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Chapter 11
Ventilation
Learning Objectives
• Describe the physiologic functions provided by
ventilation.
• Describe the pressure gradients responsible for gas
flow, diffusion, and lung inflation.
• Identify the forces that oppose gas movement into
and out of the lungs.
• Describe how surface tension contributes to lung
recoil.
Copyright © 2017 Elsevier Inc. All Rights Reserved. 2
Learning Objectives
• Describe how lung, chest wall, and total compliance
are related.
• State the factors that affect resistance to breathing.
• Describe how various lung diseases affect the work
of breathing.
• State why ventilation is not evenly distributed
throughout the lung.
Copyright © 2017 Elsevier Inc. All Rights Reserved. 3
Learning Objectives
• Describe how the time constants affect alveolar
filling and emptying.
• Identify the factors that affect alveolar ventilation.
• State how to calculate alveolar ventilation, dead
space, and the VD/VT ratio.
Copyright © 2017 Elsevier Inc. All Rights Reserved. 4
Introduction to Ventilation
• Ventilation is the process of moving gas (usually air) in
and out of the lungs
• Ventilation is to be distinguished from respiration, which
refers to the physiologic processes of oxygen use at the
cellular level
• In health: Ventilation is regulated to meet the body’s needs under
a wide range of conditions
• In disease: This process can be markedly disrupted and often
result in inadequate ventilation and /or increased work of
breathing
Copyright © 2017 Elsevier Inc. All Rights Reserved. 5
Mechanics of Ventilation
• Cycles of ventilation: inspiration and expiration
• Tidal volume (VT): volume of gas moving in and out
of the respiratory tract during inspiration or
expiration
• The Vt refreshes the gas present in the lung,
removing CO2, and supplying O2 TO MEET METABOLIC
NEEDS
Copyright © 2017 Elsevier Inc. All Rights Reserved. 6
Pressure Differences During
Breathing
• Gases move due to pressure gradients
• Produced by thoracic expansion/contraction
• Do to elastic properties of airways, alveoli, and chest wall
• Transrespiratory pressure (PTR)
• Everything that exists between pressure measured at airway opening (PAO) and
pressure measured at body surface (PBS)
• PTR = PAO – PBS
• Equation follows direction of flow
• PAO is higher than PBS
• Components of transrespiratory pressure include:
• Airway, lungs, and chest wall
• This gradient causes gas flow in and out of lungs
Copyright © 2017 Elsevier Inc. All Rights Reserved. 7
Pressure Differences During
Breathing
Copyright © 2017 Elsevier Inc. All Rights Reserved. 8
Pressure Differences During
Breathing
• Transairway pressure (PTAW)
• PTAW = PAO– PA
• Whatever exists between pressure measured at airway opening and pressure
measured in alveoli of lungs
• Transalveolar pressure (PTA)
• PTA = PA– Ppl
• Whatever exists between pressure measured in model alveolus and pressure
measured in pleural space (Ppl).
• Trans-chestwall pressure (PTCW)
• Chest wall exists between pressure measured in pleural space and pressure on
body surface
• PTCW = Ppl – PBS
Copyright © 2017 Elsevier Inc. All Rights Reserved. 9
Pressure Differences During
Breathing
• Transpulmonary pressure difference (PTP)
• Pulmonary system (airways and alveolar region), defined:
• PTP = PAO – Ppl
• Pressures must be measured to derive mechanical properties of
pulmonary system
• Under either static or dynamic (breathing) conditions
• Note, some confusion arises from:
• PTA = PAO – Ppl but only under static conditions
• Considered a special case of PTP = PAO – Ppl
• Static conditions can be imposed during mechanical ventilation
• Through use of inspiratory hold maneuver
Copyright © 2017 Elsevier Inc. All Rights Reserved. 10
Pressure Differences During
Breathing
• Transthoracic pressure difference (PTT)
• PTT = PA – PBS
• Causes gas to flow into and out of alveoli during
breathing
• Beginning of inspiration in spontaneous breathing
subject, PA is subatmospheric compared to PAO
• Causes air to flow into alveoli
• Beginning of exhalation is opposite
• PA is higher than PAO
• Causing air to flow out of the airway
Copyright © 2017 Elsevier Inc. All Rights Reserved. 11
Pressure Differences During
Breathing
• At end of resting exhalation, Ppl, is normally 5
cm H2O; PA = zero, there is no gas flow
• PTP is also approximately 5 cm H2O in resting
state
• This positive end expiratory PTP maintains lung
at its resting volume (i.e., functional residual
capacity, FRC)
Copyright © 2017 Elsevier Inc. All Rights Reserved. 12
Pressure Differences During
Breathing
• Inspiration begins
• When muscular effort expands the thorax
• Thoracic expansion causes a decrease in Ppl
• Causes positive change on expiratory PTP and PTA,
which induces flow into lungs
• Inspiratory flow is proportional to (+) change in
transairway pressure difference
• The higher the change in PTA, the higher the flow
• Ppl continues to decrease until the end of inspiration
Copyright © 2017 Elsevier Inc. All Rights Reserved. 13
Pressure Differences During
Breathing
• Beginning of expiration
• Thoracic recoil causes Ppl to start to rise
• Thus, transpulmonary pressure difference starts to decrease
• PTP is decreasing; opposite of inspiration
• So flow is in opposite (negative) direction
• Driving force for expiratory flow is energy stored in combined elastances of lungs and
chest wall
• Pleural pressures: always negative (subatmospheric) during
normal inspiration and exhalation
• During forced inspiration (big downward movement of
diaphragm), pleural pressure can drop up to –50 cm H2O
Copyright © 2017 Elsevier Inc. All Rights Reserved. 14
Pressure Differences During
Breathing
Pmus = 0
= (Elastance × Volume) + (Resistance × Flow)
• Rearranging the formula, we get:
(Elastance  Volume) = − (Resistance  Flow)
= Resistance  (− Flow)
• Flow is negative (indicating expiration)
• The driving force for expiratory flow is the energy stored in the
combined elastances of lungs and chest wall
Copyright © 2017 Elsevier Inc. All Rights Reserved. 15
Pressure Differences During Breathing
Copyright © 2017 Elsevier Inc. All Rights Reserved. 16
Forces Opposing Lung Inflation
• Lungs have tendency to recoil inward, while chest
wall has tendency to move outwards
• Those opposing forces keep lung at its resting volumes
(FRC)
Copyright © 2017 Elsevier Inc. All Rights Reserved. 17
Forces Opposing Lung Inflation
• Elastic opposition to ventilation
• Elastic and collagen fibers provide resistance to lung stretch
• Application of pressure causes stretch
• Greater pressure causes greater stretch until maximum
inflation is reached
• Deflation is passive recoil; less force is required to maintain
same volume
• During deflation, lung volume at any given pressure is slightly
greater than during inflation.
• Difference between inflation and deflation curves is hysteresis
Copyright © 2017 Elsevier Inc. All Rights Reserved. 18
Forces Opposing Lung Inflation
• Hysteresis indicates factors other than simple elastic
tissue forces are present
• Major factor, especially in sick lungs: opening of
collapsed alveoli during inspiration that tend to stay
open during expiration until very low lung volumes
are reached
Copyright © 2017 Elsevier Inc. All Rights Reserved. 19
Forces Opposing Lung Inflation
• Chest wall elastance and lung elastance are
connected in a series:
• Have same flow and change in volume but do not
have same pressure differences
• Elastance of respiratory system (ERS) = sum of lung
(pulmonary) elastance (EL) and chest wall elastance
(ECW)
• Applies to both natural and artificial airways (ETT)
Copyright © 2017 Elsevier Inc. All Rights Reserved. 20
Copyright © 2017 Elsevier Inc. All Rights Reserved. 21
Forces Opposing Lung Inflation
Copyright © 2017 Elsevier Inc. All Rights Reserved. 22
Surface Tension Forces
• Hysteresis partly caused by surface tension
• Surface tension opposes lung inflation
• If surface tension is removed, hysteresis becomes very small
• Lung recoil occurs due to tissue elasticity and surface tension
• Pulmonary surfactant reduces lung surface tension
• Produced in alveolar type II pneumocytes
• Surfactant stabilizes alveoli by preventing collapse
• When surface area decreases, ability of pulmonary surfactant to
lower surface tension increases
Copyright © 2017 Elsevier Inc. All Rights Reserved. 23
Surface Tension Forces (Cont.)
Copyright © 2017 Elsevier Inc. All Rights Reserved. 24
Lung Compliance
• CL defined as change in volume (ΔV) per unit of change in
pressure (ΔP) difference across structure or
CL = ΔV L (normal 0.2 L/cm H2O)
ΔP cm H2O
• Pulmonary pathology alters CL
• Emphysema , obstructive lung disease, increases CL (loss elastic
tissue, lungs more distensible)
• Large changes in volume for small pressure changes
• Fibrosis, restrictive lung disease, decreases CL (↑ elastic tissue)
• Smaller volume change for any change in pressure
• Stiffer lungs, usually with reduced volume
Copyright © 2017 Elsevier Inc. All Rights Reserved. 25
Lung Compliance
Copyright © 2017 Elsevier Inc. All Rights Reserved. 26
Relationship Between
Chest Wall and Lung
• Lungs and chest wall recoil in opposite
directions
• Compliance in both is ~0.2 L/cm H2O
• Each oppose other, resulting in system compliance
of ~0.1 L/cm H2O
• FRC established at resting lung level where
tendency of chest wall to expand equals that of
lungs to collapse
• Occurs at ~40% TLC
Copyright © 2017 Elsevier Inc. All Rights Reserved. 27
Relationship Between
Chest Wall and Lung (Cont.)
Copyright © 2017 Elsevier Inc. All Rights Reserved. 28
Frictional Resistance to
Ventilation
• Tissue viscous resistance (~20% of the total resistance to lung inflation )
• Frictional forces during displacement of lungs, ribs, diaphragm, and abdominal
organs
• Airway resistance (~80% of of the frictional resistance to ventilation)
• Gas flow causes frictional resistance
Airway radius exponential effect (r4) on resistance
• Artificial airway size or bronchospasm
• Resistance is highest at nose (50% of total resistance) falls to ~20% of total
resistance at small airways
• Resistance in nonventilated patients is measured in pulmonary function
laboratory
Copyright © 2017 Elsevier Inc. All Rights Reserved. 29
Frictional Resistance to Ventilation
(Cont.)
Copyright © 2017 Elsevier Inc. All Rights Reserved. 30
Frictional Resistance to Ventilation
(Cont.)
Copyright © 2017 Elsevier Inc. All Rights Reserved. 31
Static Versus Dynamic Mechanics
• Resistance and compliance can be evaluated under static
or dynamic conditions
• Static implies flow throughout respiratory system has
ceased and all ventilatory muscle activity is absent
• Static conditions can be imposed with an inspiratory pause
when patient is sedated and being mechanically ventilated
• Dynamic is when flow of airway opening = 0
• Useful for lung protective ventilation strategies in patients w/
acute lung injury and acute respiratory distress syndrome
Copyright © 2017 Elsevier Inc. All Rights Reserved. 32
Static Versus Dynamic Mechanics
• Due to different time constants, mechanics estimated
during static conditions will yield different values than
when evaluated during dynamic conditions
• This due to multiple compartment system when flow is zero at
airway opening, there may still be flow between compartments
(pendelluft)
• Result: dynamic mechanics become dependent on
respiratory frequency
• Typically, both compliance and resistance decrease as
frequency increases
Copyright © 2017 Elsevier Inc. All Rights Reserved. 33
Mechanics of Exhalation
• Airway size is determined by structural support and
transmural pressure
• Pressure difference between inside and outside airway wall
• Support comes from cartilage and traction from
surrounding tissues
• Small airways lack cartilage, thus they are more subject to
collapse
Copyright © 2017 Elsevier Inc. All Rights Reserved. 34
Mechanics of Exhalation
• During quiet breathing, Ptm is negative, maintaining
airway’s patency
• Equal pressure point (EPP): pressure inside airway =
pressure outside, downstream airway compression
occurs
• May result in airway collapse
• Dynamic compression of the airways (narrowing of the
airways owing to an increase in surrounding pressures)
• Responsible for the characteristic flow patterns observed in
forced expiratory tests of pulmonary function
Copyright © 2017 Elsevier Inc. All Rights Reserved. 35
Mechanics of Exhalation (Cont.)
Copyright © 2017 Elsevier Inc. All Rights Reserved. 36
Work of Breathing (WOB)
• Respiratory muscles perform work
• Resting inhalation requires work
• Resting exhalation is passive
• Forced exhalation requires work
• Pulmonary disease can dramatically increase WOB
• Restrictive disease work is greater due to elastic tissue recoil
• Obstructive disease work is greater due to increased
resistance
Copyright © 2017 Elsevier Inc. All Rights Reserved. 37
Work of Breathing (WOB)
• Mechanical
• Work done on an object is result of force (F) exerted
on object and distance (x) it is moved
• W = force  distance
• Work muscles do to inflate pulmonary system is
defined as transpulmonary pressure (PTP )
• Work done by a ventilator to inflate respiratory system
is defined as transrespiratory system pressure (PTR)
• Pressure-volume curve is used for setting optimal
PEEP
Copyright © 2017 Elsevier Inc. All Rights Reserved. 38
Pathology’s Affect on WOB
A: Normal
B: Restrictive disease: slope of the volume-pressure
curve is less, showing increased elastic work
C: Obstructive disease: Frictional resistance
increases dramatically, noted as bulging inspired
and expired curves 39
Pathology’s Affect on WOB
Copyright © 2017 Elsevier Inc. All Rights Reserved. 40
Metabolic Impact of
Increased WOB
• Respiratory muscles consume O2 to perform work
• O2 cost of breathing (OCB) is indirect measurement of
WOB
• Normal OCB <5% of oxygen consumption
• In disease, OCB may increase dramatically and may > 30%
• Limits exercise tolerance
• Impacts ability to wean from mechanical ventilation
• In shock, intubation and mechanical ventilation may be
indicated to decrease excess oxygen consumption of
respiratory muscles
• Preserves oxygen delivery for vital organs
Copyright © 2017 Elsevier Inc. All Rights Reserved. 41
Distribution of Ventilation
• In healthy lungs, neither ventilation (V) or perfusion (Q)
are distributed evenly
• Result: uneven ventilation to perfusion ratio
• V/Q ratio of 0.8
• In upright lung, ventilation and perfusion (V/Q) are
matched best at bases (dependent area)
• Apical alveoli are larger but harder to ventilate compared to
those at bases
• Gravity pulls more blood to bases
• In local disease, place good lung down for better V/Q
matching
Copyright © 2017 Elsevier Inc. All Rights Reserved. 42
Regional Factors Affecting
Distribution of Ventilation
• Regional factors interact with gravity:
• Thoracic expansion
• Shape of lungs and muscle action causes greater
expansion at bases, so more gas flow
• Transpulmonary pressure gradients: Directly related
to Ppl, closest alveoli most affected
• Apical Ppl −10 cm H2O, while at bases –2.5
• Alveoli at apices have larger resting volume than at
bases
Copyright © 2017 Elsevier Inc. All Rights Reserved. 43
Local Factors Affecting
Distribution of Ventilation
• CL and Raw influence local distribution of ventilation
• Time constants: time required for local alveolar filling
and emptying
• Time constant (units of time) = R  C
• Time constant (TC) always equals time necessary for lungs
to fill or empty by 63%
• For each time constant , inspiratory or expiratory, lung
volume changes by 63%
• After 2 time constants, lung volume has changed 86%
• In ventilator pressure control modes, inspiratory time must
be set to at least 3 time constants long to deliver 95% of
volume
• For any mode, expiratory time must be set to at least 3 time
constants for lungs to passively empty by 95%
Copyright © 2017 Elsevier Inc. All Rights Reserved. 44
Factors Affecting
Distribution of Ventilation
• Lung unit has long time constant (TC) if CL and Raw is high
• Lung unit has short time TC if CL and Raw is low
• Effects of unequal lung TCs are different for different ventilator
modes
• e.g., Volume Control (VC) with constant inspiratory flow, compared to
Pressure Control (PC) with constant inspiratory pressure
• Units with equal R and C: both VC and PC result in equal
distribution of volume
• Units with different TCs but equal Rs: VC gives more uniform
volumetric expansion and perhaps lower risk of volutrauma than
PC
• Units with different TCs but equal Cs: PC gives more uniform
volumetric expansion and perhaps lower risk of volutrauma than
PC
Copyright © 2017 Elsevier Inc. All Rights Reserved. 45
Factors Affecting Distribution of
Ventilation
Copyright © 2017 Elsevier Inc. All Rights Reserved. 46
Factors Affecting Distribution of
Ventilation
Copyright © 2017 Elsevier Inc. All Rights Reserved. 47
Efficiency of Ventilation
• Efficiency
• Lungs should have low OCB and produce little CO2
• Healthy lungs waste some gas due to:
• Anatomic dead space
• Gas left in conducting airways after inspiration
• Alveolar dead space
• Alveoli that are ventilated but have no perfusion
VE = VA –VD or VT = VA –VD
Copyright © 2017 Elsevier Inc. All Rights Reserved. 48
Efficiency of Ventilation
• Physiologic dead space = sum of anatomic and
alveolar dead space
• The larger the dead space, the less efficient the tidal
volume will be in eliminating CO2
Copyright © 2017 Elsevier Inc. All Rights Reserved. 49
Minute and Alveolar Ventilation
• Ventilation = expressed in liters per minute of
fresh gas entering the lungs
• Total volume moved in and out per minute =
Minute ventilation (VE)
• Normal VE = 5-10 L/min
• VE = fB  VT
• 6 L/min = 12 breaths/min  0.5 L (500 mL)
• VE driven by CO2 production (metabolic rate) and subject size
Copyright © 2017 Elsevier Inc. All Rights Reserved. 50
Minute and Alveolar Ventilation
• Alveolar Ventilation: amount of fresh gas
reaching alveoli per minute
• Determined by VT, dead space, and fB (RR)
VA = (VT – VD)  fB
• VA is always less than VE due to dead space
Copyright © 2017 Elsevier Inc. All Rights Reserved. 51
Dead Space Ventilation
• Physiologic dead space (VDphs) = anatomic
(VDanat) + alveolar dead space (VDalv)
• VDanat: volume in conducting airways
• 1 mL/lb of IBW (2.2 mL/kg)
• Does not participate in gas exchange because it is
rebreathed
• Recent research shows poor agreement
between individual patient’s estimated VD and
actual measured
Copyright © 2017 Elsevier Inc. All Rights Reserved. 52
Dead Space Ventilation
• VD/VT can be more accurately estimated for
mechanically ventilated adult patients using
more data available at bedside
• Using measured end tidal CO2
Copyright © 2017 Elsevier Inc. All Rights Reserved. 53
Dead Space Ventilation
• Alveolar dead space (VDalv): Volume of gas
ventilating unperfused alveoli
• Alveoli receive gas, but no perfusion or:
• have ventilation exceeding perfusion (high V/Q
ratios)
• excessive ventilation, more than necessary to
arterialize alveolar blood is wasted ventilation
Copyright © 2017 Elsevier Inc. All Rights Reserved. 54
Dead Space Ventilation
• Usually related to defects in pulmonary circulation
• e.g., pulmonary embolism
• Blocks portion of pulmonary circulation
• Apical alveoli have minimal or no perfusion in
normal upright subject at rest, contributing to dead
space
Copyright © 2017 Elsevier Inc. All Rights Reserved. 55
Dead Space Ventilation
Copyright © 2017 Elsevier Inc. All Rights Reserved. 56
Bohr Equation: VD/VT Ratio
• Sum of anatomic and alveolar dead space
= physiologic dead space (Vdphys )
• Measuring (Vdphys ):
• More accurately assesses alveolar ventilation
• Preferred clinical measure of ventilation
efficiency
• VDphys is expressed as ratio (VD/VT)
Copyright © 2017 Elsevier Inc. All Rights Reserved. 57
Bohr Equation: VD/VT Ratio
• Measured clinically using modified Bohr equation
• Provides an index of wasted ventilation
• If no dead space existed, then PaCO2 would equal
PeCO2
• Due to anatomic and alveolar dead space, PeCO2 is always
less than PaCO2
Copyright © 2017 Elsevier Inc. All Rights Reserved. 58
VD/VT
=
(PaCO2 – PeCO2)
Pa2
Bohr Equation: VD/VT Ratio
• Normal VD/VT ratio is 30% (range of 0.2-0.4)
• VD/VT increases with disease
• Tough to wean from mechanical ventilation if >0.6
• High FB and low VT result in high proportion of
wasted ventilation per minute (low VA)
• Most efficient breathing pattern is slow and deep
• Effective compensation for increase requires
increased VT , not increased FB
Copyright © 2017 Elsevier Inc. All Rights Reserved. 59
Effectiveness of Ventilation
• Ventilation is effective when CO2 is removed to
maintain normal pH
• Resting CO2 production (VCO2) = 200 mL/min
• CO2 level determined by VA and VCO2
Copyright © 2017 Elsevier Inc. All Rights Reserved. 60
.
PCO2 =
VCO2
VA

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Egan's chpt. 11 ventilation1 pp

  • 2. Learning Objectives • Describe the physiologic functions provided by ventilation. • Describe the pressure gradients responsible for gas flow, diffusion, and lung inflation. • Identify the forces that oppose gas movement into and out of the lungs. • Describe how surface tension contributes to lung recoil. Copyright © 2017 Elsevier Inc. All Rights Reserved. 2
  • 3. Learning Objectives • Describe how lung, chest wall, and total compliance are related. • State the factors that affect resistance to breathing. • Describe how various lung diseases affect the work of breathing. • State why ventilation is not evenly distributed throughout the lung. Copyright © 2017 Elsevier Inc. All Rights Reserved. 3
  • 4. Learning Objectives • Describe how the time constants affect alveolar filling and emptying. • Identify the factors that affect alveolar ventilation. • State how to calculate alveolar ventilation, dead space, and the VD/VT ratio. Copyright © 2017 Elsevier Inc. All Rights Reserved. 4
  • 5. Introduction to Ventilation • Ventilation is the process of moving gas (usually air) in and out of the lungs • Ventilation is to be distinguished from respiration, which refers to the physiologic processes of oxygen use at the cellular level • In health: Ventilation is regulated to meet the body’s needs under a wide range of conditions • In disease: This process can be markedly disrupted and often result in inadequate ventilation and /or increased work of breathing Copyright © 2017 Elsevier Inc. All Rights Reserved. 5
  • 6. Mechanics of Ventilation • Cycles of ventilation: inspiration and expiration • Tidal volume (VT): volume of gas moving in and out of the respiratory tract during inspiration or expiration • The Vt refreshes the gas present in the lung, removing CO2, and supplying O2 TO MEET METABOLIC NEEDS Copyright © 2017 Elsevier Inc. All Rights Reserved. 6
  • 7. Pressure Differences During Breathing • Gases move due to pressure gradients • Produced by thoracic expansion/contraction • Do to elastic properties of airways, alveoli, and chest wall • Transrespiratory pressure (PTR) • Everything that exists between pressure measured at airway opening (PAO) and pressure measured at body surface (PBS) • PTR = PAO – PBS • Equation follows direction of flow • PAO is higher than PBS • Components of transrespiratory pressure include: • Airway, lungs, and chest wall • This gradient causes gas flow in and out of lungs Copyright © 2017 Elsevier Inc. All Rights Reserved. 7
  • 8. Pressure Differences During Breathing Copyright © 2017 Elsevier Inc. All Rights Reserved. 8
  • 9. Pressure Differences During Breathing • Transairway pressure (PTAW) • PTAW = PAO– PA • Whatever exists between pressure measured at airway opening and pressure measured in alveoli of lungs • Transalveolar pressure (PTA) • PTA = PA– Ppl • Whatever exists between pressure measured in model alveolus and pressure measured in pleural space (Ppl). • Trans-chestwall pressure (PTCW) • Chest wall exists between pressure measured in pleural space and pressure on body surface • PTCW = Ppl – PBS Copyright © 2017 Elsevier Inc. All Rights Reserved. 9
  • 10. Pressure Differences During Breathing • Transpulmonary pressure difference (PTP) • Pulmonary system (airways and alveolar region), defined: • PTP = PAO – Ppl • Pressures must be measured to derive mechanical properties of pulmonary system • Under either static or dynamic (breathing) conditions • Note, some confusion arises from: • PTA = PAO – Ppl but only under static conditions • Considered a special case of PTP = PAO – Ppl • Static conditions can be imposed during mechanical ventilation • Through use of inspiratory hold maneuver Copyright © 2017 Elsevier Inc. All Rights Reserved. 10
  • 11. Pressure Differences During Breathing • Transthoracic pressure difference (PTT) • PTT = PA – PBS • Causes gas to flow into and out of alveoli during breathing • Beginning of inspiration in spontaneous breathing subject, PA is subatmospheric compared to PAO • Causes air to flow into alveoli • Beginning of exhalation is opposite • PA is higher than PAO • Causing air to flow out of the airway Copyright © 2017 Elsevier Inc. All Rights Reserved. 11
  • 12. Pressure Differences During Breathing • At end of resting exhalation, Ppl, is normally 5 cm H2O; PA = zero, there is no gas flow • PTP is also approximately 5 cm H2O in resting state • This positive end expiratory PTP maintains lung at its resting volume (i.e., functional residual capacity, FRC) Copyright © 2017 Elsevier Inc. All Rights Reserved. 12
  • 13. Pressure Differences During Breathing • Inspiration begins • When muscular effort expands the thorax • Thoracic expansion causes a decrease in Ppl • Causes positive change on expiratory PTP and PTA, which induces flow into lungs • Inspiratory flow is proportional to (+) change in transairway pressure difference • The higher the change in PTA, the higher the flow • Ppl continues to decrease until the end of inspiration Copyright © 2017 Elsevier Inc. All Rights Reserved. 13
  • 14. Pressure Differences During Breathing • Beginning of expiration • Thoracic recoil causes Ppl to start to rise • Thus, transpulmonary pressure difference starts to decrease • PTP is decreasing; opposite of inspiration • So flow is in opposite (negative) direction • Driving force for expiratory flow is energy stored in combined elastances of lungs and chest wall • Pleural pressures: always negative (subatmospheric) during normal inspiration and exhalation • During forced inspiration (big downward movement of diaphragm), pleural pressure can drop up to –50 cm H2O Copyright © 2017 Elsevier Inc. All Rights Reserved. 14
  • 15. Pressure Differences During Breathing Pmus = 0 = (Elastance × Volume) + (Resistance × Flow) • Rearranging the formula, we get: (Elastance  Volume) = − (Resistance  Flow) = Resistance  (− Flow) • Flow is negative (indicating expiration) • The driving force for expiratory flow is the energy stored in the combined elastances of lungs and chest wall Copyright © 2017 Elsevier Inc. All Rights Reserved. 15
  • 16. Pressure Differences During Breathing Copyright © 2017 Elsevier Inc. All Rights Reserved. 16
  • 17. Forces Opposing Lung Inflation • Lungs have tendency to recoil inward, while chest wall has tendency to move outwards • Those opposing forces keep lung at its resting volumes (FRC) Copyright © 2017 Elsevier Inc. All Rights Reserved. 17
  • 18. Forces Opposing Lung Inflation • Elastic opposition to ventilation • Elastic and collagen fibers provide resistance to lung stretch • Application of pressure causes stretch • Greater pressure causes greater stretch until maximum inflation is reached • Deflation is passive recoil; less force is required to maintain same volume • During deflation, lung volume at any given pressure is slightly greater than during inflation. • Difference between inflation and deflation curves is hysteresis Copyright © 2017 Elsevier Inc. All Rights Reserved. 18
  • 19. Forces Opposing Lung Inflation • Hysteresis indicates factors other than simple elastic tissue forces are present • Major factor, especially in sick lungs: opening of collapsed alveoli during inspiration that tend to stay open during expiration until very low lung volumes are reached Copyright © 2017 Elsevier Inc. All Rights Reserved. 19
  • 20. Forces Opposing Lung Inflation • Chest wall elastance and lung elastance are connected in a series: • Have same flow and change in volume but do not have same pressure differences • Elastance of respiratory system (ERS) = sum of lung (pulmonary) elastance (EL) and chest wall elastance (ECW) • Applies to both natural and artificial airways (ETT) Copyright © 2017 Elsevier Inc. All Rights Reserved. 20
  • 21. Copyright © 2017 Elsevier Inc. All Rights Reserved. 21
  • 22. Forces Opposing Lung Inflation Copyright © 2017 Elsevier Inc. All Rights Reserved. 22
  • 23. Surface Tension Forces • Hysteresis partly caused by surface tension • Surface tension opposes lung inflation • If surface tension is removed, hysteresis becomes very small • Lung recoil occurs due to tissue elasticity and surface tension • Pulmonary surfactant reduces lung surface tension • Produced in alveolar type II pneumocytes • Surfactant stabilizes alveoli by preventing collapse • When surface area decreases, ability of pulmonary surfactant to lower surface tension increases Copyright © 2017 Elsevier Inc. All Rights Reserved. 23
  • 24. Surface Tension Forces (Cont.) Copyright © 2017 Elsevier Inc. All Rights Reserved. 24
  • 25. Lung Compliance • CL defined as change in volume (ΔV) per unit of change in pressure (ΔP) difference across structure or CL = ΔV L (normal 0.2 L/cm H2O) ΔP cm H2O • Pulmonary pathology alters CL • Emphysema , obstructive lung disease, increases CL (loss elastic tissue, lungs more distensible) • Large changes in volume for small pressure changes • Fibrosis, restrictive lung disease, decreases CL (↑ elastic tissue) • Smaller volume change for any change in pressure • Stiffer lungs, usually with reduced volume Copyright © 2017 Elsevier Inc. All Rights Reserved. 25
  • 26. Lung Compliance Copyright © 2017 Elsevier Inc. All Rights Reserved. 26
  • 27. Relationship Between Chest Wall and Lung • Lungs and chest wall recoil in opposite directions • Compliance in both is ~0.2 L/cm H2O • Each oppose other, resulting in system compliance of ~0.1 L/cm H2O • FRC established at resting lung level where tendency of chest wall to expand equals that of lungs to collapse • Occurs at ~40% TLC Copyright © 2017 Elsevier Inc. All Rights Reserved. 27
  • 28. Relationship Between Chest Wall and Lung (Cont.) Copyright © 2017 Elsevier Inc. All Rights Reserved. 28
  • 29. Frictional Resistance to Ventilation • Tissue viscous resistance (~20% of the total resistance to lung inflation ) • Frictional forces during displacement of lungs, ribs, diaphragm, and abdominal organs • Airway resistance (~80% of of the frictional resistance to ventilation) • Gas flow causes frictional resistance Airway radius exponential effect (r4) on resistance • Artificial airway size or bronchospasm • Resistance is highest at nose (50% of total resistance) falls to ~20% of total resistance at small airways • Resistance in nonventilated patients is measured in pulmonary function laboratory Copyright © 2017 Elsevier Inc. All Rights Reserved. 29
  • 30. Frictional Resistance to Ventilation (Cont.) Copyright © 2017 Elsevier Inc. All Rights Reserved. 30
  • 31. Frictional Resistance to Ventilation (Cont.) Copyright © 2017 Elsevier Inc. All Rights Reserved. 31
  • 32. Static Versus Dynamic Mechanics • Resistance and compliance can be evaluated under static or dynamic conditions • Static implies flow throughout respiratory system has ceased and all ventilatory muscle activity is absent • Static conditions can be imposed with an inspiratory pause when patient is sedated and being mechanically ventilated • Dynamic is when flow of airway opening = 0 • Useful for lung protective ventilation strategies in patients w/ acute lung injury and acute respiratory distress syndrome Copyright © 2017 Elsevier Inc. All Rights Reserved. 32
  • 33. Static Versus Dynamic Mechanics • Due to different time constants, mechanics estimated during static conditions will yield different values than when evaluated during dynamic conditions • This due to multiple compartment system when flow is zero at airway opening, there may still be flow between compartments (pendelluft) • Result: dynamic mechanics become dependent on respiratory frequency • Typically, both compliance and resistance decrease as frequency increases Copyright © 2017 Elsevier Inc. All Rights Reserved. 33
  • 34. Mechanics of Exhalation • Airway size is determined by structural support and transmural pressure • Pressure difference between inside and outside airway wall • Support comes from cartilage and traction from surrounding tissues • Small airways lack cartilage, thus they are more subject to collapse Copyright © 2017 Elsevier Inc. All Rights Reserved. 34
  • 35. Mechanics of Exhalation • During quiet breathing, Ptm is negative, maintaining airway’s patency • Equal pressure point (EPP): pressure inside airway = pressure outside, downstream airway compression occurs • May result in airway collapse • Dynamic compression of the airways (narrowing of the airways owing to an increase in surrounding pressures) • Responsible for the characteristic flow patterns observed in forced expiratory tests of pulmonary function Copyright © 2017 Elsevier Inc. All Rights Reserved. 35
  • 36. Mechanics of Exhalation (Cont.) Copyright © 2017 Elsevier Inc. All Rights Reserved. 36
  • 37. Work of Breathing (WOB) • Respiratory muscles perform work • Resting inhalation requires work • Resting exhalation is passive • Forced exhalation requires work • Pulmonary disease can dramatically increase WOB • Restrictive disease work is greater due to elastic tissue recoil • Obstructive disease work is greater due to increased resistance Copyright © 2017 Elsevier Inc. All Rights Reserved. 37
  • 38. Work of Breathing (WOB) • Mechanical • Work done on an object is result of force (F) exerted on object and distance (x) it is moved • W = force  distance • Work muscles do to inflate pulmonary system is defined as transpulmonary pressure (PTP ) • Work done by a ventilator to inflate respiratory system is defined as transrespiratory system pressure (PTR) • Pressure-volume curve is used for setting optimal PEEP Copyright © 2017 Elsevier Inc. All Rights Reserved. 38
  • 39. Pathology’s Affect on WOB A: Normal B: Restrictive disease: slope of the volume-pressure curve is less, showing increased elastic work C: Obstructive disease: Frictional resistance increases dramatically, noted as bulging inspired and expired curves 39
  • 40. Pathology’s Affect on WOB Copyright © 2017 Elsevier Inc. All Rights Reserved. 40
  • 41. Metabolic Impact of Increased WOB • Respiratory muscles consume O2 to perform work • O2 cost of breathing (OCB) is indirect measurement of WOB • Normal OCB <5% of oxygen consumption • In disease, OCB may increase dramatically and may > 30% • Limits exercise tolerance • Impacts ability to wean from mechanical ventilation • In shock, intubation and mechanical ventilation may be indicated to decrease excess oxygen consumption of respiratory muscles • Preserves oxygen delivery for vital organs Copyright © 2017 Elsevier Inc. All Rights Reserved. 41
  • 42. Distribution of Ventilation • In healthy lungs, neither ventilation (V) or perfusion (Q) are distributed evenly • Result: uneven ventilation to perfusion ratio • V/Q ratio of 0.8 • In upright lung, ventilation and perfusion (V/Q) are matched best at bases (dependent area) • Apical alveoli are larger but harder to ventilate compared to those at bases • Gravity pulls more blood to bases • In local disease, place good lung down for better V/Q matching Copyright © 2017 Elsevier Inc. All Rights Reserved. 42
  • 43. Regional Factors Affecting Distribution of Ventilation • Regional factors interact with gravity: • Thoracic expansion • Shape of lungs and muscle action causes greater expansion at bases, so more gas flow • Transpulmonary pressure gradients: Directly related to Ppl, closest alveoli most affected • Apical Ppl −10 cm H2O, while at bases –2.5 • Alveoli at apices have larger resting volume than at bases Copyright © 2017 Elsevier Inc. All Rights Reserved. 43
  • 44. Local Factors Affecting Distribution of Ventilation • CL and Raw influence local distribution of ventilation • Time constants: time required for local alveolar filling and emptying • Time constant (units of time) = R  C • Time constant (TC) always equals time necessary for lungs to fill or empty by 63% • For each time constant , inspiratory or expiratory, lung volume changes by 63% • After 2 time constants, lung volume has changed 86% • In ventilator pressure control modes, inspiratory time must be set to at least 3 time constants long to deliver 95% of volume • For any mode, expiratory time must be set to at least 3 time constants for lungs to passively empty by 95% Copyright © 2017 Elsevier Inc. All Rights Reserved. 44
  • 45. Factors Affecting Distribution of Ventilation • Lung unit has long time constant (TC) if CL and Raw is high • Lung unit has short time TC if CL and Raw is low • Effects of unequal lung TCs are different for different ventilator modes • e.g., Volume Control (VC) with constant inspiratory flow, compared to Pressure Control (PC) with constant inspiratory pressure • Units with equal R and C: both VC and PC result in equal distribution of volume • Units with different TCs but equal Rs: VC gives more uniform volumetric expansion and perhaps lower risk of volutrauma than PC • Units with different TCs but equal Cs: PC gives more uniform volumetric expansion and perhaps lower risk of volutrauma than PC Copyright © 2017 Elsevier Inc. All Rights Reserved. 45
  • 46. Factors Affecting Distribution of Ventilation Copyright © 2017 Elsevier Inc. All Rights Reserved. 46
  • 47. Factors Affecting Distribution of Ventilation Copyright © 2017 Elsevier Inc. All Rights Reserved. 47
  • 48. Efficiency of Ventilation • Efficiency • Lungs should have low OCB and produce little CO2 • Healthy lungs waste some gas due to: • Anatomic dead space • Gas left in conducting airways after inspiration • Alveolar dead space • Alveoli that are ventilated but have no perfusion VE = VA –VD or VT = VA –VD Copyright © 2017 Elsevier Inc. All Rights Reserved. 48
  • 49. Efficiency of Ventilation • Physiologic dead space = sum of anatomic and alveolar dead space • The larger the dead space, the less efficient the tidal volume will be in eliminating CO2 Copyright © 2017 Elsevier Inc. All Rights Reserved. 49
  • 50. Minute and Alveolar Ventilation • Ventilation = expressed in liters per minute of fresh gas entering the lungs • Total volume moved in and out per minute = Minute ventilation (VE) • Normal VE = 5-10 L/min • VE = fB  VT • 6 L/min = 12 breaths/min  0.5 L (500 mL) • VE driven by CO2 production (metabolic rate) and subject size Copyright © 2017 Elsevier Inc. All Rights Reserved. 50
  • 51. Minute and Alveolar Ventilation • Alveolar Ventilation: amount of fresh gas reaching alveoli per minute • Determined by VT, dead space, and fB (RR) VA = (VT – VD)  fB • VA is always less than VE due to dead space Copyright © 2017 Elsevier Inc. All Rights Reserved. 51
  • 52. Dead Space Ventilation • Physiologic dead space (VDphs) = anatomic (VDanat) + alveolar dead space (VDalv) • VDanat: volume in conducting airways • 1 mL/lb of IBW (2.2 mL/kg) • Does not participate in gas exchange because it is rebreathed • Recent research shows poor agreement between individual patient’s estimated VD and actual measured Copyright © 2017 Elsevier Inc. All Rights Reserved. 52
  • 53. Dead Space Ventilation • VD/VT can be more accurately estimated for mechanically ventilated adult patients using more data available at bedside • Using measured end tidal CO2 Copyright © 2017 Elsevier Inc. All Rights Reserved. 53
  • 54. Dead Space Ventilation • Alveolar dead space (VDalv): Volume of gas ventilating unperfused alveoli • Alveoli receive gas, but no perfusion or: • have ventilation exceeding perfusion (high V/Q ratios) • excessive ventilation, more than necessary to arterialize alveolar blood is wasted ventilation Copyright © 2017 Elsevier Inc. All Rights Reserved. 54
  • 55. Dead Space Ventilation • Usually related to defects in pulmonary circulation • e.g., pulmonary embolism • Blocks portion of pulmonary circulation • Apical alveoli have minimal or no perfusion in normal upright subject at rest, contributing to dead space Copyright © 2017 Elsevier Inc. All Rights Reserved. 55
  • 56. Dead Space Ventilation Copyright © 2017 Elsevier Inc. All Rights Reserved. 56
  • 57. Bohr Equation: VD/VT Ratio • Sum of anatomic and alveolar dead space = physiologic dead space (Vdphys ) • Measuring (Vdphys ): • More accurately assesses alveolar ventilation • Preferred clinical measure of ventilation efficiency • VDphys is expressed as ratio (VD/VT) Copyright © 2017 Elsevier Inc. All Rights Reserved. 57
  • 58. Bohr Equation: VD/VT Ratio • Measured clinically using modified Bohr equation • Provides an index of wasted ventilation • If no dead space existed, then PaCO2 would equal PeCO2 • Due to anatomic and alveolar dead space, PeCO2 is always less than PaCO2 Copyright © 2017 Elsevier Inc. All Rights Reserved. 58 VD/VT = (PaCO2 – PeCO2) Pa2
  • 59. Bohr Equation: VD/VT Ratio • Normal VD/VT ratio is 30% (range of 0.2-0.4) • VD/VT increases with disease • Tough to wean from mechanical ventilation if >0.6 • High FB and low VT result in high proportion of wasted ventilation per minute (low VA) • Most efficient breathing pattern is slow and deep • Effective compensation for increase requires increased VT , not increased FB Copyright © 2017 Elsevier Inc. All Rights Reserved. 59
  • 60. Effectiveness of Ventilation • Ventilation is effective when CO2 is removed to maintain normal pH • Resting CO2 production (VCO2) = 200 mL/min • CO2 level determined by VA and VCO2 Copyright © 2017 Elsevier Inc. All Rights Reserved. 60 . PCO2 = VCO2 VA