A Comparison of Gas Flow Resistance in Parker Flex-tip and Mallinckrodt RAE Nasal Endotracheal Tubes THESIS Presented in Partial Fulfillment of the Requirements for the Degree Master of Science in the Graduate School of The Ohio State University By Joshua L. Perry, D.D.S. Graduate Program in Dentistry The Ohio State University 2013 Dr. Simon Prior – Advisor Dr. William Johnston Dr. William Brantley Copyright by Joshua L. Perry 2013 Abstract Introduction: The newer Parker Flex-Tip endotracheal tube causes less trauma and/or bleeding than more traditional designs during naso-tracheal intubation. However, the Parker tube appears to deform to a greater extent during normal use than other endotracheal tubes. This study aimed to investigate the resistance to gas flow that both the Mallinckrodt RAE and Parker Flex-Tip demonstrate, and how these two types of tubes may differ in their ability to withstand the deformation caused by thermosoftening and clinical positioning during normal use. Methods: Mallinckrodt RAE (Mallinckrodt Medical, Dublin, Ireland) and Parker Flex-Tip (Parker Medical, Highlands Ranch, CO) cuffed nasal endotracheal tubes, sizes 4.0, 4.5, 5.0, 5.5, 6.0, 7.0, 7.5 were connected to two Certifier FA Plus high flow modules (TSI Incorporated, Shoreview, MN), one connected to the proximal and the second, via a 90° fitting, to the distal end of each tube. A precise gas flow of 6 L/min was confirmed and measurements of pressure were collected at both ends of each tube as each tube was bent to angles of 70, 60, 50, and 45 degrees. ii Statistical analysis was done using a repeated measures analysis of variance and making a Satterthwaite adjustment to degrees of freedom to eliminate any bias due to heteroscedasticity. The alpha level was set at 0.05. The three main effects found were the brand of the tube, the internal diameter of the tube, and the degree of bend of the tube. Results: None of the two-way interactions tested was found to be statistically significant (P≥0.198) (Table 1). However, the Parker Flex-tip nasal endotracheal tube, when compared to the Mallinckrodt RAE tube, demonstrated a statistically significant higher resistance to gas flow, at 98°F, over the entire range of tube diameters tested at both 50° and 60° bends (P=0.013) (Table 2) (Figure 4). Conclusion: As is to be expected, smaller diameter nasal endotracheal tubes are associated with an increased resistance to gas flow. Interestingly, the resistance to gas flow was shown to be greater in the Parker Flex-tip nasal endotracheal tube under the conditions of our testing. When used properly, the Parker Flex-tip nasal endotracheal tube has been shown to cause less trauma and epistaxis during routine naso-tracheal intubation. However, the increased resistance to gas flow may have a negative impact on the physiologic work of breathing in nasally intubated patients; particularly in the smaller size tubes used in the pediatric population. The physiological impact of this in terms of iii the increased work of breathing that may be required through a Parker tube warrants further investigation. iv Acknowledgments I would like to acknowledge Drs. Simon Prior, William Johnston, and William Brantley for the time and effort they have given to this research project. A special thank you to Dr. Simon Prior for his help and guidance, not only on this research project, but throughout my anesthesia residency. I would also like to acknowledge Matthew Gray, Biomedical Electronics Technician at the Wexner Medical Center, for his expertise and assistance in the design and execution of our experiments. v Vita January 21, 1984.......................................... Born in Bellefontaine, Ohio 2006 ............................................................ B.S. Exercise Science, Miami University 2011 ............................................................ D.D.S., The Ohio State University 2011 to present ........................................... Dental/Maxillofacial Anesthesiology Residency, The Ohio State University College of Dentistry Fields of Study Major Field: Dentistry Minor Field: Anesthesiology vi Table of Contents Abstract .......................................................................................................................... ii Acknowledgments ........................................................................................................... v Vita ................................................................................................................................ vi Table of Contents .......................................................................................................... vii List of Tables ............................................................................................................... viii List of Figures ................................................................................................................ ix Chapter 1: Introduction .................................................................................................. 1 Chapter 2: Methods ......................................................................................................... 5 Chapter 3: Results ......................................................................................................... 10 Chapter 4: Discussion ................................................................................................... 12 Chapter 5: Conclusion ................................................................................................... 15 Appendix A: Tables ...................................................................................................... 16 Appendix B: Figures ..................................................................................................... 19 References .................................................................................................................... 22 vii List of Tables Table 1: Resistance Data: R = pressure/flow ..................................................................16 Table 2: AVONA Data ..................................................................................................17 Table 3: Tukey Pairwise Comparisons ..........................................................................18 viii List of Figures Figure 1: Clinical Deformation of the Nasal Endotracheal Tube....................................19 Figure 2: Experimental Set-up ......................................................................................20 Figure 3: Grid for Experimental Measurements ............................................................20 Figure 4: Bar Graph – Comparisons of Resistance ........................................................21 ix Chapter 1: Introduction Nasal endotracheal intubation is preferred for several reasons by both oral and dental surgery providers. Foremost among them, it allows unobstructed access to the oral cavity. It also permits free movement of the mandible and maxilla during orthognathic surgery, and significantly minimizes the possibility of having the tube unintentionally damaged or displaced during treatment. Nasal endotracheal tubes are manufactured with thick-walled, medical grade, polyvinyl chloride, much the same as oral endotracheal tubes. They are, however, subject to many forms of thermosoftening: exposure to body temperature, increased ambient temperature, and even intentional softening by the anesthesiologist prior to intubation. Placement in warm saline, blanket warmers, or next to a heated anesthetic vaporizer are common practices seen clinically. Thermosoftening characteristics of nasal endotracheal tubes improve navigability of the tube through the nasal passages and reduce damage to nasal mucosa and epistaxis.1 The nasal cavity is a fragile environment covered with a sensitive and well perfused epithelium. It has a particularly variable anatomical structure and one that is very difficult to visualize during the routine passage of a nasal endotracheal tube.2 The common result being that nasal epistaxis is often observed during nasal intubations. Although the above mentioned characteristics and practices of thermosoftening do provide benefits, the structural integrity of the tubes may be undermined and cause 1 changes to the flow characteristics of gases; most notably, increases in resistance and therefore work of breathing. Furthermore, the materials and processes by which nasal endotracheal tubes are constructed differ between manufacturers, and perhaps to such an extent that even standard clinical use may have different effects on the breathing environment Flow can be described as the volume of gas passing a cross sectional area per unit of time, with the two main patterns of flow being laminar and turbulent. Endotracheal tubes, whether oral or nasal, exhibit both types of flow with increasing amounts of turbulent flow attributed to curvatures in the tube.3 In particular; nasal endotracheal tubes are designed to approximate the anatomical path of the nose and pharynx. As a result, they have a distinctive curvature as part of their design. The Hagen-Poiseuille equation states that resistance varies inversely to the fourth power of the radius. However, this relation applies only to laminar flow. At gas flows and tube diameters that we use clinically the flow is assumed to be turbulent. Therefore, the resistance of nasal endotracheal tubes must be determined empirically.4,5 Based on previous experiments, resistance can be calculated by dividing the gas pressure by the flow rate. Resistance is expressed in cm H2O/L/sec.3,6,7 Changes in the internal diameter of nasal endotracheal tubes do occur during clinical use as a result of thermosoftening and manipulation. The preformed bend of nasal endotracheal tubes is an area of concern. It has been noted clinically that this particular area of the tube does not hold its original circular form and tends to collapse in on its self, decreasing the internal diameter of the tube. The Parker Flex-Tip nasal 2 endotracheal tube is a recent addition to the anesthesiologist’s selection of intubating tubes and brought with it a unique and very advantageous design of its distal tip (navigating end). However, regular use of this particular nasal endotracheal tube for oral and maxillofacial surgeries has revealed a tendency of this tube to collapse at its preformed bend as the tube exits the nasal cavity (Figure 1). In comparison, one type of nasal endotracheal tube may be more capable of withstanding the manipulation and changes that occur with thermosoftening and clinical use. With a reduction in the internal diameter of endotracheal tubes, an increased resistance to gas flow is observed. The effect varies for different sizes of tubes and is seen more profoundly in smaller sized endotracheal tubes, such as those used in pediatric anesthesia. This increased resistance may result in an increased work of breathing and place a considerable load on the respiratory muscles.8,9 In the general surgery situation this would be seen most notably during spontaneous breathing trials, assessing whether or not patients are ready to be weaned off mechanical ventilation. In dentistry, it is not uncommon to have intubated patients breathing spontaneously for the entire duration of the case. The implications of such influences on the work of breathing may be even more pronounced in patients with conditions such as asthma and COPD. Additionally, should this increased resistance prove to be clinically significant, the greater compliance of the pediatric thorax may result in adequate gas exchange being affected.9,10 For these patients, the extra work of breathing needed to overcome the increased resistance from thermosoftened and collapsed endotracheal tubes could lead to problems with spontaneous ventilation. 3 Both Parker Flex-Tip and Mallinckrodt RAE tubes are commonly used for nasal intubations. While being clinically useful, nasal intubations typically require choosing a smaller sized tube than the anesthesiologist may use for the same patient being orally intubated. The combination of smaller tube size and the inherent curvature of the nasal endotracheal tube increase the probability that thermosoftening will affect the structural integrity of the tube. We wished to investigate the resistance to gas flow that both the Mallinckrodt RAE and Parker Flex-Tip demonstrate, and how these two types of tubes may differ in their ability to withstand the deformation caused by thermosoftening and clinical positioning. This was done by testing the flow characteristics of oxygen through the tubes under simulated clinical conditions. Our null hypothesis is that there is no statistically significant difference in the resistance to gas flow between the Parker FlexTip and Mallinckrodt RAE at a temperature and degree of bend found clinically. 4 Chapter 2: Methods Experimental: Mallinckrodt RAE (Mallinckrodt Medical, Dublin, Ireland) and Parker Flex-Tip (Parker Medical, Highlands Ranch, CO) cuffed nasal endotracheal tubes of the sizes 4.0, 4.5, 5.0, 5.5, 6.0, 7.0, 7.5 were used for testing in this study. One tube of each size was stored in a 22.2°C (72°F) room for 24 hours prior to testing. Each tube was kept in its original packaging and no manipulation of the tube was done prior to removal from its package. All tests were conducted using a GE Datex-Ohmeda Excel 210 SE anesthesia machine connected to a central oxygen source. Rubber circuit module test plugs were placed in lieu of a breathing bag and to block the expiratory limb of the anesthesia machine. The oxygen flowmeter was set to 6 L/min. Subsequently, the adjustable pressure-limiting valve was adjusted to maintain a circuit pressure of 70 cm H2O throughout our tests. Two Certifier FA Plus high flow modules (TSI Incorporated, Shoreview, MN) with corresponding digital interfaces were used to conduct our tests. Both of the high flow modules were calibrated by a biomedical electronics technician prior to use. The settings of the two digital interfaces were adjusted to allow analysis of the flow and pressure of oxygen. The high flow modules were in-line positioned such that they followed the correct flow of gas indicated by the blue label “FLOW →” on the front of 5 the module. The first high flow module (HFM1) was connected to the inspiratory limb of the anesthesia machine with a 48-inch reusable corrugated breathing circuit tube. The distal port of HFM1 was connected to an airway pressure fitting and the corresponding ¼ inch diameter silicone pressure tubing was connected to the positive pressure port of the high flow module (Figure 2). The second high flow module (HFM2) was fitted with the same airway pressure fitting and tubing on its proximal port with the distal port left open to the atmosphere (Figure 2). The first Mallinckrodt Nasal RAE tube to be tested was removed from its package and cut with scissors at a mark two centimeters proximal to the cuff of the tube. This was done to provide a uniform circular tip to all of the tubes and to remove the possibility of the cuffed portion of the tube interfering with the set-up. The cuffed portion of the tube that was removed was then discarded. The distal end of our remaining RAE tube was then secured to a 90° fitting with black electrical tape (Figure 3). The tubes were positioned carefully, making sure that the open end of the tube did not contact the fitting and obstruct the flow of oxygen. Once secured, the tube was connected to the two high flow modules with the proximal end of the tube connected to HFM1 and the distal end, with the 90° fitting, connected to HFM2. A precise flow of 6 L/min was confirmed via the digital interface. All measurements for use in our statistical analysis were collected from HFM1. HFM2 was used to check for consistent, unobstructed flows of gas and to confirm that the length of the tube distal to the preformed bend did not have any influence on the pressure and flow measurements. 6 A grid with angles of 70, 60, 50, and 45 degrees was constructed on white poster board and used to systematically manipulate the tubes to pre-marked angulations for each measurement of flow and pressure (Figure 3). Each of 14 different tubes we tested comes from the manufacturer pre-formed at a slightly different angulation. Therefore, our initial measurement was done at this “out of package” angulation and not manipulated. Each subsequent measurement was done with the tube manipulated to the pre-marked angulations described above. The tube was secured at each angulation with pins to allow sufficient time for the tube to conform to its new position and to obtain accurate measurements. As a result, there were five measurements of pressure and flow for the RAE tube being tested at 22.2°C. This same process was repeated for each size of RAE and Parker Flex-Tip tube. Measurements of pressure and flow were collected three separate times for each tube in order to calculate a mean pressure and identify any obscure pressure measurements. A new assortment of the same tubes (size and type) as described previously was used for our second series of tests. Again, the tubes were stored at 22.2°C for 24 hours and subsequently cut 2 centimeters proximal to the cuff prior to testing. This series of tubes was then suspended in a 36.7°C (98°F) water bath for at least five minutes. After the minimum five minutes, the tube to be tested was removed from the water bath and the desired 36.7°C temperature of the tube confirmed using a laser thermometer. Our requirement for testing was a tube temperature between 35°C and 37.8°C. If at any time during the experiment the temperature of the tube was not within our designated range, it was placed back into the water bath for at least two minutes until the desired temperature 7 was reached again. Measurements of pressure and flow for the warmed 36.7°C tube were collected using the same method and angulations described for those tubes tested at 22.2°C. Resistance to gas flow is an important component in the equation of physiologic work of breathing. Our collected pressure and flow data was used in each case to calculate resistance by dividing the mean of our three measurements of pressure by flow as described by Manczur6 and Wright7. Statistical: Although multiple sets of data were collected, the purpose of our study was to analyze only that data set determined as best representative of usual clinical conditions. As a consequence, the pressure data only at the temperature of 98°F and at bends of 50° and 60° was analyzed. This was done using a repeated measures analysis of variance. This incorporated the method of using maximum likelihood estimates for the variances and making a Satterthwaite adjustment to degrees of freedom to eliminate any bias due to heteroscedasticity. The alpha level was set at 0.05. The three main effects were the brand of the tube, the internal diameter of the tube, and the repeated factor, the degree of bend in the tube. Further, this ANOVA tested the statistical significance of every possible two-way interaction of these three main effects. The analysis was done using the MIXED procedure in SAS® Proprietary Software 9.2 (SAS Institute Inc., Cary, NC, USA). 8 Tukey pairwise comparisons were used whenever a significant effect was found involving more than one degree of freedom in the effect. 9 Chapter 3: Results All of the calculated values of resistance are presented in Table 1. The subset of data that was used for our statistical analysis has been highlighted. None of the two-way interactions tested was found to be statistically significant (P≥0.198) (Table 1). However, the Parker Flex-tip nasal endotracheal tube, when compared to the Mallinckrodt RAE tube, demonstrated a statistically significant higher resistance to gas flow, at 98°F, over the entire range of tube diameters tested at both the clinically representative 50° and 60° bends (P=0.013) (Table 2) (Figure 4). A statistically significant difference was also detected between the mean resistance to gas flow between the two bends (P=0.020) (Table 2). This was demonstrated for both brands of tubes and over all diameters tested. The resistance to gas flow at a bend of 60° was higher than the resistance to gas flow at a bend of 50° (Figure 4). Finally, a statistically significant difference between the mean resistance to gas flow at the various diameters (P<0.001) was found for both brands of tubes and the two bends tested (Table 2). As the diameter of the tube decreases, the resistance to gas flow increases (Figure 4). 10 Our Tukey pairwise comparison of the effect ‘diameter’ is shown in Table 3. ‘Rchange’ is the difference in the average resistance to gas flow of ‘Diameter B’ compared to ‘Diameter A’. Nasal endotracheal tubes, in general, demonstrate a difference in resistance to gas flow with incremental decreases in diameter (5.0 to 4.5, 4.5 to 4.0 etc.). A statistically significant change in resistance is revealed in the smaller diameter tubes. 5.5 to 5.0 (P=0.002). 5.0 to 4.5 (P=0.001). 4.5 to 4.0 (<0.001). This change in resistance to gas flow between incremental sizes becomes non-significant at diameters 6.0 and greater. 11 Chapter 4: Discussion Based on our results, the Parker Flex-tip nasal endotracheal tube, when compared to the Mallinckrodt RAE, demonstrated higher resistance to gas flow, at 36.7°C (98°F), over the range of tube diameters tested at both 50° and 60° bends. We found, however, that the difference in the mean resistance to gas flow between the two brands was independent of either bend and/or diameter. This may have been due to the fact that such a dependency does not exist, but we also have to recognize the possibility that our limited initial experimental design may not have been able to identify either or both of these dependencies. A larger sample size and/or further testing of our collected data may elucidate such interactions if they exist. As is to be expected, smaller diameter nasal endotracheal tubes are associated with an increased resistance to gas flow following the principles and experiments described by Mitchell3, Manczur6, Wright7, and El-Khatib8. Interestingly, the resistance to gas flow was shown to be greater in the Parker Flex-tip nasal endotracheal tube in all comparisons under the conditions of our testing. The physiologic implications of this difference may be of a magnitude worth investigating further. Should this difference be physiologically interesting, then this would logically be of particular importance for spontaneously ventilating pediatric patients or those with respiratory conditions such as asthma or COPD. It has been suggested that the presence of a nasal endotracheal tube 12 may doubles the work of breathing in chronically intubated adults and lead to respiratory failure in certain children and infants.11 Furthermore, in vivo measurements of resistance are generally higher than in vitro measurements, perhaps because of secretions, head and neck positioning, or increased turbulence. Based on this information, it seems appropriate to question how great the impact of this increased resistance to gas flow is in the smaller diameter nasal endotracheal tubes when these other factors are taken into consideration. Often times the anesthesiologist is presented with a choice between two different sizes of nasal endotracheal tube. Does he/she choose the larger size tube that will allow higher volumes of unobstructed gas flow at the expense of traumatizing the fragile epithelium of the nasal cavity? Or is the smaller size tube chosen in an attempt to reduce possible injury or irritation at the expense of higher resistance to gas flow and respiratory compromise? Based on our results, this decision does not have as many potential implications when choosing between incremental sizes that are larger than 6.0. However, when dealing with tubes that are smaller than 6.0, the decision potentially weighs more heavily on respiratory physiology, and perhaps more so when using a Parker Flex-tip nasal endotracheal tube. That the material used in the Parker Flex-tip naso-tracheal tube is slightly more prone to deformation may be suggested by the manufacturer’s later decision to package these tubes in pre-formed cases; an attempt to maintain the original shape and deter any manipulation of the tubes that may compromise structural integrity prior to immediate clinical use. 13 When used properly, the Parker Flex-tip nasal endotracheal tube has been shown to cause less trauma and epistaxis during routine naso-tracheal intubation. Our study has shown however, a statistically significant difference in its resistance to gas flow compared to the Mallinckrodt RAE under simulations of relevant clinical situations, with the Parker Flex-tip showing the higher resistance, especially in the smaller sizes. In vivo investigations would now be valuable to determine if the higher resistance to gas flow that we found in the Parker-Flex tip tube has a negative impact on the physiologic work of breathing in nasally intubated patients; particularly in the smaller size tubes used in the pediatric population. It may be, that despite the statistically significant difference demonstrated between Parker Flex-tip and Mallinckrodt RAE tubes in the bench top situation, that both brands still provide adequate flow of gas despite undergoing deformation from thermosoftening and clinical positioning. However, knowing that the pediatric population has a higher thoracic compliance, it seems plausible that there would be greater sensitivity to the impact of the higher resistance to gas flow that the Parker Flex-tip demonstrates, and this existing uncertainty warrants further investigation. 14 Chapter 5: Conclusion Parker Flex tip and Mallinckrodt RAE nasal endotracheal tubes are commonly used in the dental surgery setting. This experiment has shown that the resistance to gas flow is different between the two brands of tubes, with the Parker Flex-tip demonstrating higher resistance to gas flow under clinically relevant situations. Further testing should be done to determine the physiologic impact of our findings. 15 Appendix A: Tables Ø (mm) Tube Temp Bend 7.5 7.0 6.0 5.5 5.0 4.5 4.0 RAE 72° As received 0.061 0.075 0.105 0.116 0.162 0.221 0.338 45° 0.065 0.077 0.107 0.122 0.167 0.236 0.350 50° 0.068 0.078 0.110 0.123 0.171 0.241 0.366 60° 0.069 0.078 0.114 0.130 0.182 0.254 0.364 70° 0.071 0.080 0.117 0.137 0.199 0.295 0.394 As received 0.066 0.074 0.104 0.116 0.163 0.221 0.342 45° 0.068 0.077 0.107 0.121 0.168 0.237 0.355 50° 0.068 0.078 0.110 0.124 0.183 0.262 0.367 60° 0.069 0.079 0.115 0.132 0.192 0.279 0.365 70° 0.071 0.081 0.117 0.138 0.200 0.307 0.395 As received 0.066 0.075 0.106 0.116 0.169 0.241 0.342 45° 0.068 0.078 0.111 0.123 0.178 0.250 0.352 50° 0.069 0.081 0.113 0.125 0.180 0.264 0.368 60° 0.072 0.081 0.120 0.132 0.189 0.279 0.382 70° 0.077 0.091 0.125 0.142 0.207 0.301 0.421 As received 0.066 0.076 0.107 0.117 0.171 0.242 0.342 45° 0.069 0.079 0.114 0.123 0.184 0.254 0.360 50° 0.070 0.082 0.119 0.127 0.197 0.268 0.381 60° 0.074 0.086 0.124 0.137 0.204 0.298 0.426 70° 0.079 0.098 0.131 0.149 0.216 0.334 0.471 RAE Parker Parker 98° 72° 98° Table 1: Resistance Data: R = pressure/flow. Units = (cmH2O)/(L/sec). Ø = Diameter 16 Type 3 Tests of Fixed Effects Num Den DF DF Effect F Value Pr > F Tube 1 4.3 16.67 0.0130 Diameter 6 4.3 860.53 <0.0001 Bend 1 6 9.88 0.0200 Tube*Diameter 6 4.3 2.24 0.2169 Tube*Bend 1 6 2.09 0.1983 Diameter*Bend 6 6 1.03 0.4863 Table 2: AVONA Data: alpha = 0.05 17 R-change (cm Diameter A (mm) Diameter B (mm) AdjP H2O)/(L/sec) 4 4.5 0.65 <.001 4 5 1.14 <.001 4 5.5 1.53 <.001 4 6 1.61 <.001 4 7 1.82 <.001 4 7.5 1.88 <.001 4.5 5 0.50 0.001 4.5 5.5 0.88 <.001 4.5 6 0.96 <.001 4.5 7 1.17 <.001 4.5 7.5 1.24 <.001 5 5.5 0.38 0.002 5 6 0.46 0.001 5 7 0.68 <.001 5 7.5 0.74 <.001 5.5 6 0.08 0.386 5.5 7 0.29 0.005 5.5 7.5 0.36 0.002 6 7 0.21 0.018 6 7.5 0.28 0.006 7 7.5 0.07 0.519 Table 3: Tukey Pairwise Comparisons (Pairwise comparisons of mean resistance to gas flow between each size of endotracheal tube tested. The underlined data shows the incremental size comparisons that were most relevant for our study.) 18 Appendix B: Figures Figure 1: Clinical Deformation of the Nasal Endotracheal Tube (Clinical placement of a size 5.5 Parker Flex-tip nasal endotracheal tube demonstrating the collapse that occurs at the preformed bend due to thermosoftening. The picture on the left was taken within minutes of initial intubation. The picture on the right was taken 30 minutes after intubation.) 19 Figure 2: Experimental Set-up (Experimental set-up demonstrating the connection of the endotracheal tube to the two high flow modules.) Figure 3: Grid for Experimental Measurements (Close up view of the grid placed behind the endotracheal tube to allow measurements to be taken at our predefined degrees of bend.) 20 Figure 4: Bar Graph – Comparisons of Resistance (Bar graph representing the difference in resistance to gas flow between the two brands of tube tested at 98°F. Each ‘P’ represents the Parker Flex-tip and each ‘S’ represents the standard tip (Mallinckrodt RAE) at the corresponding diameter and degree of bend. 21 References 1. Kim YC, Lee SH, Noh GJ, et al. Thermosoftening treatment of the naso-tracheal tube before intubation can reduce epistaxis and nasal damage. Anesth Analg. 2000;91:698-701. 2. Prior S, Heaton J, Jatana K, Rashid R. Parker Flex-tip and Standard-tip endotracheal tubes: A comparison during naso-tracheal intubation. Anesth Prog. 2010;57:18-24. 3. Mitchell M, Cheesman K. Gas, tubes and flow. Anaesthesia and Intensive Care Medicine. 2009;11:32-35. 4. Hendrick HHL. Comparative study of the different factors influencing resistance of tubes to gas flow. Acta Anaesthesiol Belg. 1980;31:307-315. 5. Grinnan DC, Truwit JD. Clinical Review: Respiratory mechanics in spontaneous and assisted ventilation. Critical Care. 2005;9:472-484. 6. Manczur T, Greenough A, Nicholson GP, Rafferty GF. Resistance of pediatric and neonatal endotracheal tubes: Influence of flow rate, size, and shape. Crit Care Med. 2000;28:1595-1597. 7. Wright PE, Marini JJ, Bernard GR. In vitro versus in vivo comparison of endotracheal tube airflow resistance. Am Rev Respir Dis. 1989;140:10-16. 8. El-Khatib MF, Husari A, Jamaleddine GW, et al. Changes in resistances of endotracheal tubes with reductions in the cross-sectional area. Eur J Anaesth. 2008;25:275-279. 9. Bolder PM, Healy TEJ, Bolder AR, et al. The extra work of breathing through adult endotracheal tubes. Anesth Analg. 1986;65:853-859. 10. Peters RM. The energy cost (work) of breathing. Ann Thorac Surg. 1969;7:51-67. 11. Doyle DJ, O’Grady KF. “Physics and Modeling of the Airway”. Benumof’s Airway Management; Principles and Practice. Ed. Jonathan Benumof, Ed. Carin Hagberg. Philadelphia: Mosby Elsevier, 2007. 88-99. 22
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