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Experimental Therapeutics |
Department of Biomedical Engineering [G. K.] and Department of Radiation Oncology [R. D. B., M. W. D.], Duke University Medical Center, Durham, North Carolina 27710
| ABSTRACT |
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| INTRODUCTION |
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To overcome some of the delivery issues seen with in vivo use of many cancer therapeutics, liposomes have been identified as promising carriers for therapeutic agents in the treatment of cancer (4 , 5) . Since their introduction, liposomes have been altered to improve delivery in various ways, including the addition of PEG3 , targeting antibodies, and pH-sensitive polymers (6) . Modification of liposome size has been another method to alter the pharmacokinetics of drug delivery. Size can determine circulation half-life (7, 8, 9, 10, 11) and accumulation site in the body (12) . In the case of drug carriers, size can also influence the delivery volume, release characteristics for drug vehicles (13) , and the accumulation site in the body (liver, tumor, or bone marrow; Ref. 14 ). Ultimately, these factors make particle size an important factor in determining the efficacy of a cancer therapy (15 , 16) .
HT has been used to modify the local tumor environment to increase liposomal drug delivery to tumors (17) . Although classically viewed as a form of adjuvant therapy to increase the efficacy of radiation and chemotherapy, HT can be applied to augment liposomal drug delivery by increasing tumor blood flow and tumor microvascular permeability. At temperatures of 4143°C, HT has been shown to increase blood flow (18) and oxygenation (19) . HT has also been shown to increase permeability of tumor vessels to antibodies (20, 21, 22, 23) , ferritin (24) , and Evans blue dye (25) . More specifically, HT has been shown to increase liposome permeability from tumor vessels (26) . Extravasation of liposomes and albumin from tumor microvasculature has been explored in the literature (27) , but the effect of HT on enabling and augmenting extravasation in a model where extravasation was initially not possible, especially as a function of size, has not been well defined. We now report experiments in which we investigate the ability of HT to enable and augment extravasation of different size particles, from tumor and normal vasculature. We hypothesized that: (a) HT will augment nanoparticle extravasation from tumor vessels; (b) HT can enable extravasation of nanoparticles into tumor where initially no extravasation occurred; (c) this extravasation will be a function of particle size; and (d) this increased extravasation will be preferentially seen in tumor vessels compared with normal vessels.
| MATERIALS AND METHODS |
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Animal and Tumor Model.
Homozygous NCr athymic nude mice (20 ± 3 g) were
purchased from Taconic (Germantown, NY). Animals were housed in
appropriate isolated caging with sterile rodent laboratory chow and
acidified water ad libitum and a 12-h light/dark cycle. All
protocols were approved by the Duke Institutional Animal Care and Use
Committee. The athymic nude mouse dorsal skin flap window chamber model
was used (30)
. Briefly, titanium window chambers were
surgically placed on the dorsal skin flap of athymic nude mice, and a
small volume (
0.1 mm3
) of tumor tissue (human
ovarian carcinoma; SKOV-3) was implanted in the window chamber. After
1014 days, the tumor was visibly well vascularized and
12 mm in
diameter. This preparation was then used for experiments. For
experiments requiring normal vessels, the same window chamber model was
prepared without tumors implanted and allowed to mature for 1014 days
before experimentation.
The permeability of tumor vasculature to liposomes is dependent on the tumor type (31) . Some tumors have pore cutoff sizes between 400 and 600 nm (29) . After initially screening several tumor types, SKOV-3, a human ovarian carcinoma was found to be highly impermeable to 100-nm liposomes under normothermic conditions. Non-tumor-bearing window chamber vessels were similarly impermeable to 100-nm liposomes under normothermic conditions. Because this tumor represents a limiting case for permeability, it was chosen as the model for this study. It provides a strict model for assaying the ability of HT to enable and increase permeability as well as pore cutoff size in tumor relative to normal vessels.
Experimental Groups.
Each experimental group had six mice. Albumin, 100-nm liposomes, 200-nm
liposomes, and 400-nm liposomes were each tested in tumor-bearing
window chambers at 34°C, the normal s.c. skin temperature of mice
(26)
, and 42°C, a temperature that has been shown
previously to have some effect on liposome delivery (17)
.
Liposomes (100 nm) were also tested for extravasation from normal
vessels in non-tumor-bearing window chambers at 42°C.
Experimental Procedure.
In each experiment, animals were anesthetized with sodium pentobarbital
(80mg/kg; i.p.). The tail vein was cannulated for i.v. injection of
albumin or liposomes during the experiment. The animal was placed on a
temperature-controlled microscopic stage to maintain normal body
temperature throughout the experiment. The window chamber was fixed in
a specially designed HT chamber (32)
that allowed for
visualization of the tumor, whereas the chamber was being heated (to
34°C or 42°C, depending on the experimental group). The window
chamber and tumor were allowed to reach steady-state temperature (
2
min as determined by thermographic imaging) in the HT chamber before
injection of liposomes or albumin. The preparation in the window
chamber was observed with a x20 objective lens. A region in the
preparation with steady blood flow and few obvious underlying vessels
was selected. The images of the selected region were recorded with a
SIT camera (Hamamatsu; C2400-08) connected to an S-VHS video tape
recorder (Mitsubishi; BV-1000). This region was first recorded under
transillumination. Then, under epi-illumination with a filter set for
rhodamine (H546; Zeiss), a background image of the selected region was
recorded before injection of liposomes or albumin. Next, 0.2 ml of
rhodamine-labeled liposomes or albumin was administered i.v. The region
was recorded under epi-illumination intermittently (for 10 s every
2 min) for 60 min after the injection of nanoparticles.
The videotape of the experiment was analyzed with image processing software (NIH Scion Image). The fluorescent light intensities of the entire selected region and representative vascular regions were measured at serial time points. The relative fluorescent light intensities of the vascular and interstitial components were determined as described by Wu et al. (33) . All light intensities were normalized to the initial vascular light intensity in the region after injection of liposomes or albumin. Vascular volumes for all experimental groups were not statistically different. Because the light intensity is proportional to the number of particles present (33) , the data are presented as RTIA or accumulation in this report. RTIA values taken at 60 min are defined as RTIA60.
Statistics.
Changes in RTIA were summarized by averaging data from individual
animals in each group (albumin, 100-nm liposomes, 200-nm liposomes, and
400-nm liposomes at 34°C or 42°C). Statistical significance between
experimental groups (treatment temperatures for each size or different
sizes for same treatment temperature) was determined using the Mann
Whitney U test. Two quantities were regarded as different if
P < 0.05.
| RESULTS |
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10 s
after injection and became stable within
30 s. Throughout the 60-min
observation, the tumor blood vessels retained fluorescent signal (Fig. 1
|
7 nm; Ref. 29
) extravasation was
generally diffuse throughout the time course of the experiment and the
tumor interstitium. It freely accumulated in the tumor interstitium at
34°C (Fig. 2a
0.95. At 42°C
(Fig. 2a
1.45, but was not statistically different from
the RTIA60 seen at 34°C. This suggests that
albumin extravasation is largely independent of the effect of HT. The
accumulation of albumin at 34°C and 42°C did not plateau but rather
appeared to increase linearly throughout the hour experiment.
|
0 (Fig. 1
1.5. Overall at 42°C, the
RTIA60 of albumin and 100-nm liposomes was
similar. The remaining two liposomes sizes (200 and 400 nm) also did
not extravasate significantly at 34°C (RTIA60
0; Fig. 2 and d
0.96. The 400-nm liposomes at 42°C
accumulated to a plateau within 25 min and remained there for the rest
of the experiment, resulting in a RTIA60 of
0.43 (Fig. 2d
Effect of Particle Size on Extravasation.
Although HT enabled extravasation for all sizes
100 nm, the degree of
enhancement was a function of particle size (Fig. 3
). At all sizes, the addition of HT resulted in more accumulation in the
tumor interstitium. At 34°C, extravasation quickly dropped off as
size increased from albumin (
7nm) to the 100-nm liposome and stayed
negligible as liposome size increased. The RTIA60
of albumin was significantly higher than all larger particles at 34°C
(P < 0.005). At 42°C, significant
accumulation was maintained from albumin to 100-nm liposomes and then
decreased as liposome size increased to 200 and 400 nm. Even at 400 nm,
HT still facilitated some significant degree of accumulation over
normothermia. At 42°C, the degree of extravasation between the 100-nm
liposome compared with the 400-nm liposome was significantly higher
(P < 0.02), whereas the differences between
the 100- and 200-nm liposome and the 200- and 400-nm liposome were not
significant.
|
0; Fig. 4
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| DISCUSSION |
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7 nm in diameter, extravasated easily from tumor vessels under
normothermic conditions (Fig. 2a
HT was able to overcome limitations in extravasation of particles and
enabled delivery to the tumor interstitium. At 42°C, the 100-nm
liposomes and albumin had similar RTIA60s, which
were not different from the RTIA60 of albumin at
34°C. From the particle accumulation viewpoint, HT made the two
species functionally equivalent. As the particles got larger in
diameter, the RTIA60s with HT did decrease;
however, the presence of HT always yielded a higher
RTIA60 than normothermia (which was
0 for all
liposome sizes tested). This decrease in RTIA60
for the 200- and 400-nm liposome species may be attributable to
heterogeneity in pore size distribution of the tumor vessels created by
HT. In other words, as the particle species increases in size, a
smaller proportion of these pores in the tumor vessel are large enough
to allow for extravasation, thereby resulting in a smaller
RTIA60.
Differential Effect of HT on Normal Vessel Extravasation.
The SKOV-3 tumor line was used as a limiting case of tumor vessel
impermeability for liposomes because 100-nm liposomes were unable to
extravasate under normothermic conditions (Fig. 2b
). Because
HT (42°C) was shown to overcome this limitation in this tumor, the
next logical step was to study normal vessels and determine whether
there was a difference between tumor and normal vessels at this
temperature. At 42°C, the 100-nm liposomes did not extravasate from
the normal vessels (Fig. 4
). Normal vessels were thus a limiting case
for the effect of HT-induced extravasation for 100-nm liposomes. These
results from the normal vessel experiments show that combination HT and
liposomal therapy could potentially be clinically useful because of the
size specificity of HT-induced liposome extravasation in this model. In
the case of the SKOV-3 tumor, 100-nm liposomes would not significantly
accumulate in the tumor or normal tissue (aside from the
reticuloendothelial system) at normal body temperature. By
administering local HT to the tumor, the 100-nm liposomes would only be
able to extravasate in the heated region. The results from the
experiments using normal vessels and HT show that the normal vessels in
the heated region would not yield significant liposome extravasation
either. This allows for regions of normal tissue that may be heated
during a HT treatment (e.g., deep seated tumors) to
experience minimal toxicity from the liposomal drug. The effect of HT
on the tissue immediately surrounding the tumor is still unknown,
because this tissue may be influenced by cytokines secreted from the
tumor. Overall, the results support the idea that HT can be an
important factor in successful liposomal drug delivery to tumors and
that liposome size can be used as a mechanism for targeting and
modifying the amount of drug delivered when combined with HT.
Possible Mechanisms for HT-induced Nanoparticle Extravasation.
The mechanism behind HT-induced extravasation has thus far been
described as the pore cutoff size. This theoretical concept
schematically facilitates the understanding of the extravasation of
different sized particles from tumor vessels. Mechanistically, the
exact pathways that lead to increased extravasation have not been
determined. There have been many studies and competing theories that
attempt to explain the dominant pathway for particle extravasation.
Functional and structural studies have shown that large pores exist in
tumor vessels that allow nanoparticles to extravasate (3)
.
HT has been shown previously to increase the permeability of the
already hyperpermeable tumor vessels (20, 21, 22, 23, 24, 25)
, but the
mechanism is not well established.
One of the more widely accepted explanations for HT-induced extravasation is the "shrinking" of the endothelial cells as a stress response to heat and subsequent widening of the endothelial cell gaps, allowing for larger particles to extravasate (25 , 26) . The "shrinking" or morphological changes in endothelial cell structure are likely attributable to disaggregation of the cytoskeleton after HT (38, 39, 40) . This phenomenon has been supported in electron microscopic studies (41) .
Modification of tumor blood flow has also been proposed as a possible
mechanism for increased RTIA seen with HT. Mild HT (4042°C) has
been recognized to increase tumor blood flow (18
, 42)
.
This overall increase in blood flow could translate into more
nanoparticles perfusing through tumor vessels, eventually leading to
increased extravasation. Although blood flow was not measured in this
study, no change in vessel diameter or vessel density was noted over
the course of the 1-h experiments. This is most likely because the
tumor was allowed to reach steady-state temperature before injection of
the nanoparticles. Furthermore, an increase in blood flow alone cannot
account for the large change seen in 100-nm liposome
RTIA60 at 34°C and 42°C because most
increases in tumor blood flow attributable to HT have been
520%
(26
, 43)
, not orders of magnitude as seen in Fig. 2b
. Finally, a significant change in blood flow should have
also increased the albumin RTIA60 at 42°C, but
this was not seen.
HT has also been shown to increase intravascular pressure in animal
models (44
, 45)
and patients (46)
. This
increased pressure could translate into a larger driving force across
the vessel wall and result in more extravasation of nanoparticles.
However, increased intravascular pressure cannot account for the
increased extravasation seen with HT in this study because no increased
extravasation was seen with albumin and HT (Fig. 2a
).
Ultimately, all or most of these mechanisms for HT-induced extravasation may be important. The lack of HT-induced change in albumin extravasation makes an increase in pore size the most likely explanation.
Consistency of HT-induced Nanoparticle Extravasation.
The variation in the data among 100-nm liposome experiments at 42°C
(Fig. 2b
) is likely a function of tumor heterogeneity,
vessel heterogeneity, pore size distribution, and liposome size
distribution. As the liposome sizes get larger and/or the pore sizes
get smaller (e.g., normothermia), there is less
extravasation and less variation in the data. This is most clearly seen
in the extravasation of all of the liposomes at 34°C, where the pores
are too small for any extravasation and thus the data are very
consistent. This concept is similarly true in both the 200-nm (Fig. 2c
) and 400-nm (Fig. 2d
) liposome data at 42°C.
As the liposome sizes get larger, only certain pores will facilitate
extravasation and allow for less variation in the data. Thus, for the
smallest particle studied, albumin (Fig. 2a
), the largest
variation in results is expected and seen.
Another consideration in the case of the 400-nm liposomes is the
circulation half-life. Despite the incorporation of PEG in the
membrane, the size of these liposomes results in easy detection by the
reticuloendothelial system and rapid removal from circulation
(7)
. At 42°C, whereas all other liposomes continue to
extravasate over the course of 1 h, the 400-nm liposomes plateau
within
25 min. After 25 min, only
30% of the initial vascular
concentration of 400-nm liposomes remained in circulation (data not
shown). This drop in liposome concentration in circulation reduces the
number of liposomes available for extravasation.
Implications for Drug Delivery to Tumors.
The RTIA60 is a function of both circulation
half-life and tumor vessel permeability. Circulation half-life, in this
set of experiments, is largely modified by particle size. Tumor vessel
permeability is determined by the distribution of pore sizes in the
tumor vessel and the distribution of particle sizes in circulation; the
former is also potentially modified by HT. It has been shown that
particles, such as liposomes, that are too small (<70 nm) or too large
(>300 nm) have a reduced circulation half-life (10
, 47)
.
Optimization of circulation half-life based on size must be tempered by
the optimization for permeability (i.e., the smaller the
particle, the easier it exits the vessel). The maximal
RTIA60 is achieved when the combination of
circulation half-life and permeability is optimized.
Although it would initially appear to be ideal to maximize the RTIA60, the absolute amount of drug delivered to the tumor is the most important factor in determining efficacy. The amount of actual drug delivered is indeed a function of RTIA60, but it is also a function of the internal volume of the drug carrier, a liposome in this case. In the study presented, the 100-nm liposomes at 42°C had the highest RTIA60. Although the 100-nm liposomes had a higher RTIA60 than the 200-nm at 42°C, the 100-nm liposomes may not actually deliver more drugs to the tumor because of the smaller internal volume. It must be remembered that a 200-nm liposome could have an internal volume that is an order of magnitude higher (depending on the thickness of the membrane) than that of a 100-nm liposome. Thus, the final efficacy for a liposomal treatment is likely to be a function of the product of accumulation and internal volume.
Using HT as the modality for targeting delivery to tumors has several
other advantages. Comparable temperatures (
4243°C) have been
shown to trigger drug release from specially designed thermosensitive
liposomes (48, 49, 50, 51)
, making it possible to release liposome
contents as desired. With a known tumor location, using HT to target
and trigger drug release may be advantageous over other methods that
require some inherent property of the tissue (pH or certain specific
surface antigens), because it is controlled by external means and thus
more easily modified to the desired conditions. In addition,
preclinical data have indicated that several cancer chemotherapeutic
agents in combination with HT have supra-additive cytotoxic effects
(52
, 53)
. Lastly, besides targeting and triggering release
in liposomes, HT itself has been shown to be directly cytotoxic
(54)
. The therapeutic benefits from liposomes and HT
individually, coupled with the potential advantages seen by their
combination, make the use of the two modalities together an attractive
method for drug delivery to tumors.
| ACKNOWLEDGMENTS |
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| FOOTNOTES |
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1 This work was supported by Grant CA40355 from
the NIH and a grant from the Celsion Corporation. ![]()
2 To whom requests for reprints should be
addressed, at Duke University Medical Center, Department of Radiation
Oncology, Box 3455, Duke University Medical Center, Durham, NC 27710. ![]()
3 The abbreviations used are: PEG, polyethylene
glycol; HT, hyperthermia; Rho-PE, rhodamine labeled
phosphoethanolamine; RTIA, relative tumor interstitial amount;
RTIA60, relative tumor interstitial amount at 60 min. ![]()
Received 3/ 7/00. Accepted 6/20/00.
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