Neonatal Ventilator Graphics
A Clinical Guide
BY:
DR. AHMED HEGAZI
M.SC, MRCPCH
NICU-ADAN HOSPITAL
Evolution of ventilator
graphics
Principles of Pulmonary
Graphics
Principles of Pulmonary
Graphics
Waveforms
 Waveforms depict the relationship
between respiratory parameters and time
on a breath-to-breath basis.
 The three most commonly used signals
are pressure (cm H2O), volume (mL),
and flow (mL/s), and these three signals
describe the respiratory cycle.
 When displayed in aggregate, the cyclic
phases of respiration can be
appreciated.
Waveforms
Volume Waveform
 The volume waveform displays the
changes in delivered volume over time.
 It is determined by integrating the
inspiratory and expiratory flow signals.
 expired volume is usually a bit less
than inspired volume because of air
leak around the uncuffed neonatal
endotracheal tube.
Volume Waveform
Pressure Waveform
 The pressure waveform represents the
airway pressure throughout the
respiratory cycle.
 Virtually every newborn requiring
conventional mechanical ventilation
receives some degree of PEEP. Thus,
the waveform at end inspiration or the
initiation of inspiration is above the
baseline (zero) value.
Pressure Waveform
 Pressure rises during inspiration, reaching
its maximum value, or peak inspiratory
pressure (PIP), then declines during
expiration to the PEEP level.
 The area under a single cycle represents
the mean airway pressure (mean Paw).
 The difference between the PIP and the
PEEP is referred to as the amplitude or
delta P.
Techniques to Alter Mean Airway
Pressure
Pressure Waveform
Changes in PIP and PEEP
Change in Inspiratory Time
Pressure Overshoot
 Pressure control and pressure
support ventilation utilize an
accelerating-decelerating inspiratory
flow waveform.
 If set too high, it may deliver pressure
too rapidly for the patient’s need. This
creates a condition known as pressure
overshoot.
Pressure Overshoot
 The pressure waveform exhibits a
notch and double peak at PIP. Most
ventilators have an adjustable rise
time function to respond to this.
Flow Waveform
 The flow waveform is the most complex
because its inspiratory and expiratory phases
each have two components.
 the baseline represents a zero flow state,
meaning that no gas is entering or leaving the
airway.
 anything above the baseline (positive value)
represents inspiratory flow (gas flow into the
patient), and conversely, anything below the
baseline (negative value) represents expiratory
flow (gas flow from the patient).
Flow Waveform
Flow Waveform
Two major ways in which inspiratory
flow can be delivered to the patient:
 Variable (sinusoidal wave):
pressure control
pressure support ventilation.
 Constant (square wave):
volume targeted ventilation
Flow Waveform
 Flow wave form during volume control
ventilation. Inspiratory flow is
continuous, rather than variable, and
produces a characteristic “square”
waveform
Flow Waveform
 Increased Expiratory Resistance
1. shallow accelerating expiratory flow
and decreased peak expiratory flow
rate.
2. a longer time to return to baseline
during decelerating expiratory flow
Flow Waveform
 Gas Trapping
the decelerating expiratory
component never reaches the
baseline (zero flow state) before the
subsequent breath is initiated.
Flow Waveform
Gas Trapping
 It occurs when the expiratory flow is less
than the inspiratory flow, resulting in
more gas entering than leaving the lung.
 This is a potentially dangerous situation
that can lead to alveolar rupture and air
leak.
 Now, careful observation of the flow
waveform can detect this condition,
allowing time to avoid its consequences.
Flow Waveform
 Gas Trapping (how to intervene?)
1. decreasing the ventilator rate.
2. decreasing the flow rate.
3. shortening the inspiratory time.
4. increasing the PEEP.
depending upon the clinical condition,
ventilator modality, and underlying
pathophysiology.
Cycling Mechanisms
Cycling refers to the mechanism that
transitions inspiration to expiration and
expiration to inspiration.
 Time cycling mechanism:
Cycling Mechanisms
 Flow-cycling
As a breath is delivered, the ventilator
notes the peak inspiratory flow rate. The
inspiratory flow rate then decelerates, by
5-25%, the exhalation valve will open,
discharging the remainder of inspiratory
flow
Cycling Mechanisms
Flow-cycling
 Flow-cycling takes advantage of the
natural pattern of breathing by
focusing on the baby’s inspiratory flow.
 It prevents gas trapping and the
inversion of the inspiratory:expiratory
ratio during patient-triggered
ventilation.
 It can be used in conjunction with
time-cycling, in that a breath will be
terminated by whichever condition
Endotracheal Tube Leaks
 Because cuffed ETTs are not used in
newborns, there will almost always be
some degree of leak around the ETT.
 Most of this occurs during inspiration when
pressure is higher.
 A significant leak may divert gas flow, such
that the decelerating inspiratory flow may
never reach the termination point. The
breath will then be time-cycled, but often
with inadequate pressure or volume
Endotracheal Tube Leaks
Endotracheal Tube Leaks
 The flow waveform, has virtually no
expiratory component.
 the actual end of the expiratory volume
waveform is shown by (the arrows, and by
the short blue line) which is followed by a
reset artifact (yellow coloured line dropping
to the zero baseline).
 The volume waveform, in the lower panel,
shows almost no expired volume.
 This also results in auto-cycling, with a
rate of 75/m.
Auto-cycling (Auto-triggering)
 When it occurs, there may be rapid
delivery of mechanical breaths, inducing
hypocapnia as well as the risk of lung
injury.
 Note the relative uniformity of the
breaths, which helps to distinguish this
from just rapid breathing, where there
will be some variability
Auto-cycling (Auto-triggering)
 It may occur during flow-triggered
ventilation if the ventilator interprets an
aberrant flow signal as patient effort.
 This can happen if there is a leak that
exceeds the trigger threshold, and it
may occur anywhere in the path of gas
flow.
 It may also occur from excessive
condensation in the ventilator circuit
(“rainout”).
Pulmonary Mechanics and
Loops
 pressure, flow, and volume to time, may be
presented relative to each other “commonly
referred to as loops”.
 The two most frequently used in clinical practice
are the pressure-volume (P-V) loop and the
flow-volume (F-V) loop.
 The interpretation of which can provide valuable
information about the mechanical properties of
the lung, how it is “performing” on a breath-to-
breath basis, and how it responds to changes in
pathophysiology, mechanical ventilation
The P-V Loop
The P-V Loop
The P-V Loop
 It displays the relationship of pressure and
volume during a single breath.
 the origin of the loop does not start at the
origin of the graph because of the application
of positive end-expiratory pressure (PEEP).
 The P-V loop provides
valuable information about
lung mechanics.
The dotted line is the compliance axis , a
measure of the stiffness or elasticity of the
lung.
The P-V Loop
“Compliance”
 Compliance is defined as the change in
volume divided by the change in pressure.
Thus, if a 1 cm H2O increase in pressure
results in a 1 mL increase in lung volume,
the axis will be 45°.
 As compliance decreases,
the axis will shift downward
and to the right. Conversely,
as compliance improves,
the axis will shift upward and to the left.
The P-V Loop
“work of breathing”
 The work of breathing can be qualitatively
estimated by the P-V loop.
 It is the area bounded by the inflation limb
and a horizontal line connecting the PIP with
the y-axis.
 As the compliance
decreases and the loop
shifts downward and to
the right, this area
increases and more pressure must be
applied to achieve the same lung volume.
The P-V Loop
“resistance”
 A line drawn from the midpoint of the
inflation limb to the compliance axis is a
measure of inspiratory resistance.
 a line drawn from the midpoint of the
deflation limb to the compliance axis is
a measure of expiratory resistance.
The P-V Loop
“Hysteresis”
 Hysteresis is a term that is used to
describe the difference between the
inflation and the deflation limbs and is
determined by the elastic properties of the
lung.
 Under normal circumstances, the shape of
the P-V loop is oval, resembling a football.
Hysteresis, thus represents the resistive
work of breathing.
The F-V Loop
The F-V Loop
The F-V Loop
 describes the pattern of airflow during
tidal breathing.
 Volume is shown on the x-axis and flow
is shown on the y-axis.
 Like the flow waveform, inspiratory and
expiratory flows are in opposite
directions.
The F-V Loop
 Inspiration begins at the origin of the
graph (zero flow) and increases until it
reaches the peak inspiratory flow rate
(PIFR).
 Flow then decelerates, and reaches the
zero flow state at the point where it
crosses the volume axis, representing the
delivered V
The F-V Loop
 Expiratory flow begins with the accelerating
phase, reaches the peak expiratory flow rate
(PEFR).
 Then, it decelerates until it returns to the origin
and another zero flow state at end expiration.
 The general shape of the loop should be round
or ovoid and the two halves (inspiratory and
expiratory) should be close to mirror images.
Decreased Compliance
Lung Compliance
Lung Inflation
Lung Inflation
“Hyperinflation”
 As the lung approaches maximum filling and tissue
distensibility becomes more limited, the compliance
will decrease, resulting in less volume gain per unit of
incremental pressure, and the slope of the
compliance axis will shift downward.
 This creates an upper inflection point on the P-V
inflation limb and graphically creates a “penguin
beak” or “duck bill” appearance to the loop.
Lung Inflation
“Hyperinflation”
 Hyperinflation can be quantified by using a metric
known as the C20/C ratio (Fisher, 1988).
 The C20/C ratio examines the slope of the last 20 %
of the inflation limb and compares it with the linear
portion of the curve.
 If the curve remained linear to the peak pressure, the
ratio would remain at 1.0; if the loop begins to bend to
the right, the slope will decrease and the ratio will
decrease to <1.0.
Lung Inflation “Hyperinflation”
Lung Inflation “Underinflation”
 Lung inflation below the FRC will also
produce a slope that is less than the linear
portion of the compliance axis.
 Little volume is being delivered at the lower
end of the inflation limb until the opening
pressure has been exceeded and volume
starts to increase, creating a lower inflection
point in the loop.
Lung Inflation “Underinflation”
 The loop looks more like a box than a
football.
 Applied pressure does not deliver any
effective volume for much of the inspiratory
phase.
 Similarly, during deflation the lung rapidly de-
recruits when the critical closing pressure is
reached.
Pressure Overshoot
Pressure Overshoot
 Ventilator modalities that use variable inspiratory
flow, such as PC and PS, may produce flow rates
that exceed the mechanical properties of the lung
and lead to hyperinflation.
 the P-V curve shows a bulge or a notch, and the
pressure waveform shows a double peak at PIP.
 The flow rate may be modulated by a feature
known as rise time, available on most devices,
which allows a qualitative adjustment in the flow
rate.
Air Hunger
 If the delivered Vt is inadequate to meet the
patient’s need, air hunger may develop.
 In this situation the baby may be noted to be
“pulling” or displaying increased work of
breathing.
 This creates a distinctive pattern on the P-V
loop, with a “figure of eight” reversal of the
inflation and deflation limbs at the top of the
loop.
Increased Inspiratory
Resistance
 Excessive distance between the inflation
limb and the compliance axis represents
increased inspiratory resistance.
 This pattern can often be corrected by
increasing inspiratory flow, inspiratory
time, or PEEP.
Elevated Inspiratory
Resistance
 Rather than having an oval or circular
appearance with a discernible peak
inspiratory flow rate, the loop is flat across
most of the inspiratory phase. This suggests
an extrathorcic obstruction
Increased Expiratory
Resistance
 It conversely, produces changes in the
deflation limb of the P-V loop, in which
it may be separated or bowed from the
compliance axis.
 Adjustments to correct this might
include increases in expiratory time
and/or PEEP.
Elevated Expiratory
Resistance
 Rather than having an ovular or circular
appearance, the loop looks compressed due to
reduction in the PEFR, suggestive of obstructive
airway disease.
Surfactant Administration
 Surfactant administration to a newborn
with RDS will lower alveolar surface
tension and improve pulmonary
compliance.
 Because this can happen rapidly, there is
a risk of overdistension of the lung if
pressure is not reduced rapidly enough.
Surfactant Administration
Surfactant Administration
Fixed Airway Obstruction
 both inspiratory and expiratory resistances may
be elevated, resulting in a “compression” of the
F-V loop with lower PIFR and PEFR & Both
inspiratory and expiratory portions of the loop
are flattened.
Evaluation of Bronchodilator
Therapy
Evaluation of Bronchodilator
Therapy
 . There has been a significant improvement in
both the PIFR and PEFR. The loop has
“opened” and the tidal volume delivery has
also improved
Turbulence
 This results from secretions or condensation in
the airway or the ventilator circuit. Turbulence
creates a “noisy” flow signal, which alters both
the flow waveform and the F-V loop.
Turbulence
examine the baby and to look carefully for:
 secretions
 condensation
 or other obstructive matter in the airway,
endotracheal tube, sensor, or ventilator circuit
Some centers have used this information to
determine when to suction a mechanically
ventilated baby rather than performing
suctioning on a routine basis.
Excessive Dynamic Airway
Collapse
 note the “notching” at end expiration.
Excessive Dynamic Airway
Collapse
 EDAC is a condition that may be
congenital or acquired, in which there is
airway luminal narrowing during
expiration creating a severe expiratory
flow restriction.
 The appearance of the F-V loop shows
a rapid decline from the PEFR after a
sharp acceleration to peak
Ventilator graphics
Ventilator graphics

Ventilator graphics

  • 2.
    Neonatal Ventilator Graphics AClinical Guide BY: DR. AHMED HEGAZI M.SC, MRCPCH NICU-ADAN HOSPITAL
  • 3.
  • 4.
  • 5.
  • 6.
    Waveforms  Waveforms depictthe relationship between respiratory parameters and time on a breath-to-breath basis.  The three most commonly used signals are pressure (cm H2O), volume (mL), and flow (mL/s), and these three signals describe the respiratory cycle.  When displayed in aggregate, the cyclic phases of respiration can be appreciated.
  • 7.
  • 8.
    Volume Waveform  Thevolume waveform displays the changes in delivered volume over time.  It is determined by integrating the inspiratory and expiratory flow signals.  expired volume is usually a bit less than inspired volume because of air leak around the uncuffed neonatal endotracheal tube.
  • 9.
  • 10.
    Pressure Waveform  Thepressure waveform represents the airway pressure throughout the respiratory cycle.  Virtually every newborn requiring conventional mechanical ventilation receives some degree of PEEP. Thus, the waveform at end inspiration or the initiation of inspiration is above the baseline (zero) value.
  • 11.
    Pressure Waveform  Pressurerises during inspiration, reaching its maximum value, or peak inspiratory pressure (PIP), then declines during expiration to the PEEP level.  The area under a single cycle represents the mean airway pressure (mean Paw).  The difference between the PIP and the PEEP is referred to as the amplitude or delta P.
  • 12.
    Techniques to AlterMean Airway Pressure
  • 13.
  • 14.
  • 15.
  • 16.
    Pressure Overshoot  Pressurecontrol and pressure support ventilation utilize an accelerating-decelerating inspiratory flow waveform.  If set too high, it may deliver pressure too rapidly for the patient’s need. This creates a condition known as pressure overshoot.
  • 17.
    Pressure Overshoot  Thepressure waveform exhibits a notch and double peak at PIP. Most ventilators have an adjustable rise time function to respond to this.
  • 18.
    Flow Waveform  Theflow waveform is the most complex because its inspiratory and expiratory phases each have two components.  the baseline represents a zero flow state, meaning that no gas is entering or leaving the airway.  anything above the baseline (positive value) represents inspiratory flow (gas flow into the patient), and conversely, anything below the baseline (negative value) represents expiratory flow (gas flow from the patient).
  • 19.
  • 20.
    Flow Waveform Two majorways in which inspiratory flow can be delivered to the patient:  Variable (sinusoidal wave): pressure control pressure support ventilation.  Constant (square wave): volume targeted ventilation
  • 21.
    Flow Waveform  Flowwave form during volume control ventilation. Inspiratory flow is continuous, rather than variable, and produces a characteristic “square” waveform
  • 22.
    Flow Waveform  IncreasedExpiratory Resistance 1. shallow accelerating expiratory flow and decreased peak expiratory flow rate. 2. a longer time to return to baseline during decelerating expiratory flow
  • 23.
    Flow Waveform  GasTrapping the decelerating expiratory component never reaches the baseline (zero flow state) before the subsequent breath is initiated.
  • 24.
    Flow Waveform Gas Trapping It occurs when the expiratory flow is less than the inspiratory flow, resulting in more gas entering than leaving the lung.  This is a potentially dangerous situation that can lead to alveolar rupture and air leak.  Now, careful observation of the flow waveform can detect this condition, allowing time to avoid its consequences.
  • 25.
    Flow Waveform  GasTrapping (how to intervene?) 1. decreasing the ventilator rate. 2. decreasing the flow rate. 3. shortening the inspiratory time. 4. increasing the PEEP. depending upon the clinical condition, ventilator modality, and underlying pathophysiology.
  • 26.
    Cycling Mechanisms Cycling refersto the mechanism that transitions inspiration to expiration and expiration to inspiration.  Time cycling mechanism:
  • 27.
    Cycling Mechanisms  Flow-cycling Asa breath is delivered, the ventilator notes the peak inspiratory flow rate. The inspiratory flow rate then decelerates, by 5-25%, the exhalation valve will open, discharging the remainder of inspiratory flow
  • 28.
    Cycling Mechanisms Flow-cycling  Flow-cyclingtakes advantage of the natural pattern of breathing by focusing on the baby’s inspiratory flow.  It prevents gas trapping and the inversion of the inspiratory:expiratory ratio during patient-triggered ventilation.  It can be used in conjunction with time-cycling, in that a breath will be terminated by whichever condition
  • 29.
    Endotracheal Tube Leaks Because cuffed ETTs are not used in newborns, there will almost always be some degree of leak around the ETT.  Most of this occurs during inspiration when pressure is higher.  A significant leak may divert gas flow, such that the decelerating inspiratory flow may never reach the termination point. The breath will then be time-cycled, but often with inadequate pressure or volume
  • 30.
  • 31.
    Endotracheal Tube Leaks The flow waveform, has virtually no expiratory component.  the actual end of the expiratory volume waveform is shown by (the arrows, and by the short blue line) which is followed by a reset artifact (yellow coloured line dropping to the zero baseline).  The volume waveform, in the lower panel, shows almost no expired volume.  This also results in auto-cycling, with a rate of 75/m.
  • 32.
    Auto-cycling (Auto-triggering)  Whenit occurs, there may be rapid delivery of mechanical breaths, inducing hypocapnia as well as the risk of lung injury.  Note the relative uniformity of the breaths, which helps to distinguish this from just rapid breathing, where there will be some variability
  • 33.
    Auto-cycling (Auto-triggering)  Itmay occur during flow-triggered ventilation if the ventilator interprets an aberrant flow signal as patient effort.  This can happen if there is a leak that exceeds the trigger threshold, and it may occur anywhere in the path of gas flow.  It may also occur from excessive condensation in the ventilator circuit (“rainout”).
  • 34.
    Pulmonary Mechanics and Loops pressure, flow, and volume to time, may be presented relative to each other “commonly referred to as loops”.  The two most frequently used in clinical practice are the pressure-volume (P-V) loop and the flow-volume (F-V) loop.  The interpretation of which can provide valuable information about the mechanical properties of the lung, how it is “performing” on a breath-to- breath basis, and how it responds to changes in pathophysiology, mechanical ventilation
  • 35.
  • 36.
  • 37.
    The P-V Loop It displays the relationship of pressure and volume during a single breath.  the origin of the loop does not start at the origin of the graph because of the application of positive end-expiratory pressure (PEEP).  The P-V loop provides valuable information about lung mechanics. The dotted line is the compliance axis , a measure of the stiffness or elasticity of the lung.
  • 38.
    The P-V Loop “Compliance” Compliance is defined as the change in volume divided by the change in pressure. Thus, if a 1 cm H2O increase in pressure results in a 1 mL increase in lung volume, the axis will be 45°.  As compliance decreases, the axis will shift downward and to the right. Conversely, as compliance improves, the axis will shift upward and to the left.
  • 39.
    The P-V Loop “workof breathing”  The work of breathing can be qualitatively estimated by the P-V loop.  It is the area bounded by the inflation limb and a horizontal line connecting the PIP with the y-axis.  As the compliance decreases and the loop shifts downward and to the right, this area increases and more pressure must be applied to achieve the same lung volume.
  • 40.
    The P-V Loop “resistance” A line drawn from the midpoint of the inflation limb to the compliance axis is a measure of inspiratory resistance.  a line drawn from the midpoint of the deflation limb to the compliance axis is a measure of expiratory resistance.
  • 41.
    The P-V Loop “Hysteresis” Hysteresis is a term that is used to describe the difference between the inflation and the deflation limbs and is determined by the elastic properties of the lung.  Under normal circumstances, the shape of the P-V loop is oval, resembling a football. Hysteresis, thus represents the resistive work of breathing.
  • 42.
  • 43.
  • 44.
    The F-V Loop describes the pattern of airflow during tidal breathing.  Volume is shown on the x-axis and flow is shown on the y-axis.  Like the flow waveform, inspiratory and expiratory flows are in opposite directions.
  • 45.
    The F-V Loop Inspiration begins at the origin of the graph (zero flow) and increases until it reaches the peak inspiratory flow rate (PIFR).  Flow then decelerates, and reaches the zero flow state at the point where it crosses the volume axis, representing the delivered V
  • 46.
    The F-V Loop Expiratory flow begins with the accelerating phase, reaches the peak expiratory flow rate (PEFR).  Then, it decelerates until it returns to the origin and another zero flow state at end expiration.  The general shape of the loop should be round or ovoid and the two halves (inspiratory and expiratory) should be close to mirror images.
  • 47.
  • 48.
  • 49.
  • 50.
    Lung Inflation “Hyperinflation”  Asthe lung approaches maximum filling and tissue distensibility becomes more limited, the compliance will decrease, resulting in less volume gain per unit of incremental pressure, and the slope of the compliance axis will shift downward.  This creates an upper inflection point on the P-V inflation limb and graphically creates a “penguin beak” or “duck bill” appearance to the loop.
  • 51.
    Lung Inflation “Hyperinflation”  Hyperinflationcan be quantified by using a metric known as the C20/C ratio (Fisher, 1988).  The C20/C ratio examines the slope of the last 20 % of the inflation limb and compares it with the linear portion of the curve.  If the curve remained linear to the peak pressure, the ratio would remain at 1.0; if the loop begins to bend to the right, the slope will decrease and the ratio will decrease to <1.0.
  • 52.
  • 53.
    Lung Inflation “Underinflation” Lung inflation below the FRC will also produce a slope that is less than the linear portion of the compliance axis.  Little volume is being delivered at the lower end of the inflation limb until the opening pressure has been exceeded and volume starts to increase, creating a lower inflection point in the loop.
  • 54.
    Lung Inflation “Underinflation” The loop looks more like a box than a football.  Applied pressure does not deliver any effective volume for much of the inspiratory phase.  Similarly, during deflation the lung rapidly de- recruits when the critical closing pressure is reached.
  • 55.
  • 56.
    Pressure Overshoot  Ventilatormodalities that use variable inspiratory flow, such as PC and PS, may produce flow rates that exceed the mechanical properties of the lung and lead to hyperinflation.  the P-V curve shows a bulge or a notch, and the pressure waveform shows a double peak at PIP.  The flow rate may be modulated by a feature known as rise time, available on most devices, which allows a qualitative adjustment in the flow rate.
  • 57.
    Air Hunger  Ifthe delivered Vt is inadequate to meet the patient’s need, air hunger may develop.  In this situation the baby may be noted to be “pulling” or displaying increased work of breathing.  This creates a distinctive pattern on the P-V loop, with a “figure of eight” reversal of the inflation and deflation limbs at the top of the loop.
  • 58.
    Increased Inspiratory Resistance  Excessivedistance between the inflation limb and the compliance axis represents increased inspiratory resistance.  This pattern can often be corrected by increasing inspiratory flow, inspiratory time, or PEEP.
  • 59.
    Elevated Inspiratory Resistance  Ratherthan having an oval or circular appearance with a discernible peak inspiratory flow rate, the loop is flat across most of the inspiratory phase. This suggests an extrathorcic obstruction
  • 60.
    Increased Expiratory Resistance  Itconversely, produces changes in the deflation limb of the P-V loop, in which it may be separated or bowed from the compliance axis.  Adjustments to correct this might include increases in expiratory time and/or PEEP.
  • 61.
    Elevated Expiratory Resistance  Ratherthan having an ovular or circular appearance, the loop looks compressed due to reduction in the PEFR, suggestive of obstructive airway disease.
  • 62.
    Surfactant Administration  Surfactantadministration to a newborn with RDS will lower alveolar surface tension and improve pulmonary compliance.  Because this can happen rapidly, there is a risk of overdistension of the lung if pressure is not reduced rapidly enough.
  • 63.
  • 64.
  • 65.
    Fixed Airway Obstruction both inspiratory and expiratory resistances may be elevated, resulting in a “compression” of the F-V loop with lower PIFR and PEFR & Both inspiratory and expiratory portions of the loop are flattened.
  • 66.
  • 67.
    Evaluation of Bronchodilator Therapy . There has been a significant improvement in both the PIFR and PEFR. The loop has “opened” and the tidal volume delivery has also improved
  • 68.
    Turbulence  This resultsfrom secretions or condensation in the airway or the ventilator circuit. Turbulence creates a “noisy” flow signal, which alters both the flow waveform and the F-V loop.
  • 69.
    Turbulence examine the babyand to look carefully for:  secretions  condensation  or other obstructive matter in the airway, endotracheal tube, sensor, or ventilator circuit Some centers have used this information to determine when to suction a mechanically ventilated baby rather than performing suctioning on a routine basis.
  • 70.
    Excessive Dynamic Airway Collapse note the “notching” at end expiration.
  • 71.
    Excessive Dynamic Airway Collapse EDAC is a condition that may be congenital or acquired, in which there is airway luminal narrowing during expiration creating a severe expiratory flow restriction.  The appearance of the F-V loop shows a rapid decline from the PEFR after a sharp acceleration to peak