Chapter 7- Gas Diffusion
What is Diffusion
Net movement of molecule
- From high to low concentration
- Diffusion gradient
Continues until equilibrium
Diffusion across alveolar-capillary membrane and tissue
Disunion Gradients of Respiratory Gases
Inspired air contains about 21% O2 and essentially no CO2
PO2 in the conducting airway gas is lower than PO2 in the atmosphere
- Gas in the lung is 100% saturated with water vapor
- At body tempature, the partial pressure of water vapor in the lung (PH2O) is 47mmHg
- PO2 in conducting airways is about 150mmHg
PIO2= 760mmHg x 0.21= 158mmHg
PIO2 (humidified)= (760-47) x 0.21=149.73 149mmHg
Respiratory exchange ratio (R=0.8)
- R= VCO2/VO2
O2 consumption= 250mL/min
CO2 production= 200mL/min
Alveolar air equation
- PAO2= PIO2-PACO2[FIO2+(1-PIO2/R)]
PAO2= PIO2- (PaCO2)1.2
PAO2=PIO2-PaCO2(if FIO2>0.60)
Laws of Governing Diffusion
Fick’s Law
Vgas=[AxDx(P1-P2)]T
A=Surface Area
D=Diffusion coefficient (solubility)
(P1-P2)= diffusion gradient
T= membrane thickness
This means the greater the surface area, solubility coefficient and pressure gradient, the greater the diffusion rate; the greater the membrane thickness, the slower the diffusion rate
Physicalgas characteristics and diffusion
- Grams Law: Gas diffusion rate s inversely proportional to the square root of its gram molecular weight (or density); lighter gas=faster diffusion ratw
- Henry’s Law: Gas diffusion is directly proportional to he gas partial pressure (greater pressure, greater diffusion)
- CO2 diffuses 20 times faster than O2 across alveolar-capillary membrane because of its much greater solubility (it is actually a heavier molecule)
Limitations of Oxygen Diffusion
Effects of partial pressure gradient and capillary blood transit time
- Capilary transit time =0.75 seconds
- Alveolar- capillary equilibrium= within first 0.25 second
Perfusion and diffusion limitations to O2 transfer
- Increased blood flow
CO= diffusion limited
N2O= perfusion limited
Diffusion path length
- From alveolar gas to red blood cells
- Path distance <0.1 micrometers
Fibrotic thickening of alveolar and capillary walls
Interstitial edema fluid, separating alveolar can capillary membranes
Fluids in the alveoli
Interstitial fibrotic process that thicken the interstitial space
Dilated, engorged capillaries, which allow RBCs to flow side by side. Interstitial edema fluid
Diffusion surface area
- The total area of contact between ventilated alveoli and perfumed apilaries
- Decreased the diffusion surface area and the lungs diffusion
A decrease in the number of open, perfumed capillaries
The decrease in the number of open, ventilated alveoli
Measuring Difusión Capacity
General Principles
- Single-breath CO diffusion tests (DLCO)
-DLCO=Ml CO transferred to blood/min - mean PACO-mean PCCO
Normal Values
- 20 to 30mL/min/mmHg
- DLCO-DLCO x 1.23= about 32mL/min/mmHg
- Notice unit of diffusion is opposite of resistance: flow/pressure= coonductance
Factors Affecting Measured Carbon Monoxide Diffusion in the Lung
ody
Age
Lung Volume
Exercise
Body position
- DLCO 15% to 20% higher in supine
Alveolar PO2 and PCO2
Hemoglobin concentration
Pulmonary diseases
Conditions That Decrease Diffusion Capacity
Increased diffusion path distance
- Interstitial or alveolar edema
- Intestinal or alveolar fibrosis
- Dilated, engorged capillaries (CHF)
Decreased diffusion surface area
- Destrction of alveolar capillaries bed (emphysema)
- Reduced capillary blood flow
- Pulmonary embolus
- Low cardiac output (heart failure and blood loss)
- Tumors
Decreased uptake by red blood cells
- Anemia
- low pulmonary capillary blood volume
Ventiltion-perfusion mismatch
- Obstructive lung diseases (reduced regional ventilation)
- Atelectasis (small airway and alveolar collapse)
- Pneumonia (fluid-filled alveoli)
Clinical se of DLCO
Assessment of gas diffusion across alveolar-capillary membrane
More sensitive that PaO2 to detect O2 transfer problems
DLCO clarifies mechanisms of arterial hypoxemia
- If DLCO is normal, diffusion is not a contributing factor