. After electrophoresis, the gels were fixed in 100 g/L sulfosalicylic acid for 1 h and stained for protein for 34 h in 0.4 g/L Coomassie Brilliant Blue R-250 in 35 mL/L perchloric acid. Gels were destained in 50 mL/L acetic acid for at least 2 h. After destaining, gels were soaked overnight in 30 mL/L glycerol and dried between two Gelair Cellophane sheets.
The gels were scanned with a Model GS700 imaging computer-assisted scanning densitometer with Molecular Analyst software. The migration distance of each LDL band relative to thyroglobulin was measured. The LDL calibrators A and B were used to calculate the particle diameters of the unknown samples by linear interpolation (39). LDL samples larger than calibrator A or smaller than calibrator B were calculated by linear extrapolation. Some subjects had several bands, but the size of the most predominant LDL subfraction was calculated.
statistics
Throughout the present study, results are expressed as mean
± SD. Pearson's correlation coefficients were calculated to describe
the relationships between variables. Statistical difference was tested
by paired Student's t-test. The value of statistical
significance used in this study was P <0.01. To reduce
skewness, the plasma TG concentrations were transformed to their
natural logarithms before statistical analyses.
| Results |
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hpgc vs gge
The LDL peak particle diameters of 60 NIDDM patients determined by
HPGC were compared with values obtained by GGE. The mean LDL diameter
of the NIDDM patients obtained by GGE and HPGC was 25.27 ± 0.81
and 25.48 ± 0.85 nm, respectively. As shown in Fig. 3
A, the LDL particle sizes estimated by GGE and HPGC were highly
correlated [y = (0.93 ± 0.07)x +
(2.05 ± 1.66); r = 0.88;
Sy|x = 0.41 nm]. However, the results obtained by
HPGC were somewhat, but significantly (P <0.001), higher
than those determined by GGE. To detect the between-method bias for the
LDL size methods under comparison, the absolute difference was plotted
in Fig. 3B
against the mean for each pair of measurements
(40).
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relations between ldl size and plasma lipids and ldl composition
The mean LDL size determined by HPGC and GGE and lipoprotein
composition analyses are shown in Table 2
. The correlation coefficients for the associations between LDL
size and lipid variables are shown in Table 3
. Correlation coefficients between lipid variables and LDL size
as measured by HPGC and GGE were of the same magnitude, but correlation
coefficients were slightly higher for the HPGC measurements. LDL size
showed a positive correlation with HDL cholesterol and a strong inverse
correlation with the logarithm of plasma TG. The association between
LDL size estimated by HPGC and plasma TG is illustrated in Fig. 4
. Small dense LDL particles (
25.5 nm), according to HPGC, were
found only in subjects with plasma TG
1.9 mmol/L. LDL size as
measured by HPGC was strongly correlated with the FC content of LDL and
to a lesser extent with the CE content. We also observed a positive
correlation with LDL-PL, whereas LDL size was not correlated with the
TG content of LDL (Fig. 5
).
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reproducibility
Between-run reproducibility for particle diameter was determined
by repeatedly analyzing an isolated LDL sample stored in aliquots at
-70 °C. GGE and HPGC reproducibility, expressed as CV determined
over an 8-week period, were 0.6% (n = 14) and 0.2% (n =
12), respectively. Within-run imprecision for LDL size measurements was
assessed only for the HPGC method. The CVs for two different samples
were <0.1% (n = 10). To establish the influence of the HPLC pump
on the HPGC reproducibility, we also tested another pump (Gynkotek,
Model 480). With this pump, the within-run imprecision was also
<0.1%.
column-column variation
We analyzed >500 samples with one Superose column (column I). To
verify column variation, we measured LDL size of 20 samples on two
separate HPGC columns. We compared column I with a brand new column
(column II). There was no statistical difference (P =
0.639) between the LDL size measured on column I or II. The mean LDL
size for column I was 25.38 ± 0.91 nm and for column II,
25.37 ± 0.95 nm [y = (1.03 ±
0.03)x - (0.76 ± 0.83); r =
0.99; Sy|x 0.13 nm].
ldl aggregation during isolation
Once isolated, LDL exhibits a tendency to aggregate. Aggregated
LDL can easily be recognized by HPGC, as it elutes at the same time as
VLDL. We stimulated LDL aggregation by vortex-mixing an isolated LDL
sample. Vortex-mixing (30 s) of isolated LDL resulted in a diminished
peak area of the main LDL peak eluting at 23 min, with a concomitant
increase of the peak of aggregated LDL eluting at 15 min. The
calculated LDL size of the native LDL (26.23 nm) was almost equal to
the size of the aggregated LDL sample (26.21 nm), suggesting that mild
LDL aggregation does not seriously affect size determination by HPGC.
interference by idl and lp(a)
LDL used in this study was isolated by dual-spin
ultracentrifugation. After the first ultracentrifuge run, the top layer
contains VLDL and most of the IDL (1.006 < d <
1.019 kg/L). VLDL subjected to HPGC eluted between 14 and 17 min as
illustrated in Fig. 1A
. IDL elutes between VLDL and LDL (~17 min,
data not shown). Hence, it is not likely that the remaining IDL in the
second ultracentrifuge run will affect the position of the LDL peak in
HPGC.
On the other hand, the density of Lp(a) spans both the LDL and HDL
range, with most of the Lp(a) found between 1.050 and 1.100 kg/L. In
patients with substantial amounts of Lp(a) it is likely that LDL
isolated by ultracentrifugation between 1.019 and 1.063 kg/L is
contaminated with Lp(a). To establish the retention time of Lp(a) in
the HPGC system, Lp(a) was isolated by ultracentrifugation between
1.063 < d < 1.090 kg/L from a plasma with a high
Lp(a) content (720 mg/L). As shown in Fig. 6
the retention time of Lp(a) is considerably shorter than that
of LDL. Fig. 6
also illustrates that addition of Lp(a) to LDL resulted
in the appearance of a prominent shoulder on the leading edge of the
LDL peak. However, this addition did not influence the retention time
of the LDL peak. Visual inspection of the LDL HPGC profiles of all 60
NIDDM patients revealed four samples with a leading shoulder, although
much less conspicuous than in Fig. 6
. The presence of substantial
amounts of Lp(a) was corroborated by Lp(a) measurements in the plasma
of these four patients, ranging from 490 to 1030 mg/L. In contrast, the
range of Lp(a) of four plasma samples with HPGC profiles without a
shoulder was 2045 mg/L. The disulfide bridge linking
apolipoprotein(a) and apolipoprotein (apo) B-100 is cleaved when Lp(a)
is incubated with 0.01 mol/L dithiothreitol for 1 h at room
temperature, resulting in a smaller particle very similar to LDL
(41). Addition of dithiothreitol to the four
Lp(a)-containing LDL samples before chromatography resulted in the
disappearance of the shoulder in the LDL profiles. The retention time
of LDL samples, with and without a shoulder, was not influenced by the
addition of dithiothreitol.
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influence of storage conditions of isolated ldl samples
Isolated LDL samples were tested for stability during storage at
4 °C and -70 °C. The LDL sizes measured by HPGC of 9 fresh LDL
samples were compared with those in the same samples after storage for
4 weeks at 4 °C. The mean LDL sizes were 25.37 ± 1.02 and
25.36 ± 0.99 nm (P = 0.814) before and after
storage, respectively. A QC sample stored in aliquots at -70 °C
demonstrated no change in size over a 4-month period.
| Discussion |
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Column-to-column variation for the HPGC method was examined by measuring a series of samples on two different columns. The conclusion was that the LDL size did not depend on the HPGC column.
Within-run CV of LDL size as measured by HPGC was <0.1%. Because LDL size is linearly related to retention time, this means that retention time was reproducible within 0.1%, equivalent to 1.4 s for a retention time of 23 min. To attain this high precision, several instrumental and methodological variables must be carefully controlled. First, the acquisition rate of the data system must be high enough to allow sufficient resolution on this time scale. We routinely use an acquisition rate of 2 Hz, equivalent to a resolution of 0.5 s. Second, a fixed injection volume should be used during the analysis of a series of unknown and calibration samples. Increasing the injection volume leads to an apparent increase in retention time, caused by the sample being introduced on the column as a plug. A 50-µL sample will take 6 s to be flushed from the sample loop onto the column at a flow rate of 0.5 mL/min. With a 100-µL injection volume this time is increased to 12 s, leading to an increased retention time and thus substantial underestimation of LDL size. Finally, pump flow imprecision should be <0.1%. We tested two different pumps that were both sufficiently precise. However, pumps should be tested regularly for flow reproducibility. Between-run CV of the GGE method was 0.6%, in accordance with published values from other laboratories (0.73.5%) (3)(4)(21)(38)(42). Between-run CV for the HPGC method was <0.2%. Therefore, the reproducibility of the HPGC method is at least 3 times better than the GGE method.
As mentioned by Tallis et al. (32), the Superose column has a long lifetime and was in their hands capable of analyzing 300 filtered plasma samples. Loading the HPGC column with isolated LDL, as we did in this study, we observed no deterioration of column performance after >500 injections.
In some patients, LDL shows several peaks (polydisperse LDL) on
polyacrylamide GGE. We calculated the LDL size of the predominant GGE
subfraction. However, with the HPGC technique, LDL eluted as a single
peak (Figs. 1
and 2
), so polydispersity was not observed. LDL size as
measured by HPGC thus represents the weighted average of LDL
subfractions in polydisperse LDL. Because the meaning of polydispersity
is not really understood, we do not consider this as a disadvantage of
HPGC. It may in part explain small differences in LDL size as measured
by both methods.
Several studies have demonstrated that LDL size is inversely associated
with plasma TG and positively associated with HDL cholesterol
(1)(2)(3)(4). The results (Table 3
and Fig. 4
) of our selected
NIDDM patients are consistent with these studies, showing significant
correlations between LDL size estimated by HPGC and plasma TG and HDL
cholesterol (r = -0.84 and +0.50, respectively).
The mechanism by which plasma TG affects LDL size is hypothesized by Lagrost et al. (3). In hypertriglyceridemia, LDL-CE is exchanged for VLDL-TG, mediated by cholesteryl ester transfer protein. Subsequent hydrolysis of LDL-TG by hepatic lipase or lipoprotein lipase results in small, dense LDL particles. Our observation that LDL-TG in subjects with increased plasma TG (2.05.6 mmol/L; n = 34) is inversely associated with LDL-CE (r = -0.56, P <0.001) strengthens this hypothesis.
Correlation studies with LDL size estimated by GGE and HPGC and the LDL
lipid composition gave comparable results (Table 3
). HPGC associations
with LDL lipids are even somewhat stronger. The present study also is
in agreement with the findings by Capell et al. (42) in
showing a significant positive correlation between LDL size estimated
by HPGC and LDL-FC, LDL-CE, and LDL-PL and the absence of a significant
relationship with LDL-TG (Table 3
). The correlation between LDL size
and LDL-PL (Fig. 5
) is strongly influenced by two single samples
with extremely low LDL-PL concentrations (LDL-PL: 0.52 and 0.65 mmol/g
LDL-protein), resulting in a less significant correlation. In contrast,
the LDL-FC concentrations of these two samples were remarkably high
(1.30 and 1.29 mmol/g LDL-protein). FC and PL are primarily located at
the surface of the LDL particle. It can be speculated that in these two
samples the low PL content was by some mechanism compensated by
increased FC concentrations, resulting in a partial conservation of the
total amount of surface lipids.
The relationship between GGE migration distance and particle diameter is gel-specific. Therefore, in each gel two LDL calibration samples and one control sample were included. The two outer lanes were not used, so only 5 places remain for unknown samples. In contrast, the automated HPGC procedure allows the unattended analysis of large series of samples. For example, we routinely analyze series of 64 samples during the weekend.
As mentioned above, LDL calibrators A and B were run on each GGE gel and in every HPGC sample set to calibrate for particle size. Marker proteins, e.g., apoferritin and thyroglobulin, and calibrated latex beads are frequently used in GGE for calibration. To transform the migration distance into the LDL size, lipoprotein particles are assumed to exclude from the gel by the same criteria as the (protein) calibrators (39). Calibration of the HPGC column with these proteins resulted in calculated LDL diameters ranging from 20 to 23 nm. Apparently, the shape of the stretched proteins differs too much from the spherical LDL. This phenomenon has been observed by others as well. For example, in a study by Van Gent and Van Tol (28) a Superose 6 column was calibrated with four proteins of known molecular mass. The molecular mass of LDL was estimated by them at 1.0 x 106 Da. However, the average molecular mass of LDL, calculated by dividing the molecular mass of apo B protein (43) by the protein content (weight percent) is ~2.6 x 106 Da (24). Attempts to calibrate our HPGC column with small (<50 nm) polystyrene latex beads (Duke Scientific) failed because these particles aggregated in PBS and clogged the column.
Lp(a) is structurally very similar to LDL, with an overlapping density and a somewhat greater size (41). Addition of Lp(a) to LDL in various amounts did not influence the retention time of LDL. Furthermore, cleavage of the disulfide bond between apo(a) and apo B in Lp(a) did not alter the retention time of Lp(a)-contaminated LDL samples. Hence, LDL size estimated by HPGC is not affected by Lp(a) in patients with substantial amounts of Lp(a).
Carroll and Rudel (44) showed that varying the elution buffer concentration altered the elution profile of lipoproteins separated by HPGC. They suggested that at low buffer concentration, ion-exclusion effects may prevent lipoprotein particles from entering the pores in the column packing. We obtained comparable results by varying the ionic strength at low buffer concentrations. We found that an ionic strength of 0.4 mol/L is sufficient to obtain stable retention times. The ionic strength of the PBS buffer in the present study was 0.46 mol/L.
We have developed a HPGC-based technique for determination of the mean LDL particle diameter. Values measured by HPGC were in close agreement with values obtained by GGE. Although the HPGC method requires isolation of LDL by ultracentrifugation, we do not consider this as a major drawback, because in clinical studies LDL isolation is frequently required for other measurements as well, e.g., lipid composition and susceptibility to oxidation. In comparison with GGE the main advantages of the HPGC method are its high precision, good reproducibility, and the possibility for the automated analysis of large series of samples.
| Acknowledgments |
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| Footnotes |
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| References |
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