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Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital of Geneva Geneva, Switzerland

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Page 1: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Basic respiratory mechanicsrelevant for mechanical vnetilation

Peter C. RimensbergerPediatric and Neonatal ICUDepartment of Pediatrics

University Hospital of GenevaGeneva, Switzerland

Page 2: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Volume ChangeVolume ChangeVolume ChangeVolume Change

TimeTimeTimeTime

Gas FlowGas FlowGas FlowGas Flow

Pressure DifferencePressure DifferencePressure DifferencePressure Difference

Basics of respiratory mechanics important to mechanical ventilation

Page 3: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Volume

Pressure

V

P

C = V P

Compliance

Page 4: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

“The Feature of the Tube”

Airway Resistance

Pressure Difference = Flow Rate x Resistance of the Tube

Resistance is the amount of pressure required to deliver a given flow of gas and is expressed in terms of a change in pressure divided by flow.

R = P

Flow

P1 P2

Page 5: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Mechanical response to positive pressure application

Active inspiration

Passive exhalation

Page 6: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

R = ∆P / V (cmH2O/L/s)

Equation of motion: P = ( 1 / Crs ) V + Rrs V.

.

Mechanical response to positive pressure application

Compliance: pressure - volume

Resistance: pressure - flow

C = V / P (L/cmH2O)

Page 7: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Pressure – Flow – Time - Volume

Time constant: T = Crs x Rrs

Volume change requires time to take place.

When a step change in pressure is applied, the instantaneous change in volume follows an exponential curve, which means that, formerly faster, it slows down progressively while it approaches the new equilibrium.

P = ( 1 / Crs ) x V + Rrs x V.

Page 8: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Time constant: T = Crs x Rrs

Pressure – Flow – Time - Volume

Will pressure equilibrium

be reached in the lungs?

Page 9: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

A: Crs = 1, R = 1B: Crs = 2

(T = R x 2C)

C: Crs = 0.5 (T = R x 1/2C)(reduced inspiratory

capacity to 0.5)

D: R = 0.5(T = 1/2R x C)

E: R = 2(T = 2R x C)

Effect of varying time constants on the change in lung volume over time(with constant inflating pressure at the airway opening)

A: Crs = 1, R = 1

C: Crs = 0.5(T = R x 1/2C) (reduced inspiratory capacity to 0.5)

E: R = 2 (T = 2R x C)

Page 10: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Ventilators deliver gas to the lungs using positive pressure at a certain rate.

The amount of gas delivered can be limited by time, pressure or volume.

The duration can be cycled by time, pressure or flow.

Volume ChangeVolume ChangeVolume ChangeVolume Change

TimeTimeTimeTime

Gas FlowGas FlowGas FlowGas Flow

Pressure DifferencePressure DifferencePressure DifferencePressure Difference

Page 11: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Nunn JF Applied respiratory physiology 1987:397

Page 12: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

time

flo

winsuflation

exhalation

0

auto-PEEP

Premature flow termination during expiration = “gas trapping” = deadspace (Vd/Vt) will increase

Expiratory flow waveform: normal vs pathologic

Page 13: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Flow termination and auto-PEEP detection

PEEPi

Trapped volume

Page 14: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Dhand, Respir Care 2005; 50:246

Correction for Auto-PEEP- Bronchodilator

Page 15: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Analysing time settings of the respiratory cycle

1) Too short Te intrinsic PEEP 1) Correct Te

2) Unnecessary long Ti 2) Too short Ti

Page 16: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Appropriate inspiratory time

Page 17: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Optimizing tidal volume delivery at set pressure

Lucangelo U, Bernabe F, and Blanch L Respir Care 2005;50(1):55– 65

Page 18: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Vt 120 ml

Page 19: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Vt 160 ml

Page 20: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Vt 137 ml

Page 21: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital
Page 22: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital
Page 23: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Progressive increase in inspiratory time

Lucangelo U, Bernabe F, and Blanch L Respir Care 2005;50(1):55– 65

CAVE: you have to set Frequency and Ti (Control) or Ti and Te (TCPL)

Page 24: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Too short Te will not allow to deliver max. possible Vt at given P

will induce PEEPi increases the risk for

hemodynamic instability

Too short Ti will reduce delivered Vt

unneccessary high PIP will be applied unnecessary high intrathoracic pressures

The patient respiratory mechanics dictate the maximal respiratory frequency

Page 25: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Proximal Airway Pressure

Alveolar Pressure

Look at the flow – time curve !

P

V.

Page 26: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Cave! Ti settings in presence of an endotracheal tube leak

Flow

LeakTime

The only solution in presence of an important leak: Look how the thorax moves

Time

Volume

Leak Vex < Vinsp

Page 27: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Who’s Watching the Patient?

Pierson, IN: Tobin, Principles and Practice of Critical Care Monitoring

Page 28: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Vol

ume

PressurePressureV

olum

e

Pressure Ventilation Volume

VentilationDecreased Tidal Volume Increased Pressure

Compliance Compliance

Decreased PressureIncreased Tidal Volume

and do not forget, the time constant (T = Crs x Rrs) will change too!

Page 29: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Compliance decrease

Lucangelo U, Bernabe F, and Blanch L Respir Care 2005;50(1):55– 65

0.4 (s) 0.35 (s)0.65 (s) 0.5 (s)

52 cmH2O33 cmH2O

Page 30: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Change in compliance after surfactant = change in time constant after surfactant

PEEP PIP PEEP PIP

pre post

Vo

lum

e

Pressure

Kelly E Pediatr Pulmonol 1993;15:225-30

Page 31: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Volume Guarantee: New Approaches in Volume Controlled Ventilation for Neonates. Ahluwalia J, Morley C, Wahle G. Dräger Medizintechnik GmbH. ISBN 3-926762-42-X

Page 32: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Time constant: = Crs x Rrs

To measure compliance and resistance - is it in the clinical setting important ?

Use the flow curve for decision making about the settings for respiratory rate and duty cycle in the mechanical ventilator

The saying “we ventilate at 40/min” or “with a Ti of 0.3” is a testimony of no understanding !

Page 33: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Pressure Ventilation - Waveforms

Flow

Pressure

Tinsp.PIP

Peak Flow

25%

Pressure Control Pressure Support

Inspiratory time or cycle off criteria

Ti given by the cycle off criteria

Pressure Control versus Pressure Support

Ti set

Page 34: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

The non synchronized patient during Pressure-Support (inappropriate end-inspiratory flow termination criteria)

Nilsestuen J Respir Care 2005;50:202–232.

Pressure-Support and flow termination criteria

Page 35: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Pressure-Support and flow termination criteria

Increase in RR, reduction in VT, increase in WOB Nilsestuen J Respir Care 2005

Page 36: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Termination Sensitivity = Cycle-off Criteria

Flow

Peak Flow (100%)

TS 5%

Tinsp. (eff.)

Leak

Set (max) Tinsp.

Time

TS 30%

Page 37: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital
Page 38: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital
Page 39: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital
Page 40: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital
Page 41: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

What do airway pressures mean?

Palv = Ppl + Ptp

Where Ptp is transpulmonary pressure, Palv is alveolar pressure, and Ppl is pleural pressure

Ptp = Palv - Ppl

Page 42: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

PPl = Paw x [E CW / (E L + E cw)]

Ptp = Paw x [E L / (E L + E cw)]

when airway resistance is nil (static condition)

Palv = PPl + Ptp Etot = EL + Ecw

Pairways (cmH2O)

Ppleural (cmH2O)

Ptranspulmonary (cmH2O)

Page 43: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

PPl = Paw x [E CW / (E L + E cw)]

Ptp = Paw x [E L / (E L + E cw)]

when airway resistance is nil (static condition)

Paw = PPl + Ptp

Etot = EL + Ecw

Gattinoni L Critical Care 2004, 8:350-355

soft stiff

Page 44: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

In normal condition: EL = Ecw

Ecw/ Etot = 0.5 and EL/ Etot = 0.5

PTP ~ 50% of Paw applied

In primary ARDS: EL > Ecw (EL / Etot > 0.5)

Stiff lung, soft thorax PTP > 50 % of Paw applied

In secondary ARDS: EL < Ecw (EL / Etot < 0.5)

Soft lung, stiff thorax PTP < 50 % of Paw applied

In ARDS: PTP ~ 20 to 80% of Paw applied

Ptp = Paw x [E L / (E L + E cw)]

Page 45: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Grasso S Anesthesiology 2002; 96:795–802

22 ARDS-patients: Vt 6 ml/kg, PEEP and FiO2 to obtain SO2 90–95%

RM: CPAP to 40 cm H2O for 40 s

Respiratory mechanics influence the efficiency of RM

transpulmonary pressure

Page 46: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Elastic properties, compliance and FRC in neonates

Neonate chest wall compliance, CW = 3-6 x CL, lung compliance

tending to decrease FRC, functional residual capacity

By 9-12 months CW = CL

In infant RDS (HMD): EL >>> Ecw (EL / Etot >>> 0.5)

Stiff lung, very soft thorax PTP >>> 50 % of Paw applied

Page 47: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Elastic properties, compliance and FRC in neonates

Neonate chest wall compliance, CW = 3-6 x CL, lung compliance

tending to decrease FRC, functional residual capacity

By 9-12 months CW = CL

Dynamic FRC in awake, spontaneously ventilating infants is maintainednear values seen in older children and adults because of

1. continued diaphragmatic activity in early expiratory phase2. intrinsic PEEP (relative tachypnea with start of inspiration

before end of preceding expiration)3. sustained tonic activity of inspiratory muscles (incl. diaphragma)

(probably most important)

By 1 year of age, relaxed end-expiratory volume predominates

Page 48: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Pplat 30 cm H2O

transpulmonary pressure = 15 cm H2O

Pplat = Palv; Pplat = Transpulmonary Pressure ?

+15 cm H2O

Stiff chest wall

Page 49: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

PCV 20 cm H2O, PEEP 10 cm

H2O; Pplat 30 cm H2O

-15 cm H2Otranspulmonary pressure = 45 cm H2O

Active inspiratory effort

Pplat = Palv; Pplat = Transpulmonary Pressure ?

Page 50: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Pplat 30 cm H2O, PCV

Pplat 30 cm H2O,PCV (PSV)

Active inspiratory effort

Pplat 30 cm H2O,PCV

Pplat = Palv; Pplat = Transpulmonary Pressure?

Risk of VILI may be different with the same Pplat

Page 51: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Pressure – Flow – Time - Volume

. V or

V

P or V

Loops

V /

P /

V. t

Curves

but we still have to decide about respiratory rate, tidal volumes, pressure settings …

… that have to be adapted to the patients respiratory mechanics

The ventilator display can help us….

Page 52: Basic respiratory mechanics relevant for mechanical vnetilation Peter C. Rimensberger Pediatric and Neonatal ICU Department of Pediatrics University Hospital

Alveolar Pressure

Airway Pressure

Residual Flows

Avoid ventilation out of control !