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(Chest. 2000;118:468-472.)
© 2000 American College of Chest Physicians

Reduction in Tracheal Lumen Due to Endotracheal Intubation and Its Calculated Clinical Significance*

Kevin R. Bock, MD; Peter Silver, MD; Maya Rom and Mayer Sagy, MD, FCCP

* From the Division of Critical Care Medicine, Schneider Children’s Hospital, Hyde Park, NY.

Correspondence to: Kevin R. Bock, MD, Division of Critical Care Medicine, Schneider Children’s Hospital, Hyde Park, NY 11040; e-mail: krbcmgb{at}massmed.org


    Abstract
 TOP
 Abstract
 Introduction
 Materials and Methods
 Results
 Discussion
 References
 
Background: The flow in the human trachea is turbulent. Thus, the tracheal resistance (R) and the pressure gradient ({Delta}P) required to maintain a given flow across the trachea is inversely related to its radius raised to the fifth power. If the caliber reduction ratio (X) after endotracheal intubation is calculated as X = radius of the endotracheal tube (rETT)/radius of the trachea (rT), then {Delta}P and/or R will be increased by (1/X)5.

Study objectives: To measure the actual ratio between rETT and rT following endotracheal intubation of pediatric patients with respiratory failure and to calculate the resulting increase in the tracheal R and {Delta}P for a given inspiratory flow rate.

Design: Retrospective chart review.

Setting: Pediatric ICU in a tertiary-care teaching children’s medical center.

Patient enrollment: Twenty consecutive pediatric patients (mean [± SD] age, 6.4 ± 7.2 years) whose tracheas had been intubated for various causes of respiratory failure, and who had received a CT scan, were included in our study. All patients received an endotracheal tube the size of which was derived from the following formula: (age in years/4) + 4.

Measurements and main results: rT and rETT were measured from CT scan sections at and around the level of the thoracic inlet, and the average values were used to calculate X. These values ranged from 0.33 to 0.65 (mean, 0.55 ± 0.8). The factor (1/X)5 was calculated for each patient and then was multiplied by the known normal value for tracheal R for adolescents and adults (0.07 cm H2O/L/s) to obtain the value of R resulting from the artificial airway, (1/X)5 x 0.07. Our results showed that tracheal R increased due to caliber reduction of the trachea after endotracheal intubation by 33.9 ± 52.5-fold (range, 8.6- to 255.5-fold). In order to maintain an inspiratory flow of 1 L/s, the value of P for the intubated trachea would increase from 0.07 cm H2O to a mean of 2.4 ± 3.7 cm H2O (range, 0.6 to 18 cm H2O). In two of our patients, the rT/rETT ratios were < 0.5 (0.33 and 0.44, respectively); this translated into a more significant increase in the calculated {Delta}Ps, 18 and 4.2 cm H2O, respectively.

Conclusions: The common value of X due to endotracheal intubation is between 0.5 and 0.6, which in and of itself results in an increase in R across the intubated trachea up to 32-fold. The calculated increase in P as a result of this is between 2 and 3 cm H2O for adolescents or young adults. The addition of pressure support of at least 3 cm H2O during spontaneous ventilation via an endotracheal tube, which is common practice in pediatric critical care, should alleviate any respiratory distress emanating from the increased R. However, a value for X < 0.5, which was found in 10% of our patients (2 of 20 patients), results in a much higher calculated increase in the pressure gradient and, therefore, a higher level of pressure support is required to overcome this increase.

Key Words: airway resistance • endotracheal intubation • mechanical ventilator • trachea


    Introduction
 TOP
 Abstract
 Introduction
 Materials and Methods
 Results
 Discussion
 References
 
In order for gas to flow into the lungs, a pressure gradient ({Delta}P) must develop to overcome the elastic and nonelastic airway resistance (R) of the respiratory system. The relationship between R and {Delta}P across the airway is expressed as

where V is the flow of gas.1 During laminar flow, the resistance is calculated from the Hagen-Poiseuille equation, and the above formula can be rearranged to

where L is the length of the airway, µ is the viscosity of the gas, and r is the radius of the airway.2 However, in the large airways, such as the trachea, V exceeds the critical velocity and becomes turbulent.3 This transition to turbulent V occurs at a Reynolds number of approximately 2,300, and V becomes completely turbulent at a Reynolds number of 4,000.2 R across the trachea becomes directly proportional to V2 and inversely proportional to the radius of the trachea (rT) to the fifth power:

where p is the density of the gas and f is the frictional factor.4

When a pediatric patient receives endotracheal intubation, the endotracheal tube that is initially selected possesses an internal diameter that is commonly derived from the following formula5 :


The relationship of the internal diameter of the endotracheal tube to the diameter of the tracheal lumen and the implications of such a relationship for respiratory mechanics have not been investigated fully in the pediatric population.

Pressure and R across the trachea for a constant V are inversely related to rT5. If the tracheal X after intubation is calculated as:

then R and {Delta}P will be increased by (1/X)5 in the intubated trachea. Our objectives were to retrospectively measure the actual ratio between the rETTs and the rTs following the intubation of pediatric patients with respiratory failure and to calculate the derived increase in R and {Delta}P across the intubated tracheas. We hypothesize that our measured and calculated data will help clinicians to understand better the difficulties that some patients may encounter during periods of spontaneous breathing through an endotracheal tube.


    Materials and Methods
 TOP
 Abstract
 Introduction
 Materials and Methods
 Results
 Discussion
 References
 
Twenty consecutive pediatric patients whose tracheas had been intubated for respiratory failure and who received a CT scan of the lung as part of their diagnostic evaluation were included in our study. All patients had received placement of an endotracheal tube, with the size of the tube derived from the following standard formula: (age in years/4) + 4. Patient’s ages and the diagnoses they received are listed in Table 1 . CT scan images of the trachea at and around the level of the thoracic inlet were selected for each patient, and digital images were created with a scanner (Scan Jet 5P; Hewlett Packard; Singapore) attached to a personal computer (model 300GL; IBM; Austin, TX). The scanned CT images then were magnified to allow for accurate measurements (Fig 1 ). Two separate investigators (K.B. and M.R.) measured the rTs and rETTs. There was no significant variance between measurements at various cuts; the individual patient’s average value was used to calculate X. The factor by which the tracheal R (or {Delta}P) had increased secondary to endotracheal intubation, (1/X)5, was calculated for each patient. Data regarding tracheal R in the young pediatric age group are unavailable. The known normal tracheal R in adolescents and adults has been determined to be approximately 0.07 cm H2O/L/s.6 Therefore, to obtain the calculated value of R for an intubated trachea for this age group, we multiplied (1/X)5 by the known normal value for tracheal R:

Utilizing an inspiratory V of 1 L/s (60 L/min), the {Delta} P across the intubated trachea ({Delta}Pint) becomes


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Table 1. Patient Age and Diagnosis

 


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Figure 1. Top: an original CT scan image (patient 1) at the level of the thoracic inlet. Bottom: a magnified computer image of the CT scan made to enable accurate measurements of rT and rETT.

 

    Results
 TOP
 Abstract
 Introduction
 Materials and Methods
 Results
 Discussion
 References
 
Data are presented as mean ± SD. The mean age of our patients was 6.4 ± 7.2 years. The measured values of X ranged from 0.33 to 0.65 (mean, 0.55 ± 0.08) (Table 2 ). The factor (1/X)5 ranged from 8.6 to 255.5 (mean, 33.9 ± 52.5). Using an inspiratory flow of 1 L/s, the {Delta}Ps would be expected to increase from the known 0.07 cm H2O for a nonintubated trachea for adolescents and adults to a mean of 2.4 ± 3.7 cm H2O (range, 0.6 to 18 cm H2O). In two of our patients (10%), X was < 0.5 (0.33 and 0.44). In these patients, the calculated {Delta}P would be expected to significantly increase to 18 and 4.2 cm H2O, respectively. In two other patients (10%), the ratio was 0.65, and, thus, the calculated {Delta} P was only 0.5 cm H2O.


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Table 2. Patient Airway Data

 

    Discussion
 TOP
 Abstract
 Introduction
 Materials and Methods
 Results
 Discussion
 References
 
The substitution of an endotracheal tube for the trachea in critically ill patients results in an additional resistive load imposed on the respiratory muscles and, thus, a possible increase in the work of breathing (WOB).7 Calculating the actual WOB during the process of weaning from mechanical ventilation might be clinically valuable when selecting the appropriate amount of pressure support ventilation required to reduce the WOB to a specific level.8 However, calculating the WOB based on the Campbell diagram entails the use of a pneumotachograph and the insertion of an intraesophageal balloon catheter to obtain the intrapleural pressure.9 While this is a simple method, it is invasive. The determination of the pressure drop across the endotracheal tube in order to calculate R or its contribution to the WOB for various rates of V is similarly invasive; it requires the insertion of a catheter into the distal tip of the endotracheal tube for pressure measurements10 and is dependent on the level at which the catheter tip is located.11 Additionally, the intraluminal catheter reduces the cross-sectional area of the endotracheal tube, thus artificially increasing R.11 The Blasius resistance formula and the acoustic Blasius technique provide noninvasive methods to calculate the pressure drop across an endotracheal tube, but requires an accurate determination of the viscosity, density, and V of the delivered gas in addition to the endotracheal tube diameter.12 13 These methods could have been considered for our patients had we planned a prospective study. Chowienczyk et al14 describe a noninvasive flow-interruption device to determine the level of airway R; however, the data generated are for the complete airway and not the trachea alone. Likewise, the body plethysmograph technique measures not just the tracheal R, but R for the entire airway14 ; additionally, this method would not be technically feasible in our ICU patients.

Our retrospective study was based on the assumption that endotracheal intubation results in a measurable reduction in the lumen of the airway through which gas is delivered to the smaller airways and alveoli. The extent of this reduction has not been studied fully in the pediatric age group and, thus, became one of the goals of our study. Various techniques have been described to measure the airway caliber, including quantitative videobronchoscopy,15 CT scanning,16 and the acoustic reflection method.17 However, there is a paucity of reports in which artificial airway calibers are measured in relation to the tracheal calibers in pediatric patients whose tracheas were intubated. Our results indicate that the commonly used formula, (age in years/4) + 4, to determine the endotracheal tube size prior to intubation, leads to the selection of endotracheal tubes with diameters that are 40 to 50% smaller than the trachea. These findings are supported by previous measurements of tracheal calibers.16 An evaluation of the clinical significance of the reduction of the tracheal caliber with respect to airway R was the second goal of our study.

R across a large artificial airway is inversely related to the internal radius of that airway raised to the fifth power. During positive-pressure mechanical ventilation, adjustments in the ventilator settings easily can overcome the R of a narrow artificial airway. However, during spontaneous ventilation, the patient has to generate the necessary {Delta}P to overcome the added R of an endotracheal tube; this might result in signs of increased effort and discomfort. The inverse (1/X)5 indicates that even a slight difference between the caliber of the endotracheal tube and the trachea might result in significantly higher R. In spontaneously breathing patients, pressure support is often utilized to alleviate this additional WOB. Brochard et al18 reported that during the weaning process from mechanical ventilation and extubation of the trachea the addition of pressure support resulted in the greatest success compared to other weaning strategies.

Our data revealed three interesting facts. First, in the majority of our patients (70%), X was similar, between 0.5 and 0.6. Therefore, the factor (1/X)5 predicted an increase in tracheal R between 11- and 32-fold. Second, this common X was similar among all ages studied. Last, when X is < 0.5, the factor (1/X)5 becomes extremely high, as found in two of our patients (patients 1 and 9). In these patients, the resistance of their intubated tracheas had increased by 255- and 60-fold, respectively. Assuming that pressure and R are directly proportional, then the {Delta}P required to overcome R would increase by the same factor. Had we known the normal tracheal R of every patient in our study, the calculated increase in R could have been converted into real {Delta}P values for specific rates of inspiratory V. Moreover, an appropriate level of pressure support could have been chosen to balance the calculated increase in {Delta}Ps and to minimize the effect of the added R due to the endotracheal tube.

Data regarding the dimensions of the pediatric and adolescent16 19 20 airways have been reported. The R of infant endotracheal tubes21 is known as well. However, the tracheal R in pediatric patients is unknown. Pedley et al6 have determined the tracheal resistance in adults to be approximately 0.07 cm H2O/L/s. Since our data showed that the tracheal caliber reduction factor is similar among all ages, we used this value to calculate the resistance of the intubated trachea for the various values of X found in our patients. Our results show that we can expect tracheal R to increase due to intubation by 33.9 ± 52.5-fold (range, 8.6- to 255-fold). To maintain an inspiratory flow rate of 1 L/s, the {Delta}P across the intubated trachea would increase from the known 0.07 cm H2O to a mean of 2.4 ± 4.5 cm H2O (range, 0.6 to 18 cm H2O). In two of our patients, the rT/rETT ratios were < 0.5 (0.33 and 0.44, respectively); this translated into a much greater increase in the calculated {Delta}P, 18 and 4.2 cm H2O, respectively. When X is between 0.5 and 0.6, a pressure support of 2 to 3 cm H2O is sufficient to offset the increase in the {Delta}P required to maintain a V of 1 L/s. If rates of inspiratory V increase or decrease, then the pressure support would need to be adjusted accordingly. Similarly, large values of X would dictate that a large amount of pressure support is needed. In patient 1, X was 0.33. In this patient, approximately 18 cm H2O of pressure support would be required to offset the tracheal tube R. These data are similar to those of Banner et al,22 who described a mean pressure support of 13.5 ± 4.5 cm H2O to reduce the WOB to 0 in their study of 11 adult patients and 4 pediatric patients.

The limitations of our study emanate from the fact that it was retrospectively conducted and, therefore, actual measurements of parameters, such as pressure drops across the endotracheal tube, tracheal R, and rates of V, were not obtained. Moreover, we used a previously published value for tracheal R (0.07 cm H2O/L/s) in studied adults6 as the basis for our calculations. While no data are available for the tracheal R in the pediatric population, the value obtained by Pedley et al6 is similar to the values extrapolated from the Moody diagram plots of adult endotracheal tubes published by Lofaso et al.12 An additional limitation of our study is the assumption of a constant flow rate for our calculations, as opposed to integrating the V differential across time. While patients’ V rates are not constant,23 our hypothetical mean V rate of 1 L/s is consistent with the V levels utilized for the in vivo and in vitro testing of endotracheal Rs.10 11 12 13 Lastly, the fact that endotracheal tubes are frequently curved or bent was ignored in our study, yet this may have a significant effect on respiratory mechanics.23

In summary, calculating the endotracheal tube size by using the formula (age in years/4) + 4 may occasionally result in the insertion of an endotracheal tube that imposes a high R and does not permit comfortable spontaneous breathing. During assisted mechanical ventilation, the problems of increased R secondary to a small endotracheal tube are usually overcome by the ventilator’s power. However, during spontaneous ventilation, increased patient effort may be due in part to a large reduction in airway caliber. In such instances, a CT scan of the chest can provide data to calculate this factor. Based on our results, if X < 0.5, the clinician should be advised that the pressure support level required to achieve comfortable breathing is likely to exceed what he or she is accustomed to delivering.


    Footnotes
 
Abbreviations: {Delta}P = pressure gradient; rETT = radius of the endotracheal tube; R = resistance; rT = radius of the trachea; V = flow; WOB = work of breathing; X = caliber reduction ratio

Received for publication September 27, 1999. Accepted for publication February 24, 2000.


    References
 TOP
 Abstract
 Introduction
 Materials and Methods
 Results
 Discussion
 References
 

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  9. Banner, MJ, Jaeger, MJ, Kirby, RR (1994) Components of the work of breathing and implications for monitoring ventilator dependent patients. Crit Care Med 22,515-523[ISI][Medline]
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