RESPIRATORY SYSTEM

We will begin with

CHAPTER 17

&

Pages 43 through 53

In the CB

 

Respiratory Structures:

Be certain to view Figures 17.2, 3, & 4

Look at these!

 

LUNG STRUCTURES

RESPIRATORY STRUCTURES

ALVEOLI

 

To illustrate, try breathing through a garden hose

DEAD SPACE

You must subtract the volume of each breath that does not reach the alveoli to get the alveolar ventilation rate

TIDAL VOLUME vs. ALVEOLAR VENTILATION

IN EACH CASE TIDAL VOLUME = 6 L / min

SO, WHICH ONE IS BEST?

= 4200 ml / min

= 0 ml / min

5100 ml / min

 

LaPlace’s Law as applied to alveoli:

P = 2T / r

P = 2T/r

SURFACE TENSION:

Due to its polar nature, water molecules adhere together, giving rise to surface tension at air - water interfaces

 

Surface Tension

Wall tension of an Alveolus:

FROM INHALATION TO EXHALATION:

P = 2 X 50 dynes/cm P = 2 X 50 dynes/cm

0.05 cm 0.025 cm

P = 2000 dynes/cm2 P = 4000 dynes/cm2

 

Therefore, surface tension must decrease as alveolar radius decreases!

Thus, as alveolar radii decrease, the (2T / r) or alveolar wall tension gets larger than the pressure and alveoli would collapse.

How do alveoli adjust to prevent this?

 

TO DECREASE SURFACE TENSION, ADD DETERGENT! (also called SURFACE ACTIVE AGENT
or SURFACTANT)

 

Secreted by Alveolar

Type II Pneumocytes

THUS Surface Tension is proportional to 1/ [DPL] at the surface of the water layer in the alveoli and it changes as alveoli change radii during respiration

As alveolar r decreases during exhalation, LaPlace’s Law

P = 2T/r

is satisfied and the alveoli do not collapse.

Hyaline membrane disease:

An insufficiency of DPL secretion by a new born

Pulmonary Circulation (vs. Systemic)

 

Capillaries in the Lung:

Fluid Movement in Lungs

Venous Admixture