Multiple inert gas elimination technique

Hypoxemia is generally attributed to one of four processes: hypoventilation, shunt (right to left), diffusion limitation, and ventilation/perfusion (V_A/Q) inequality.[1] Moreover, there are also "extrapulmonary" factors that can contribute to fluctuations in arterial PO₂.

There are several measures of hypoxemia that can be assessed, but there are various limitations associated with each. It was for this reason that the MIGET was developed, to overcome the shortcomings of previous methods.[2][3][4][5]

Steady-state gas exchange in the lungs obeys the principles of conservation of mass.[6] This leads to the ventilation/perfusion equation for oxygen:

${\displaystyle V_{A}/Q=8.63\times {\frac {C_{c'}{\ce {O2}}-C_{v}{\ce {O2}}}{P_{I}{\ce {O2}}-P_{A}{\ce {O2}}}}}$

and for carbon dioxide:

${\displaystyle V_{A}/Q=8.63\times {\frac {C_{v}{\ce {CO2}}-C_{c'}{\ce {CO2}}}{P_{A}{\ce {CO2}}}}}$

where:

• ${\displaystyle C_{c'}}$ denotes the end-capillary concentration of the gas (mL/dL),
• ${\displaystyle C_{v}}$ denotes the mixed venous concentration of the gas (mL/dL),
• ${\displaystyle P_{I}}$ denotes the inspired partial pressure of the gas (mmHg), and
• ${\displaystyle P_{A}}$ denotes the alveolar partial pressure of the gas (mmHg)
• ${\displaystyle V_{A}/Q}$ denotes the ratio of alveolar ventilation to cardiac output

For the purposes of utilizing the MIGET, the equations have been generalized for an inert gas (IG):

${\displaystyle V_{A}/Q=8.63\times {\ce {solubility}}\times {\frac {P_{V}{\ce {IG}}-P_{C'}{\ce {IG}}}{P_{A}{\ce {IG}}}}}$

where:

• solubility is the ratio of concentration to partial pressure expressed in mL of gas dissolved per dL of blood per mmHg of the gas in blood

Assuming diffusion equilibration is complete for the inert gas, dropping the subscript IG, and substituting the blood-gas partition coefficient (λ) renders:

${\displaystyle V_{A}/Q={\lambda }\times {\frac {P_{v}-P_{A}}{P_{A}}}}$

Rearranging:

${\displaystyle P_{A}/P_{v}={\frac {\lambda }{{\lambda }+V_{A}/Q}}=P_{c'}/P_{v}}$

where:

• ${\displaystyle P_{v}}$ denotes the mixed venous partial pressure of the gas (mmHg)
• ${\displaystyle P_{c'}}$ denotes the end-capillary partial pressure of the gas (mmHg)

This equation is the foundation for the MIGET, and it demonstrates that the fraction of inert gas not eliminated from the blood via the lung is a function of the partition coefficient and the V_A/Q ratio. This equation operates under the presumption that the lung is perfectly homogenous. In this model, retention (R) is measured from the ratio ${\displaystyle P_{A}/P_{v}}$. Stated mathematically:

${\displaystyle R={\frac {\lambda }{\lambda +V_{A}/Q}}}$

From this equation, we can measure the levels of each inert gas retained in the blood. The relationship between retention (R) and ${\displaystyle V_{A}/Q}$ can be summarized as follows: As ${\displaystyle V_{A}/Q}$ for a given λ increases, R decreases; however, this relationship between ${\displaystyle V_{A}/Q}$ and R is the most obvious at values of ${\displaystyle V_{A}/Q}$ between ten times higher and lower than a gas's λ. Beyond this, however, it is possible to measure the concentrations of the inert gases in the expired gas from the subject. The ratio of the mixed expired concentration to the mixed venous concentration has been termed excretion (E) and describes the ventilation to regions of varying ${\displaystyle V_{A}/Q}$. When taken together:

${\displaystyle V_{IG}=V_{E}\times E=\lambda \times Q_{T}\times [1-R]}$

where:

• V_IG denotes volume of an inert gas eliminated per minute (mL/min)
• ${\displaystyle V_{E}}$ denotes minute ventilation (mL/min)
• ${\displaystyle Q_{T}}$ denotes cardiac output (mL/min)

When observing a collection of alveoli in which PO₂ and PCO₂ are uniform, local alveolar ventilation and local blood flow define ${\displaystyle V_{A}/Q}$:

${\displaystyle V_{A}=Q\times V_{A}/Q}$

From these equations it can be deduced that to have knowledge of either retention or excretion implies knowledge of the other. Moreover, a similar understanding exists for the relationship between the distribution of blood flow and the distribution of ventilation.[6]

The data produced by the MIGET is an approximation of the distribution of ${\displaystyle V_{A}/Q}$ ratios across the entire lung. It has been estimated that nearly 100,000 gas exchange units exist in the human lung;[7] this could lead to a theoretical maximum of VA/Q compartments as high as 100,000, in that case.