Circulation. 1999;100:2146-2152
(Circulation. 1999;100:2146.)
© 1999 American Heart Association, Inc.
Clinical Investigation and Reports |
CPR Techniques That Combine Chest and Abdominal Compression and Decompression
Hemodynamic Insights From a Spreadsheet Model
Charles F. Babbs, MD, PhD
From Indiana University School of Medicine and the Department of Basic
Medical Sciences, Purdue University, West Lafayette, Ind.
Correspondence to Charles F. Babbs, MD, PhD, Basic Medical Sciences, 1246 Lynn Hall, Purdue University, West Lafayette, IN 47907-1246. E-mail babbs{at}vet.purdue.edu
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Abstract
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BackgroundThis study was done to
elucidate mechanisms
by which newer cardiopulmonary
resuscitation (CPR) techniques,
including interposed abdominal
compression (IAC), active compression-decompression
(ACD), and
Lifestick CPR, augment systemic perfusion pressure
and forward flow and
to compare the 3 techniques in the same
test system.
Methods and ResultsMathematical models describing
hemodynamics of the adult human circulation during
cardiac arrest and CPR were created and exercised by use of spreadsheet
software. Assumptions of the models are limited to normal human
anatomy and physiology, the definition of compliance (volume
change/pressure change), and Ohms law (flow=pressure/resistance).
Standard CPR generates 1.3 L/min forward and 25 mm Hg systemic
perfusion pressure. In otherwise identical models, IAC-CPR generates
2.4 L/min and 45 mm Hg; ACD-CPR, 1.6 L/min and 30 mm Hg;
and Lifestick CPR, which combines IAC and ACD, 3.1 L/min and 58
mm Hg. Augmented CPR techniques work by enhanced priming of either
chest or abdominal pump mechanisms.
ConclusionsAdjunctive maneuvers, combined with conventional
chest compression, can produce substantial hemodynamic
benefit in CPR by credible physiological
mechanisms.
Key Words: blood flow cardiopulmonary resuscitation computers heart arrest Lifestick mechanics
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Introduction
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Two mechanical techniques have emerged from animal and
clinical
studies as potentially effective means of augmenting perfusion
during
external cardiopulmonary resuscitation (CPR). The first
is the
addition of interposed abdominal compression (IAC) to otherwise
standard
CPR.
1 2 3 The second is CPR with active
compression and decompression
(ACD) of the chest.
4 5 6
Reviews of these techniques are found
in References 7 and 8
7 8 . During
IAC-CPR, positive pressure
is applied to the abdomen in counterpoint to
the rhythm of chest
compression, so that the abdomen is being
compressed when chest
pressure is relaxed. During ACD-CPR, positive and
negative pressures
are applied alternately to the chest by means of a
"plunger"
that forms a seal with the anterior chest wall. Both
methods
improve hemodynamics in animal studies of
electrically induced
ventricular
fibrillation.
9 10 Both improve CO
2 excretion
as
a measure of effective systemic perfusion in human
resuscitation.
4 11 12 Three randomized clinical trials of
IAC-CPR compared
with standard CPR
2 11 13 have found
statistically significant
benefit, and 1 early trial found no
difference.
14 Four randomized
clinical trials of ACD-CPR
have found improved outcome,
5 6 15 16 and 4 other trials
have found no difference.
17 18 19 20 Most recently,
Lifestick CPR
21 has become the subject of active
research.
The Lifestick is a 2-handled device that is able to apply IAC
and
ACD-CPR simultaneously by alternately compressing and
decompressing
the chest and the abdomen through adhesive pads. These 3
CPR
adjuncts are illustrated in Figure 1

.
Using a mathematical model of CPR hemodynamics, the
nomenclature for which is given in Table 1
, the author has explored the
possibility that IAC, ACD-CPR, and Lifestick CPR work by similar
mechanisms. The hypothesis is that improved filling of the thoracic
aorta and right heart can be accomplished either by positive pressure
in the abdomen or by negative pressure in the chest and conversely,
that improved filling of the abdominal aorta can be achieved either by
positive pressure in the chest or by negative pressure in the abdomen.
Improved pump filling, in turn, leads to higher stroke output, systemic
perfusion pressure, and systemic blood flow.
The approach to the present research was to create and test a
mathematical model of CPR hemodynamics based on
fundamental principles of cardiovascular physiology.
Such a model is independent of the many confounding factors present
in laboratory studies and in clinical trials. These include varying
patient populations, downtime, drug therapy, central venous pressure,
peripheral vascular resistance, underlying disease, chest
configuration, and body size, as well as varying rescuer size, skill,
strength, consistency, prior training, and bias.
Mathematical models also allow exact control of the dominant
hemodynamic mechanism of CPR (thoracic pump in large
subjects versus cardiac pump in small subjects).22 This
approach facilitates quantitative comparison of various resuscitation
techniques in exactly the same test system.
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Methods
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Anatomic Parameters
To capture the essence of CPR hemodynamics, one
may solve the
family of differential equations describing pressures and
flows
in the simplified fluidic system shown in Figure 2

. The human
circulation is
represented by 7 compliant chambers connected
by
resistances through which blood may flow. The compliances
correspond to
the thoracic aorta, abdominal aorta, lumped superior
vena cava and
right heart, lumped abdominal and lower extremity
veins, carotid
arteries, and jugular veins. In addition, the
chest compartment
contains a pump representing the pulmonary
vascular
and left heart compliances between the pulmonic valve
and the aortic
valve. This pump may be configured to function
either as a heartlike
cardiac pump, in which applied pressure
squeezes blood from the heart
itself through the aortic valve,
or as a global thoracic pressure pump,
in which applied pressure
squeezes blood from the pulmonary
vascular bed through the left
heart and into the
periphery.
23 24 25
Conductance pathways with nonzero resistances, R, connect the
elastic compartments. Rh, Rht, and
Rs are large and represent resistances of the
systemic vascular beds of the head, heart, and trunk and legs.
Rc, Ra, Rj, and Rv are
small and represent in-line resistances of the great vessels.
Ri and Ro are the small input and output
resistances of the chest pump in series with the aortic and pulmonic
valves. Niemanns valves between the chest and jugular veins at the
level of the thoracic inlet are actual but little-known anatomic
structures that function to block headward transmission of large
positive pressure pulses in the chest during cough and also during
CPR.26
Physiological Parameters
Parameters describing a textbook normal "70-kg
man"27 (Table 2
) are used
to specify values of the compliances and resistances shown in Figure 2
.
The normal 30-fold ratio of venous to arterial compliance
characterizes a circulation in the absence of fluid loading or
congestive heart failure. The distribution of vascular conductances
(1/resistance) into cranial, thoracic, and caudal components reflects
textbook distributions of cardiac output to various body regions.
Solving for Pressures in the System
The relationships among the pressures in the various vascular
compartments are determined by the definition of compliance and by
Ohms law. The definition of compliance is C=
V/
P, where C is
compliance and
P is the incremental change in pressure within a
compartment as volume
V is introduced. Ohms law, which relates
flow to pressure and resistance, is
i=(1/R)(P1-P2), where
P1-P2 is the instantaneous change in pressure
across resistance R as flow i occurs. In Figure 2
, currents
ic (carotid), ia (aortic), is
(systemic), iv (venous), ij (jugular),
ii (pump input), and io (pump output) are shown
for clarity, with positive directions specified by arrows.
Extrathoracic Components
Applying these basic concepts with reference to Figure 2
provides a set of governing finite-difference equations that can be
used to describe hemodynamics. These equations can be
integrated numerically to describe instantaneous pressure versus time
waveforms in each of the 7 compartments. Beginning, for example, with
the abdominal aorta,
 | (1) |
Here,

P
abd represents
the change in
external pressure applied to vessels in the abdominal
compartment
during IAC and Lifestick CPR. For standard CPR,

P
abd is
assumed to be zero. The next term represents the increase
in
abdominal aortic pressure caused by net inflow of blood during
the
small time interval

t. Substitution for currents i
a and
i
s by use of Ohms law completes the expression.
Similarly,
the pressure changes in other extrathoracic vascular
compartments
are given by Equations 2 through 4



, as follows.
 | (2) |
 | (3) |
 | (4) |
where N=1 normally and N=0 during cough or intrathoracic
pressure
pulses (when P
RH>P
jug).
Thoracic Components
Corresponding expressions for the 3 thoracic components of the
model are as follows.
 | (5) |
where E=1 during ejection (aortic valve open) and E=0 otherwise.
 | (6) |
where F=1 during the filling phase (pulmonic valve open) and F=0
otherwise, and N=0 during CPR-induced intrathoracic pressure pulses
(Niemanns valve closed) and N=1 otherwise. Finally,
 | (7) |
Numerical Methods
Integration
Standard spreadsheet programs, such as Microsoft Excel, are
ideal for implementing numerical integration of Equations 1 through 7





to obtain pressures in all 7 compartments as a function of time. To
simulate a resuscitation, one can create a spreadsheet in which
pressures in each compartment at any point in time are computed from
the pressures at the preceding time point and the corresponding
Psthat is,
 | (8) |
Applied Pressures for Chest and Abdominal Compression
Pchest and Pabd represent
driving intrathoracic and intraabdominal pressures applied to outer
surfaces of blood vessels in the chest and abdomen of the model.
Although any arbitrary function or waveform can be used to
represent the imposed chest and abdominal pressures in external
CPR, the present studies used half-sinusoidal functions, defined as
follows and sketched in Figure 3
. To
represent chest compression,
 | (9) |
 | (10) |
 | (11) |
 | (12) |
To explore the influence of the thoracic pump
versus the cardiac
pump mechanisms that can impel blood during
cardiac arrest and chest
compression, a factor 0

Tpfactor

1 is
introduced, and a pressure
equal to the product of P
chest and
Tpfactor is applied
to the thoracic aorta and superior vena
cava to create a continuum of
hybrid pump mechanisms ranging
from pure cardiac pump (Tpfactor=0) to
pure thoracic pump (Tpfactor=1).
When Tpfactor=1, all intrathoracic
structures, including the
great veins and thoracic aorta, experience a
uniform "global"
intrathoracic pressure rise, as originally
conceived by Rudikoff
and coworkers.
28 When Tpfactor=0,
only the pump compliance,
C
P, is pressurized, as if the
heart alone, and not the great
vessels, were compressed between the
sternum and the spine,
as originally conceived by Kouwenhoven et
al.
29 Intermediate
values of the thoracic pump factor
allow models approximating
the present
understanding,
25 30 31 in which for small animals
and
children, blood is impelled in external CPR predominantly
by the
cardiac pump mechanism (for example, Tpfactor

0.25), whereas
in
larger animals and adult humans, blood is impelled predominantly
by the
thoracic pump mechanism (for example, Tpfactor

0.75).

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Figure 3. Driving pressure waveforms for phased chest and
abdominal compression and decompression. Pchest is positive chest
compression; Pacd, active chest decompression; Pabd, positive abdominal
compression; and Paad, active abdominal decompression.
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Test Cases and Validation
The spreadsheet code was validated by solution of 12 simple test
cases for very small or very large values of the resistances and
compliances and by establishment of a model of the normal adult
circulation using Tpfactor=0. This model had an aortic blood pressure
of 120/82 mm Hg and a cardiac output of 4.9 L/min for a heart
rate of 80 bpm, closely approximating the textbook normal values of
120/80 mm Hg and 5.0 L/min.
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Results
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Alternative CPR Methods in Adult Human Models
Figure 4a

, 4b

, and 4c

illustrates
5-channel pressure records
after 20 cycles of CPR for the normal
human circulatory model
as shown in Table 2

during a simulation of
continuous standard
CPR, IAC-CPR, or ACD-CPR, respectively. In Figure 4

, the peak
positive abdominal pressure for IAC-CPR is 110 mm Hg,
and the
maximal negative intrathoracic pressure for ACD-CPR is
-20 mm
Hg, approximating published values for the 2
techniques.
1 2 32 33 34 35 In this model, the thoracic pump
factor is 0.75
to simulate an adult patient in whom the thoracic pump
mechanism
is dominant but there is some degree of selective cardiac
compression.
25 The parameters in Table 2

were
used for this and all subsequent
simulations, unless explicitly stated
otherwise. Figure 4a

illustrates
steady-state pressures generated by
standard CPR.
IAC-CPR
Comparison of the pressure waveforms in Figure 4a
and 4b
shows the
mechanism of +110 mm Hg interposed abdominal compression CPR. The
abdominal venous pressure pulse induces increased right heart filling
pressure during IAC and consequent faster pump emptying during chest
compression compared with standard CPR. Faster pump filling is caused
by larger pressure gradients across the input valve from times 0.54 to
0.67 second of the cycle. Faster pump emptying is caused by the
Starling characteristic of the pump associated with greater filling
and, in turn, larger pressure gradients across the aortic valve during
ejection. With the addition of IAC, cardiac output increases from 1.3
to 2.4 L/min, and mean systemic perfusion pressure
(SPP=RAo-RRH) increases from 25 to 45
mm Hg compared with standard CPR. The abdominal aortic pressure
waveform (crosses in figure) leads the thoracic aortic pressure
waveform (squares) during the onset and peak of IAC, indicating
retrograde flow in the aorta. This action is similar to that of an
intra-aortic balloon pump.
ACD-CPR
Figure 4c
shows steady-state pressure waveforms for
-20 mm Hg ACD-CPR. Reduced pump pressure (pulmonary
vascular pressure) during diastole promotes faster pump
filling from
0.45 to 0.60 second into the cycle. Cardiac output is
increased from 1.3 to 1.6 L/min, and mean systemic perfusion pressure
is increased from 25 to 30 mm Hg compared with standard CPR. The
ACD-induced decrease in central venous pressure offsets the ACD-induced
decrease in thoracic aortic pressure, so that augmented perfusion
pressure is maintained.
The effects on systemic perfusion pressure of IAC and ACD are
similar to those reported for studies in experimental animals and in
human patients.1 32 36 37 38 39 Compared with standard CPR,
110 mm Hg IAC produced an 85% increase in total flow. In the
same model, -20 mm Hg ACD produced a 23% increase in total
flow. The present results in an independent mathematical model
confirm that the positive findings in animal studies and most clinical
studies are valid and are based on the fundamental anatomy and
physiology of the circulatory system.
Four-Phase Lifestick CPR
Although less well studied, Lifestick CPR is a recently developed
technique to combine the effects of IAC and ACD. The sticky,
self-adhesive compression pads of the Lifestick permit active
compression and decompression of both the chest and the abdomen.
Accurate simulation of Lifestick CPR is difficult, because actual
values of negative intra-abdominal pressure have not yet been reported.
If one estimates maximal decompression-phase pressure in the abdomen to
be -30 mm Hg, the results in Figure 4d
are obtained. With this
possible 4-phase technique, mean systemic perfusion pressure is 58
mm Hg. Total forward flow is 3.1 L/min2.5 times that of standard
CPR. Study of the pressure waveforms in Figure 4d
reveals that in
4-phase CPR, negative inferior vena cava pressure draws
blood out of the chest from 0 to 0.3 second into the cycle, widening
the systemic perfusion pressure. Positive inferior vena
cava pressure from 0.33 to 0.67 second promotes excellent pump
filling.
Influence of Chest Pump Mechanisms
Systemic perfusion pressures obtained by chest and abdominal
compression are dependent on the degree to which blood is impelled by
cardiac compression versus global intrathoracic pressure fluctuation.
In Figure 5
, mean systemic perfusion
pressure is plotted as a function of the thoracic pump factor for 4
possible CPR techniques: standard, IAC, ACD, and 4-phase Lifestick CPR.
Maximal compression or decompression pressures are those listed in
Table 2
. Although perfusion pressures for the augmented CPR techniques
are always better than those for standard CPR, the ratios of
experimental to standard perfusion pressures vary with the thoracic
pump factor. The relative benefit of IAC-CPR compared with standard
CPR, evident in Figure 5
, appears to be greater in a pure thoracic pump
model than in a pure cardiac pump model. Conversely, the relative
benefit of ACD-CPR appears to be greater in a pure cardiac pump model.
The apparent benefit of ACD-CPR is especially model-dependent and may
be greater in small-animal models, such as beagles, which permit more
cardiac compression, than in larger-animal models, including humans.
This effect might well explain the generally more dramatic and
favorable results with ACD in animal models compared with the overall
mixed results observed in humans.8

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Figure 5. Mean systemic perfusion pressure (SPP) generated by
standard and augmented CPR techniques in models with varying mechanisms
of blood flow. Effects of chest compression vary according to the
thoracic pump factor, ranging from 0 (no compression of the thoracic
aorta and superior vena cava) to 1.0 (same pressure applied to the
thoracic aorta and superior vena cava as is applied to the
heart).
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Discussion
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Mathematical models provide a good way to synthesize knowledge
about
complex systems in new and interesting ways and to explore
assumptions
about how the systems operate. The present mathematical
model
provides an independent test confirming the efficacy of
adjunctive
diastolic-phase maneuvers to augment perfusion
during CPR. It
offers a convenient and low-cost way to compare various
CPR
adjuncts in exactly the same test system, eliminating the need
to
extrapolate published results from one animal or clinical
model to
another. The results confirm that compression and decompression
of
either the chest or the abdomen can move blood in cardiac
arrest.
Importantly, the positive effects of IAC-CPR, ACD-CPR,
and 4-phase
Lifestick CPR can be predicted from fundamental
principles of
cardiovascular physiologythe definition
of compliance
and Ohms law.
Analysis of pressure waveforms suggests that these techniques
function primarily by pump priming. In IAC-CPR, the chest pump is
primed by positive pressure in the abdomen during thoracic recoil. In
ACD-CPR, the chest pump is primed by negative diastolic
pressure in the chest that draws blood centrally from extra-thoracic
veins. In 4-phase Lifestick CPR, these effects are combined so that
negative thoracic and positive abdominal pressures prime the chest
pump. In turn, positive thoracic and negative abdominal pressures prime
the abdominal pump.
Conclusions
The present mathematical model, based on fundamental aspects
of cardiovascular physiology, provides a recapitulation
and synthesis of abundant experimental and clinical evidence suggesting
that adjunctive compression and decompression of the chest and abdomen
can improve current standard CPR. Systemic perfusion pressure
achievable with IAC alone is approximately double that of standard CPR.
Systemic perfusion pressure achievable with full 4-phase CPR might
possibly exceed 3-fold that of current standard CPR. Improved perfusion
during IAC-CPR may not necessarily lead to better long-term survival,
especially when the underlying rhythm is asystole or electromechanical
dissociation.13 For the fraction of cardiac arrest victims
who can be saved, however, these techniques, performed by trained
healthcare providers, are valid and practical alternatives to standard
CPR and have a rational place in resuscitation protocols of the 21st
century.
Received April 20, 1999;
revision received June 29, 1999;
accepted July 9, 1999.
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