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1 Lady Davis Institute and
3 Division of Nephrology, Previous
studies have shown that renal autoregulation dynamically stabilizes
renal blood flow (RBF). The role of renal nerves, particularly of a
baroreflex component, in dynamic regulation of RBF remains unclear. The
relative roles of autoregulation and mesenteric nerves in dynamic
regulation of blood flow in the superior mesenteric artery (MBF) are
similarly unclear. In this study, transfer function analysis was used
to identify autoregulatory and baroreflex components in the dynamic
regulation of RBF and MBF in Wistar rats and young spontaneously
hypertensive rats (SHR) anesthetized with isoflurane or halothane.
Wistar rats showed effective dynamic autoregulation of both MBF and
RBF, as did SHR. Autoregulation was faster in the kidney (0.22 ± 0.01 Hz) than in the gut (0.13 ± 0.01 Hz). In the mesenteric, but
not the renal bed, the admittance phase was significantly negative
between 0.25 and 0.7 Hz, and the negative phase was abrogated by
mesenteric denervation, indicating the presence of an arterial
baroreflex. The baroreflex was faster than autoregulation in either
bed. The presence of sympathetic effects unrelated to blood pressure
was inferred in both vascular beds and appeared to be stronger in the
SHR than in the Wistar rats. It is concluded that a physiologically significant baroreflex operates on the mesenteric, but not the renal
circulation and that blood flow in both beds is effectively stabilized
by autoregulation.
transfer function; Wistar rats; spontaneously hypertensive rats; autoregulation; baroreflex
IN RATS, arterial baroreflexes operate largely on
peripheral resistance within the frequency band from 0.25 to 0.7 Hz (5, 20). Efferent renal sympathetic nerve activity is coherent with blood
pressure (PA) in a band centered
on ~0.4 Hz (3) and predicts the observed discrete rhythm in
PA at 0.4 Hz (4). Despite this, baroreflexes appear to have relatively small effects on renal blood
flow (RBF) in several species (12, 30). This is perhaps not too
surprising, since operation of baroreflexes to defend PA must introduce fluctuation of
blood flow of the bed being operated on. The kidney has a very strong
requirement for stability of RBF that follows both from the necessity
for high and stable glomerular filtration rate to permit tubular
regulation of sodium excretion and from the sensitivity of the
glomerulus to hypertensive injury. In denervated kidneys, it is
autoregulation that provides this stability, preventing
PA fluctuations slower than ~0.1
Hz from being transmitted to RBF (19). Thus one would predict that
autoregulation should dominate dynamic regulation of RBF in innervated
as in denervated kidneys.
Considerably less is known of the dynamic regulation of blood flow to
the intestine. As in the kidney, mesenteric sympathetic nerve activity
contains a large amount of information related to baroreflexes,
although there is also a substantial somatosensory component (37).
Blood flow through the superior mesenteric artery (MBF) is subject to
autoregulation (26), although both the efficiency and the mechanism of
autoregulation in this bed are subject to debate. Both myogenic and
washout mechanisms have been proposed to explain experimental data
(reviewed in Ref. 21). The requirement for stability of blood flow in
this bed is not as strict as in the kidney because organ function is
not as tightly linked to blood flow and because much larger structural
resistance protects the capillaries from hypertensive damage.
Furthermore, the gut is upstream from the portal circulation, a major
capacitance bed that is subject to control by sympathetic inputs, in
particular baroreflexes (16, 36). Thus it is not clear what control
mechanisms dominate dynamic regulation of MBF. Because this bed
receives a large fraction of cardiac output and because of the large
downstream capacitance, it is likely that baroreflexes contribute
substantially to dynamic regulation of MBF.
Experiments were performed in normotensive rats to compare dynamic
regulation of MBF and RBF; additional experiments were performed in
spontaneously hypertensive rats (SHR) at a time (6-7 wk of age)
when efferent renal sympathetic nerve activity is substantially elevated (12, 27). The relative contributions of autoregulation and
baroreflexes were assessed from changes in the pressure-flow transfer
functions induced by acute denervation of the vascular bed being
studied.
All experiments received approval of the SMBD-Jewish General Hospital
Animal Care Committee and the McGill University Animal Care Officer and
were conducted under the guidelines promulgated by the Canadian Council
on Animal Care. Adult, male Wistar rats (288 ± 57 g, mean ± SD)
and 6- to 7-wk-old male SHR (160 ± 20 g) were obtained from Charles
River (Canada). Rats had free access to food and water until the time
of the experiment.
Anesthesia was induced by isoflurane or halothane at a concentration of
5% in inspired gas (40% O2-60%
air). The animal was transferred to a servo-controlled, heated table to
maintain body temperature at 37°C, intubated, and ventilated by a
constant volume, small-animal respirator according to the Harvard
nomogram (expts 1,
2, and
5) or by a pressure-controlled
respirator operating in respiratory-assist mode (expts
3, 4, and
6). After induction, the anesthetic
concentration was reduced to ~2.5% (isoflurane) or ~1.5%
(halothane). During the postsurgical equilibration period, inspired
anesthetic concentration was titrated to the minimal concentration that
precluded a PA response when the
tail or pinna was pinched. The tail was pinched periodically throughout
the experiment to ensure adequate anesthesia. Anesthetics were
delivered by using calibrated vaporizers in a Boyle circuit modified
for small animals.
Cannulas were placed in a femoral artery (PE-90 with narrowed tip) and
vein (PE-50); the venous line contained a Silastic insert to allow drug
infusion. In experiments 1,
2, and
5, the animal was paralyzed with
pancuronium bromide (Pavulon, Organon, 1 mg/kg + 1 mg · kg Six experiments were performed. Four experiments examined the dynamics
of MBF in Wistar rats under isoflurane (expts
1 and 2,
n = 6 each) or halothane anesthesia
(expt 3,
n = 7) and in SHR under
isoflurane anesthesia (expt 4,
n = 8). RBF dynamics were evaluated in
Wistar rats (expt 5,
n = 7) and in SHR
(expt 6,
n = 6), both under isoflurane
anesthesia. Experiment 1 was a time
control designed to confirm that the observed changes in the
PA-MBF transfer function were
caused by denervation. In the other five experiments, the vascular bed
being examined was denervated after an initial control period.
After a 1-h equilibration, PA and
RBF or MBF were recorded continuously for Femoral arterial pressure was measured by a pressure transducer (HP
1290C) driven by a Stemtech GPA-1 amplifier. Blood flows were measured
by a Transonic Systems T106 transit time ultrasound flowmeter (R1
probe). Blood pressure and flowmeter output were recorded on magnetic
tape (Vetter 420-K) for off-line analysis. Pressure and flow signals
were filtered at 22 Hz and sampled at 48 Hz using 12-bit
analog-to-digital conversion. The two data streams were low-pass
filtered and subsampled to 3 Hz.
Power spectra and transfer functions based on the fast Fourier
transform were computed by using standard algorithms as previously described (1). Data segments of 1,024 s were first subjected to trend
removal by using a 500-point rectangular window with 0.006-Hz cutoff.
Fast Fourier transforms were computed on 512-point segments shaped by
the Hann window with 50% overlap. Transfer functions (magnitude and
phase angle) were calculated separately and employed 128 (MBF)- or 256 (RBF)-point segments, the Hann window, and 69% overlap. Fractional
admittance gain was calculated as magnitude divided by conductance.
Thus gain of >1 means that PA
fluctuations are actually amplified into blood flow as expected from
passive, compliant vessels or from a baroreflex operating on blood flow
to stabilize PA; gain of 1 means
that the vasculature behaves as a stiff tube; and gain of <1 means
that flow is actively being stabilized, for instance by autoregulation.
By convention, a positive admittance phase means that output (blood
flow) leads input (PA) as
expected in a passive or autoregulating system (18). A baroreflex
will produce negative admittance phase because flow follows pressure
after a delay governed by delays in nervous transmission and the
(de)activation kinetics of vascular smooth muscle.
As noted by Holstein-Rathlou et al. (19),
PA is undoubtedly the input to the
system under study. However, either blood flow or "instantaneous"
resistance may be considered to be the system's output.
Pressure-resistance transfer functions often provide information complementary to pressure-flow transfer functions (19, 23). Instantaneous resistance is calculated as pressure/flow at each 0.33-s
sampling interval. Fractional resistance gain is expected to be <1
when the system is behaving passively with respect to PA and Results are presented as means ± SE of original data. Effects of
denervation were assessed by comparing average gain and phase before
and after denervation across a frequency band faster than the operating
frequency of autoregulation. This band was defined to extend from 0.25 to 0.7 Hz and is referred to as the high-frequency (HF) band. For
statistical testing, spectral powers were subjected to logarithmic
transformation. Statistical testing was performed by paired or
independent t-tests as and where
appropriate. P Body weights, hematocrit, PA, and
blood flows are reported in Table 1.
Hematocrits were similar among the six experiments and suggest that the
animals were euvolemic. As expected, rats anesthetized with isoflurane
had higher PA than those
anesthetized with halothane (1). In the time-control experiment,
neither PA nor MBF varied from
periods 1 to
2 (Table 1). Mesenteric denervation reduced PA significantly in
experiments 2 and
4 and marginally in
experiment 3 (P < 0.1), whereas
PA was unchanged in
experiment 1 (time control). Renal
denervation in experiments 5 and
6 had no effect on
PA. Blood flow was not
significantly altered after denervation in any experiment.
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ABSTRACT
Top
Abstract
Introduction
Methods
Results
Discussion
References
![]()
INTRODUCTION
Top
Abstract
Introduction
Methods
Results
Discussion
References
![]()
METHODS
Top
Abstract
Introduction
Methods
Results
Discussion
References
1 · h
1)
after placement of the arterial cannula to permit monitoring of
PA. A constant infusion delivered
1% of body weight per hour; this infusion continued throughout the
experiment and contained 2% charcoal-washed BSA in normal saline. A
left subcostal flank incision was used in all experiments to approach
the renal or superior mesenteric artery. In
experiments 4 and
5, the left kidney was immobilized in
a plastic cup and covered with fat to limit cooling and drying. The
flow probe was placed after the minimal possible dissection, with care
taken to preserve the nerves supplying the vascular bed.
20 min. Anesthesia was then
returned to a surgical plane, and the flow probe was dismounted. In
experiment 1, the flow probe was
remounted on the superior mesenteric artery after the amount of time
typically required for denervation. In experiments 2-4, the superior mesenteric artery and vein were
stripped from the aorta to the first arterial bifurcation, and the
region was painted with 1% toluidine blue in saline, which stains the
nerve fibers (25). All stained fibers were separated, and the region was painted with 5% phenol in ethanol. In experiments
5 and 6, the renal
artery and vein were stripped from the aorta to the hilus of the kidney
by using the same procedure. After denervation of the bed, the flow
probe was remounted, and inspired anesthetic concentration was returned
to the level used in the first experimental period. After a 30- to
40-min equilibration, a second record of
20 min was acquired.
1 in regions where
regulatory systems operate. Resistance phase approaches 
rad
when the system is pressure passive and increases toward 0 rad below
the operating frequency of autoregulation (19, 23). In contrast, a
baroreflex will have positive resistance phase over the band in which
it operates. An obvious caveat is that both active and capacitative
changes may contribute to resistance at high frequencies. There are
conceptual and experimental reasons to believe that capacitative events
in the kidney are small and faster than 1 Hz (5, 19). In the gut, the
situation is not as clear cut. After denervation, however, admittance
phase in the PA-MBF transfer
function was slightly positive (0.12 ± 0.03 rad,
n = 21) and inversely related to
frequency between 0.25 and 0.7 Hz, suggesting that capacitative changes
are small in this region of the spectrum. These observations suggest
that resistance changes in the range from 0.01 to 1 Hz are dominated by
active events in both vascular beds.
0.05 was considered
to indicate a significant difference.
![]()
RESULTS
Top
Abstract
Introduction
Methods
Results
Discussion
References
Table 1.
Status of animals before and after denervation
In the MBF time-control experiment, neither
PA or MBF dynamics changed with
time, as shown in Fig. 1. Noteworthy
features of the power spectra from this experiment include a discrete
oscillation of both PA and MBF at
0.45 ± 0.03 Hz and a broad peak in the MBF spectrum at
0.1-0.15 Hz. The PA-MBF
transfer function, shown in Fig. 1, was similar in the two periods.
Fractional admittance gain declined from
1 above 0.25 Hz to <1
below 0.1 Hz, and the decline was associated with a broad peak in
admittance phase. In the HF band, gain was 1.27 ± 0.10 and 1.11 ± 0.11 in the first and second periods, respectively, whereas phase
was significantly negative, being
1.29 ± 0.14 and
1.09 ± 0.14 rad in the first and second periods,
respectively. Resistance gain and phase are reported in Table
2. In both periods, gain was
1 and phase
was positive in the HF band; neither variable differed significantly between periods.
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The results acquired in experiment 2 (Wistar, MBF, isoflurane) are shown in Fig.
2. MBF dynamics before mesenteric
denervation were very similar to those from the time-control study.
There was a peak in PA spectral
power at 0.47 ± 0.01 Hz; MBF power showed this feature plus a broad
autonomous peak at 0.1-0.15 Hz. Fractional admittance gain
declined from 1.04 ± 0.16 in the HF band to <1 below 0.1 Hz, and
this decline was associated with a broad peak in admittance phase. In
the HF band, admittance phase was significantly negative (
1.32 ± 0.23 rad). Mesenteric denervation reduced integrated PA spectral power at
0.25 Hz
(P < 0.05) due to removal of the 0.47-Hz peak. The equivalent effect on MBF power was not significant. The reduction of gain and phase peak below 0.15 Hz were not affected by
denervation. However, in the HF band, admittance gain was increased to
1.79 ± 0.07 (P < 0.05) and phase
to 0.16 ± 0.07 rad (P < 0.01). The PA-resistance transfer
function is shown in Fig. 2, E and F. Resistance gain and phase in the HF
band are also reported in Table 2. Resistance gain in the HF band was
not different from 1 either before or after denervation. Before
denervation, resistance phase was positive above 0.2 Hz (i.e.,
resistance led PA), whereas
after denervation, resistance phase was strongly negative and followed
PA in this region of the spectrum.
In the HF band, this change was highly significant
(P
0.01).
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Experiment 3 (Wistar, MBF, halothane)
was performed with halothane because this anesthetic is known to
inhibit sympathetic activity at several sites (7, 33), whereas
sympathetic nerve activity is relatively preserved under isoflurane
anesthesia, which was used for all other experiments. This inhibition
is reflected in the lack of PA
spectral power above 0.25 Hz in experiment
3 compared with experiment
1 (P < 0.05). In
particular, no discrete PA
oscillation at or about 0.45 Hz was visible, and mesenteric denervation
had no effect on PA or MBF
spectral power in the region
0.25 Hz (Fig. 3). Fractional admittance
gain declined from 1.61 ± 0.26 in the HF band to <1 below 0.1 Hz,
and this decline was associated with a broad peak in admittance phase.
In the HF band, admittance phase was significantly negative
(
1.09 ± 0.29 rad). Mesenteric denervation did not affect the
reduction of gain or the phase peak below 0.15 Hz, nor did it affect
gain in the HF band (1.56 ± 0.19). However, in this band admittance
phase was increased by denervation to 0.09 ± 0.06 rad
(P < 0.01). Resistance gain and
phase in the HF band are reported in Table 2. Resistance gain tended to
decline after denervation (P < 0.1),
and denervation changed resistance phase from positive to negative
(P < 0.01).
Six- to seven-week-old SHR were employed in experiment
4 (SHR, MBF, isoflurane) because they display increased
sympathetic activity (27), particularly during the period from 6 to 8 wk, during which they become hypertensive (12). Dynamics of
PA and MBF from this experiment
are shown in Fig. 4. No discrete 0.45 Hz
PA oscillation was evident,
although there was a prominent shoulder in the
PA spectrum (cf. Figs.
3A and
4A).
Mesenteric denervation significantly increased
PA and MBF integrated spectral power at
0.25 Hz (both P < 0.01).
Fractional admittance gain declined from 1.21 ± 0.09 in the HF band
to <1 below 0.1 Hz, and this decline was associated with a broad peak
in admittance phase. In the HF band, admittance phase was <0, being
0.31 ± 0.13 rad (P = 0.05).
Mesenteric denervation did not affect the reduction of gain or the
phase peak below 0.15 Hz, but increased admittance gain in the HF band
to 1.81 ± 0.11 (P < 0.01) and
admittance phase to 0.15 ± 0.02 (P < 0.05). Resistance gain and phase in the HF band are reported in
Table 2. Resistance gain was <1 both before and after denervation,
whereas resistance phase was negative and unchanged by denervation.
Before denervation, resistance phase in the HF band varied from 1.37 to
4.05 rad in individual animals.
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RBF dynamics were studied before and after renal denervation in Wistar
rats (expt 5) and young SHR
(expt 6) anesthetized with isoflurane. Results from experiment 5 are presented in Fig. 5. There was the
expected discrete peak in PA
spectral power centered at 0.45 ± 0.02 Hz, and this peak was
unaltered after renal denervation, as was integrated
PA spectral power at
0.25 Hz.
Fractional admittance gain displayed a prominent resonance peak at 0.21 ± 0.02 Hz, below which it declined to <1 associated with a broad
phase peak. This autoregulatory signature was not altered after
denervation. In the HF band, denervation increased admittance gain from
1.01 ± 0.12 to 1.60 ± 0.17 (P < 0.05). Admittance phase in this band was 0.08 ± 0.09 rad before denervation and was unchanged at 0.23 ± 0.05 rad after
denervation. The PA-resistance
transfer function from this experiment is also shown in Fig. 5,
E and
F. In the HF band, resistance gain was
considerably <1 both before and after denervation (Table 2),
indicating that PA fluctuations in
this band were associated with only small resistance changes.
Resistance phase was strongly negative above 0.3 Hz before and after
denervation. The apparent difference
(P < 0.1) arises from one animal
that showed positive resistance phase during the innervated period.
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Results from young SHR (expt 6) are
presented in Fig. 6. As in the other SHR
experiment (expt 4), the
PA and RBF spectra conspicuously lacked a discrete peak at ~0.45 Hz, although there were prominent shoulders in both. Denervation increased
PA and RBF integrated spectral
power at
0.25 Hz (both P < 0.01).
Renal denervation increased admittance gain in the HF band from 1.39 ± 0.07 to 1.86 ± 0.07 (P < 0.05) but did not affect admittance phase in this region of the
spectrum (0.14 ± 0.04 rad before and 0.22 ± 0.01 rad after
denervation). Resistance gain and phase in the HF band are reported in
Table 2. Resistance gain was <1 both before and after denervation,
whereas resistance phase was strongly negative and unchanged by
denervation.
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Examination of pooled results revealed that before denervation SHR
(expts 4 and
6) had considerably greater total
PA spectral power than did Wistar
rats anesthetized with isoflurane (expts 2 and 5), integrated
total power being 2.57 ± 0.40 mmHg2/Hz in Wistar rats and 12.40 ± 2.74 mmHg2/Hz in SHR
(P
0.01). In both strains of rats,
there was also a significant difference between MBF and RBF with
respect to autoregulation. The resonance peak in gain of autoregulation
can be used as an index of the system's natural frequency (18). The
resonance peak of mesenteric autoregulation occurred at 0.13 ± 0.01 after denervation in each of experiments
2-4. These values were taken from 256-point
transfer functions. In contrast, the resonance peak in gain of renal
autoregulation occurred at 0.21 ± 0.02 and 0.23 ± 0.01 Hz in
experiments 5 and
6, respectively, after denervation. When the values from the three MBF and two RBF experiments were pooled,
there was a highly significant difference between the two beds
(P
0.01).
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DISCUSSION |
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These experiments were performed to assess the dynamic regulation of blood flow to two major vascular beds, the kidney and the gut. These beds have in common that they receive large fractions of cardiac output and that their arteries originate close together on the abdominal aorta. However, they have widely disparate structure and physiology. Consequently, one might expect them to respond differently to spontaneous PA fluctuations and to contribute differently to overall cardiovascular regulation. The results show strong autoregulation of blood flow in both beds as well as significant, though different, centrally mediated (i.e., sympathetic) dynamic control elements.
Two strains of rat and two anesthetics were used to generate three
levels of sympathetic activity. SHR have elevated renal sympathetic
nerve activity compared with Wistar rats (12), especially during the
period from 6 to 8 wk of age during which they become markedly
hypertensive (27). Sympathetic vasomotor activity generates most
PA spectral power at frequencies
>0.1 Hz (5, 31) and is largely related to operation of arterial
baroreflexes (5, 20), consistent with fivefold higher integrated
PA spectral power at
0.25 Hz in
young SHR than in Wistar rats. Halothane is known to inhibit
sympathetic output at several sites (7, 33), and we have previously
observed that changing from isoflurane to halothane anesthesia within
an experiment reduced PA spectral power at frequencies >0.1 Hz (10). Similarly, in the present study,
there was less integrated PA
spectral power above 0.25 Hz (P < 0.05) in rats anesthetized with halothane (expt
3) than in identically prepared rats anesthetized
with isoflurane (expt 1). In
addition, a time-control study (expt
1) was included to ensure that observed changes in
MBF dynamics resulted from denervation. It was not necessary to include
a similar control for the effects of denervation on RBF dynamics
because the postdenervation renal transfer functions are well described
for both normotensive rats (1, 10, 18, 19, 23, 32) and SHR (6, 11).
Mesenteric, but not renal, denervation significantly reduced
PA. This response was not
associated with significant changes in MBF as shown in Table 1 or with
any consistent change in heart rate (data not shown). Most likely, it
was a consequence of the well-known regulation of portal capacitance by
sympathetic inputs (16, 36). Thus removal of adrenergic tone by
mesenteric denervation increased portal capacitance, reducing cardiac
preload. Consistent with this interpretation is the observation that
PA was reduced by
22 ± 3 mmHg in SHR (P < 0.01), by
14 ± 5 mmHg in Wistar rats anesthetized with isoflurane
(P < 0.05), and by only
3.3 ± 1.5 mmHg in Wistar rats anesthetized with halothane
(P < 0.1). Thus the reduction of
PA varied in parallel to the
predicted sympathetic activity.
Transfer functions from both vascular beds, acquired after denervation, show only one active system. This was undoubtedly autoregulation. Before denervation, particularly in the gut, two or more active systems were apparent. The additional control systems presumably reflect ongoing sympathetic activity. It is relatively simple to predict that an arterial baroreflex operating on a vascular bed to stabilize PA will have negative admittance phase because flow follows pressure after a delay governed by transmission time and that admittance gain should be high because flow is altered to regulate pressure. However, neural inputs unrelated to PA are not defined in the transfer function, although they may be expected to affect the observed transfer function in both PA-independent and -dependent fashions. Because there is no characteristic temporal relationship between "other" sympathetic nerve activity and PA, phase may be expected to trend to 0. Flow fluctuations unrelated to PA would be observed as increased gain. Sympathetic activity may also reduce arterial compliance and thus reduce the passive, PA-induced fluctuation of blood flow (2). This would be seen as reduction of admittance gain. Thus there is no clear interpretation as to how such inputs would affect the observed admittance gain. In this situation admittance phase is therefore more informative than admittance gain.
Autoregulation. Transfer functions from all six experiments show the presence of dynamic autoregulation (1, 6, 10, 11, 18, 19, 32). This signature was present before and after denervation, indicating that autoregulation was not overridden by central mechanisms. The autoregulatory signatures in the two beds (e.g., Figs. 2 and 5) are very similar to that predicted for a myogenic system (18), suggesting that dynamic autoregulation was dominated by a myogenic mechanism in both renal and mesenteric vascular beds. With respect to the kidney, this conclusion is consistent with the results of previous studies, performed in rats (1, 11) and dogs (23), in which tubuloglomerular feedback was explicitly excluded by physical or pharmacological blockade and in isolated perfused hydronephrotic kidneys that lack tubuloglomerular feedback (9).
In both beds, autoregulation substantially stabilized blood flow in the face of PA fluctuation. Pooled results indicate that, after denervation, fractional admittance gain at 0.01 Hz was 0.29 ± 0.04 in the gut and 0.28 ± 0.04 in the kidney. Thus dynamic autoregulation was as efficient in the gut as in the kidney. Although efficient renal autoregulation was expected, the gut is reputed to show weak autoregulation (e.g., Ref. 17). We are not aware of previous studies that address dynamic autoregulation by the mesenteric circulation. With respect to steady-state autoregulation (i.e., MBF responses to imposed and sustained PA steps), data in the literature are rather variable. Some reports show substantial autoregulatory efficiency (e.g., Refs. 29, 34), whereas others show considerably less efficient autoregulation (e.g., Refs. 15, 21). A number of factors could contribute to this divergence, including the presence or absence of chyme in the lumen (34) and the species studied (15, 26, 29). We cannot explicitly exclude food as a variable, since our rats were studied during the day, their inactive period, although the lumen of the small bowel typically contained chyme. Arguing by analogy to autoregulation of RBF, we would suggest that species differences are inconsequential. Steady-state autoregulation of RBF is similar in dogs (17) and rats (8), and RBF dynamics are very similar in dogs (23) and rats (19). There was one major difference between the two beds. Autoregulation was significantly slower in the gut (0.13 ± 0.01 Hz) than in the kidney (0.22 ± 0.01 Hz). The data do not address the mechanism(s) behind this difference. There are, however, several important functional consequences. First, the gut and two kidneys together receive a large portion of cardiac output. If they were to autoregulate at the same frequency, there would be considerable potential for phase locking, which could result in destabilizing oscillation of PA and of blood flows to all three organs. In this light, it is noteworthy that the operating frequencies in the two beds are linked to each other in a ratio of ~5 to 3, thus minimizing the likelihood of phase locking (13). Second, in conscious animals, frequent sudden falls of PA are surprisingly common and are often associated with onset of activity (5, 31). Because the kidney responds faster than the gut, it may well be better protected from such rapid transients.Sympathetic influences.
Before denervation both the kidney and the gut displayed active events
at
0.25 Hz, indicating the presence of significant sympathetic inputs
in this region of the spectrum. These events were specific to the
different vascular beds. In the gut, the admittance phase was
significantly negative, whereas resistance phase was >0 rad, implying
the presence of an active controller related to
PA and acting on resistance, i.e.,
a baroreflex. This result was very clear in the Wistar rats but less
clear in the young SHR. It is not possible to determine from the
present data whether a functional baroreflex in these SHR was being
swamped by unmodulated sympathetic activity or whether the baroreflex itself was impaired. The kidneys of Wistar rats and SHR did not show
the signature of a baroreflex. Instead, admittance phase was 0 or
slightly positive, whereas resistance phase was strongly negative, both
characteristic of pressure-passive behavior. Furthermore, mesenteric
denervation in experiment 2 abrogated
the 0.47-Hz PA rhythm, whereas
renal denervation in experiment 5 did
not. The simplest interpretation of these findings is that there is a
physiologically significant baroreflex operating on MBF, but not RBF,
to stabilize PA. Because
mesenteric denervation abrogated the 0.47-Hz
PA rhythm, it is tempting to
surmise that the mesenteric circulation is a predominant site of
baroreflex operation.
0.25 Hz,
and this power appeared to be modulated in a different manner: no
discrete 0.45-Hz oscillation of PA
could be identified. Unlike the Wistar rats, denervation of either bed
increased PA and blood flow
spectral power (Figs. 4 and 6). In the HF band, admittance phase was
only modestly negative (Fig. 4), whereas resistance phase was highly
variable (Table 2). In fact, only two of the eight rats studied showed
clear baroreflex signatures in the
PA-MBF and
PA-resistance transfer functions.
In the absence of nerve traffic analysis, no definitive conclusions can
be drawn. However, the overall pattern is suggestive of increased
efferent sympathetic nerve activity that is not effectively modulated
by baroreflexes. The data suggest that elevated sympathetic activity
reduced compliance and that its removal permitted a strong increase in
PA-passive blood flow fluctuation
which was then transmitted to PA.
It is known that both beds are sufficiently large, in terms of blood flow, so that blood flow fluctuations can generate corresponding PA fluctuations (22, 35).
Limitations. Positive controls to ensure intact innervation were not performed; instead, a very extensive denervation procedure was employed. A much less aggressive procedure is normally used in this laboratory and reliably reproduces the features of the PA-RBF transfer function seen after denervation (1, 10; unpublished results). We are thus confident of the effectiveness of the denervation procedure employed.
Spontaneous PA fluctuation was used as the input signal to examine dynamic regulation of RBF and MBF. Because the amount of PA fluctuation is reduced in anesthetized as opposed to conscious rats and is certainly less than when PA is externally forced, the apparent lack of an arterial baroreflex affecting RBF dynamics could reflect insufficient input power. This explanation is unlikely because strong stimuli caused only minor baroreflex modulation of RBF in steady-state experiments (30) and because the input power was similar in the MBF experiments, which did disclose an arterial baroreflex, and the RBF experiment, which did not. The identification of an arterial baroreflex rests on the predicted transfer function, the central origin of the negative admittance phase (and positive resistance phase), the known origin of the 0.47-Hz rhythm in PA, and its generation in the mesenteric circulation. Because the control systems studied were operating in closed-loop mode, it is possible that the open-loop analysis used may not capture their dynamics accurately (24). However, we would note the following: 1) the analysis captures autoregulation dynamics in both beds (observed dynamics are consistent with model-based predictions and with a large body of open- and closed-loop studies); 2) the observed central effects on RBF dynamics are consistent with what is known from steady-state studies; and 3) conclusions drawn from the PA-MBF transfer function are consistent with inferences drawn from the power spectra, which are not subject to this constraint.Perspectives
These experiments assessed three major events that actively alter vascular conductance in response to PA fluctuations. The arterial baroreflex operates on vascular admittance to stabilize PA, whereas renal and mesenteric autoregulation operate on admittance to stabilize regional blood flows. Thus the baroreflex must be separated from the autoregulatory systems to avoid potentially destructive interactions among them. This is accomplished by the baroreflex operating faster than autoregulation, i.e., separation in time. Equally, if autoregulation in two major beds (intestine and 2 kidneys) were to operate at the same frequency, there would be considerable potential for entrainment and subsequent resonance in MBF and RBF and in PA. Overall, the faster autoregulation in the kidney will tend to minimize transmission of baroreflex-induced PA fluctuations to the glomerulus, whereas the slower autoregulation in the gut will tend to minimize interactions between the baroreflex and autoregulation in this bed.| |
ACKNOWLEDGEMENTS |
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This work was funded by grants to W. A. Cupples from the Heart and Stroke Foundation of Quebec, Kidney Foundation of Canada, and Medical Research Council of Canada.
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FOOTNOTES |
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The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. §1734 solely to indicate this fact.
Address for reprint requests: W. A. Cupples, Lady Davis Institute, SMBD-Jewish General Hospital, 3755 Cote St.-Catherine Rd., Montreal, QC, Canada H3T 1E2.
Received 2 February 1998; accepted in final form 7 July 1998.
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