Compartmental Syndromes.
Edited By: Winston J. Warme, MD, Frederick A. Matsen III, M.D. Last updated Wednesday, December 23, 2009
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Tissue pressure and its measurement
In discussing the effects of increased tissue pressure on local
circulation in compartmental syndromes, the net force per unit area
exerted on the walls of vessels is of primary importance.Pressure measurement techiques
Several methods have been described for the measurement of tissue pressure, only a few of which are clinically useful.
The infusion technique is a reliable method for continuously monitoring tissue pressure in the clinical situation.
The continuous infusion and wick techniques give similar pressure readings for intramuscular tissue pressures in animal and human model systems.
Tissue pressure within a limb may significantly exceed the pressure applied externally to the limb.
To be reliable and thus clinically useful, any tissue-pressure-measurement technique should be practiced in normal subjects before it is used for evaluation of a patient with a possible acute compartmental syndrome.
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Definition of tissue pressure
By definition, increased tissue pressure is the primary
pathophysiological factor in compartmental syndromes. We must therefore
define tissue pressure and attempt to resolve some of the confusion
that has resulted from previous usage of this term.
A nonhomogeneous and anisotropic material such as tissue cannot be
thought of as having a pressure in the same sense as a liquid or gas.
This ambiguity is resolved somewhat by considering the two contexts in
which the term "tissue pressure" might be invoked. The first concerns
the exchange of fluid across a capillary wall. 1 2 This fluid movement
is related to:
K (PC - PT ( H) + R OT - R OC) [ 1 ]
where K is a constant, PC is the capillary blood pressure, PT ( H)
is the hydrostatic pressure of tissue fluid, R is the capillary
membrane reflection coefficient, OT is the oncotic pressure of tissue
fluid, and OC is the oncotic pressure of blood plasma.
The second situation in which the concept of tissue pressure might
be invoked is in the consideration of forces operating on a vessel
wall. The law of Laplace has been applied to this situation:
PI - PO = T/R [ 2 ]
where PI is the pressure exerted on the inside of the vessel wall,
PO is the net force per unit area exerted on the outside of the vessel
wall, T is the tension in the vessel wall, and R is the vascular
radius.
Neither PT (H) nor PO is simple. Because extracellular fluid may
exist in a free form, in a gel, and perhaps in other forms, PT (H)
should actually refer to the physical chemical activity of
extracellular fluid. 4 By contrast, PO is the resultant of several
different elements. A positive contribution to PO may result from
interstitial fluids, gels, and matrices, as well as from fibers and
cells under compression. A negative contribution to PO may arise from
cells and fibers under tension. Thus, in the general case it cannot be
assumed that the two "tissue pressures" [PT (H) from equation 1 and PO
from equation 2] are equal. 5- 6 To appreciate how they may differ, we
have only to consider the analogy of a beaker that contains water and
ball bearings. The hydrostatic pressure of water at the bottom of the
beaker [analogous to PT(H)] is equal to the height of water in the
beaker (H). The net force per unit area on the beaker bottom (analogous
to PO) is equal to the total weight in water of the ball bearings (W)
divided by the surface area of the beaker bottom (A) plus the
hydrostatic pressure: W/A + H.
In discussing the effects of increased tissue pressure on local
blood flow, the "tissue pressure" of primary interest is PO, the net
force per unit area exerted on the outside of a vessel wall. This is
the force that affects the pressure in and the flow through collapsible
vessels. The mechanisms by which increased tissue pressure compromises
local blood flow will be discussed in greater detail in Chapter 3.
Tissue pressure measurement
Because tissue pressure plays a central role in compartmental
syndromes, it is appropriate to review some of the described techniques
for tissue pressure measurement.
The capsule method employs a porous capsule surgically implanted in
the tissue to be studied. After several weeks the fluid in the capsule
reaches equilibrium with the surrounding interstitial fluid. The
pressure of the fluid within the capsule is then measured with a
pressure transducer. 5- 7- 8 This method has the clinical disadvantages
of requiring surgical implantation and a prolonged period for
equilibration. Stromberg and Wiederhielm 8 have criticized the capsule
method on the basis that the observed pressure is influenced by the
osmotic gradient between the fluid inside and the fluid outside the
capsule.
Collapsible segment methods measure the pressure inside a
flaccid-walled structure located within the tissue. 9 10 These methods
are based on equation 2: when the walls of a fluid-filled structure are
flaccid (the tension of the walls [ T ] is zero), the pressure of the
fluid inside (PI) is equal to the pressure outside (PO). ; Thus, the
measuring of the fluid pressure inside this structure ; yields the
tissue pressure. Although some of these methods have l the disadvantage
of requiring surgical implantation, Ryder et al. 11 and Kjellmer l2
have described variations using an in situ vein as the collapsible
segment. Although the method of Ryder et al may be clinically useful
for measuring subcutaneous tissue pressure, it is impractical for the
measurement of intramuscular pressure in a X traumatized limb because
it would require the cannulation of a deep intramuscular vein and
repeated raising and lowering of the limb relative to the heart.
A servonull technique with micropipettes has been described by
Wiederhielm. 4 In this method no net fluid is injected into the tissue,
yet a continuous fluid column between the transducer and the tissue is
maintained by a servosystem. Although this method is highly accurate
and responsive, it appears to be too delicate and complicated for
routine clinical use.
The injection technique measures the pressure necessary to inject a
small quantity of fluid into the tissue through a f needle. l3-l7
Although this method has the advantage of using inexpensive equipment,
it has a disadvantage in that a steady-state reading is not attained.
Thus, it may be somewhat awkward in practice because a fluid manometer
and an air-water meniscus must be observed simultaneously to detect the
pressure at which fluid first begins to flow into the tissue. In an
animal model where tissue pressure was elevated by fluid infusion at a
known pressure, Hargens et al found that the injection technique
overestimated low tissue pressures and underestimated high tissue
pressures. Clayton et al 9 evaluated the injection technique by
applying known pressures to the extremities of six rabbits with a
pneumatic cuff. A good linear correlation was obtained with a slope of
1.03 (r = 0.99).
The wick technique employs strands of wettable material extending
into the tissue from a fluid-filled catheter connected to a pressure
transducer. 6,7, 20-22 The wick increases the surface area in contact
with the tissue. To protect its fibers, the wick catheter is inserted
through a larger cannula, which is then withdrawn. Clotting around the
fibers is minimized by heparinization of the fluid within the catheter.
Various materials have been used to make wick catheters; these include
cotton and polyglycolic acid suture. The latter is most commonly used
in the clinical situation. Zeluff 23 pointed out, however, that
polyglycolic acid suture has a short shelf life after sterilization and
suggested that Dacron (DuPont) may be a more suitable material.
Continuity of the fluid column between the tissue and the transducer
is necessary for accurate pressure measurement. This continuity may be
verified by observing a sharp increment in the observed pressure when
the tissue overlying the catheter is pressed manually. If catheter
patency cannot be assured, the catheter may be flushed with a small
volume of heparinized saline. Mubarak et al 22 found that the wick
catheter accurately reflected pressures applied by fluid infusion in
dog limbs. We obtained reproducible results with the wick catheter when
known increments of pressure were applied externally to rabbit and
human limbs as long as the wick catheter remained patent. 24
In the continuous infusion technique, the patency of a hypodermic
needle or intravenous catheter inserted into the tissue is maintained
by the slow but continuous infusion of nonheparinized saline solution.
The pressure of the fluid within the needle or catheter is continuously
monitored with a standard blood pressure transducer. Since its original
descriptions this technique has been improved through the use of
noncompliant tubing, a simplified fluid path, and an ordinary needle or
catheters
For continuous pressure monitoring, an infusion rate of 0.7 cc per
day is used. Laboratory studies have demonstrated that the pressure
measured is relatively independent of the rate of infusion: an acute
40-fold increase in the infusion rate from 0.7 to 29 cc per day
produced only a 4-mm Hg increase in measured pressure. 25 It could be
argued theoretically that even a rate of infusion as low as 0.7 cc per
day could be hazardous to the patient. For example, Hargens et al 2
found that the acute infusion of 2 cc of plasma into a canine
anterolateral compartment (volume of 40 cc) raised the
intracompartmental pressure from 30 to 45 mm Hg. The pressure increment
from saline infusion is unlikely to be a problem clinically, however,
for two reasons: saline is absorbed three times more rapidly than
plasma, 2 and three days of pressure monitoring would be necessary to
infuse the volume of 2 cc. Furthermore, most human compartments are
well over 10 times as large as the canine anterolateral compartment.
The data obtained by Whitesides et al 7 from a limb amputated for
sarcoma of the femur indicated that over the range of
intracompartmental pressures from 10 to 50 mm Hg, the infusion of 1 cc
of saline into the anterior compartment of the leg produced a 1-mm Hg
increment in intracompartmental pressure. Thus, even assuming the worst
possible case in which saline absorption is zero (i.e., a totally
ischemic compartment), three days of continuous pressure monitoring
with an infusion rate of 0.7 cc per day would give rise to an increment
in tissue pressure of only 2 mm Hg.
We have demonstrated the accuracy and dependability of the
continuous infusion technique in rabbit and human model systems where
known increments of pressure were applied to living limbs.
Results of different tissue pressure measurement t
Earlier in this chapter we discussed the fact that there are at
least two different "tissue pressures": the PO in the law of Laplace
and the PT(H) in the capillary filtration equation. Because these two
quantities cannot in the general case be expected to be identical, it
would not be surprising if different tissue-pressure-measuring
techniques yielded somewhat different values.
To determine whether or not the wick and continuous infusion
techniques yielded significantly different results, we conducted
side-by-side studies in rabbit and human model systems in which
increments of external pressures were applied. We found that as long as
wick catheter patency was closely monitored and any obstruction was
cleared by flushing with a minimal volume of fluid, the two methods
yielded virtually identical results in compressed rabbit and human
muscle.
Even when no pressure was applied, our side-by-side comparison
yielded similar pressure measurement values in human tibialis anterior
muscle with the wick and the infusion techniques: 7+3 mm Hg and 9+3 mm
Hg, respectively. 24 These values do not appear to be significantly
different from those obtained with the wick technique by Mubarak et al
22 in normal forearm and leg muscle: 4 +4 mm Hg. Thus, in our hands,
there is no practical difference between the results of the wick and
the infusion techniques for intramuscular pressure measurement.
I prefer the continuous infusion technique for clinical tissue pressure measurement for the following reasons:
- No specially prepared catheter is required; any
needle or small intravenous catheter will serve. In compartments of the
forearm and leg we routinely use a standard 22-gauge intravenous
catheter with a 19-gauge inserting needle. This is considerably smaller
than the 14- and 16-gauge placement units recommended for use with the
wick catheters 22 We have used 25- and 27-gauge needles to measure
pressure within the interosseous compartments of the hand.
- Heparinization of the fluid within the catheter is not required; thus, the possibility of enhanced local bleeding is eliminated.
- Catheter
patency is continuously maintained by a volume-controlled infusion. As
a result, catheter obstruction has not occurred in our clinical use of
this monitoring method. Continuous pressure monitoring may be carried
out for periods of at least 72 hours without the need for adjusting or
manually flushing the system.
- The pressure can be read at any time from the meter of the transducer monitor.
- The
equipment for the technique is available in most hospitals.
Anesthesiologists are well acquainted with the calibration, zeroing,
and operation of pressure transducers and can be of great assistance in
setting up the system.
- The results are accurate and reproducible.
- On removal of the catheter or needle, there need be no concern about retained wick elements. 18
Like all other techniques for tissue pressure measurement, the
continuous infusion method requires attention to detail and practice
before proficiency and the necessary bedside efficiency are attained.
Thus, I believe it is unwise to try to learn this or any other tissue
pressure-measuring technique when confronted with a possible acute
compartmental syndrome. The experience is likely to be frustrating, and
the pressure reading obtained is unlikely to be reliable. An incorrect
pressure reading is worse than none at all because it may distract from
important clinical findings.
For those interested in being prepared to perform reliable pressure
measurements, I would suggest practicing the technique on normal
subjects until consistent readings in the normal range are obtained. If
desired, one can apply a known pressure to the limb with an air splint
to see if the measured pressure increases by the expected increment.
Relationship of applied and measured pressure
It has been generally assumed that the pressure applied to the
outside of a limb is distributed essentially unaltered throughout the
tissue. However, in our initial studies of the infusion technique, 25
we identified a phenomenon of "summation": the intramuscular pressure
measured when an external pressure is applied to a limb is equal to the
measured intramuscular pressure before pressure application plus the
externally applied). More recent data 24 indicated an additional
feature in the variance of applied and measured pressure: the increment
in measured pressure within muscle exceeds the increment in applied
pressure by a factor ranging from 1.02 to 1.3, depending upon the model
system, as indicated by slopes of the plots of measured and applied
pressure. This geometric augmentation of applied pressure is referred
to as "amplification." 24 This phenomenon was found to be most striking
in the anterior compartment of the rabbit leg, where the amplification
factor obtained with both the wick and infusion techniques was 1.3
(i.e., the increment in measured pressure was 30% higher than the
increment in externally applied pressure). At present we have not
identified the mechanism of amplification. The fact ; that in the
rabbit anterior compartment the amplification factor was dramatically
diminished by fasciotomy suggests that the nonyielding fascia may have
a significant effect on the pressure field induced by externally
applied pressure.
Both summation and amplification can result in a significant
difference between the pressure applied to an extremity and the
pressure measured within it. This difference may be important in e
interpreting experiments on the amount of pressure required to arrest
blood flow, 33 in deciding the safe limits for air splints and pressure
dressings, 34 and in interpreting the results of sphygmomanometry. 35
The magnitude of the apparent discrepancy is significant. The observed
relationship of externally applied pressure.
Surgery for Compartmental Syndromes at the University of Washington, Department of Orthopaedics and Sports Medicine, Seattle, Washington
If you are interested in making an appointment to discuss this procedure in Seattle, you can request an appointment using our online referrals website. To request a referral online, please click here. You can also call 206-598-BONE (2663) to make an appointment. Our clinical center is located in Seattle Washington, USA
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