|
|
||||||||
NEUROREGULATION AND MOTILITY
Divisions of 1Pediatric Gastroenterology and 2Gastroenterology, University of California, San Diego, California; and 3Division of Gastroenterology, San Diego Veterans Affairs Medical Center, San Diego, California
Submitted 4 August 2005 ; accepted in final form 16 January 2006
| ABSTRACT |
|---|
|
|
|---|
intraluminal impedance; ultrasound imaging of the esophagus
Intraluminal impedance is a novel technique to record physical movement of gastric contents into the esophagus, i.e., GER. The combined impedance and pH catheter technique can record all types of reflux episodes, i.e., air, liquid, acid, and neutral (16, 18, 19, 2225). The technique is based on the measurement of electrical impedance between closely spaced electrodes positioned in the esophagus. Intraluminal multiple-site impedance recordings reveal that changes in impedance during GER occur in a retrograde fashion, from the distal to the proximal site in the esophagus. In fact, impedance recordings show that retrograde movement of air or liquid in the esophagus represents GER, and antegrade movement is the result of a swallowed bolus. We observed that the common cavity pressure wave seen in association with GER occurs simultaneously along the length of the esophagus during most of the instances. If common cavity pressure and changes in impedance are indeed markers of GER (physical movement of gastric contents, liquid, or air into the esophagus), it is not clear why the impedance wave should spread though the esophagus in a retrograde fashion and the common cavity pressure wave occurs simultaneously. We recorded GER using esophageal pressure, pH, impedance, and intraluminal ultrasound (US) imaging in normal subjects to better understand the genesis of the common cavity pressure wave associated with GER.
| METHODS |
|---|
|
|
|---|
Catheter assembly. A customized catheter assembly consisting of a 2-mm diameter, 4-channel solid-state pressure transducer catheter (Galtec, Ilse of Skye, Scotland), a 1.5-mm diameter Comfortec multiluminal impedance (MII)-pH impedance-pH probe (Sandhill Scientific, Highlands Ranch, CO), and a 1.2-mm 30 MHz high-frequency intraluminal US catheter (CVIS; Sunnyvale, CA) was used for the studies. The catheters were assembled and positioned in the esophagus in such a fashion that one pressure transducer, the pH sensor, and the US transducer were located at one level in the esophagus, 5 cm above the LES (Fig. 1). The other three pressure transducers were located in the stomach, 10 and 15 cm proximal to the LES. Impedance electrodes were located at 2, 4, 6, 8, 10, 14, 16, and 18 cm proximal to the LES, which allowed recording of impedance channels at levels 3, 5, 7, 9, 15, and 17 cm proximal to the LES. Thus simultaneous impedance, pressure, and US data were recorded at a level 5 cm above the LES, and simultaneous impedance and pressure were recorded at a level 15 cm above the LES. All physiological measurements were recorded on a physiological recorder (Sandhill Scientific), and US images were recorded in real time on an S-VHS recorder using a Hewlett-Packard System. The two recording equipments were synchronized using a video timer (Thalaner Electronics, Ann Arbor, MI).
|
Data analysis.
GER episodes were identified from the physiological recordings obtained in the postprandial period with either pH or MII criteria using Bio-view Analysis software, (Sandhill Scientific). Confirmation of reflux episodes was performed manually. Esophageal common cavity was defined as a sharp and sustained rise in end-expiratory esophageal pressure of
4 mmHg in 2 consecutive leads in association with GER (6). The onset of the esophageal common cavity was defined as the inflection point at the onset of the increase in the pressure. The computerized automated analysis software determined the time of GER entry into the esophagus from the MII recordings. The MII criterion for refluxate entry into the esophagus is a 50% reduction in the baseline impedance value. Velocity of refluxate movement, from 5 to 15 cm above the LES, by impedance criteria and common cavity pressure wave criteria were determined. The time resolution for the identification of pressure and impedance events, based on the frequency of data collection, was 0.1 s (100 ms). Therefore, events occurring within 0.1 s of each other were considered simultaneous.
US images starting 15 s before the GER to 15 s after the end of the esophageal contraction that cleared the GER (identified from physiological tracings) were digitized at a frequency of 100 ms using a digital video-editing system (Pinnacle DV500 and Adobe Premiere 6.0, Adobe Systems, Mountain View, CA). These US images were analyzed for 1) opening of the esophageal lumen (as a marker of GER bolus entry into the esophagus); and 2) cross-sectional area (CSA) of the lumen (as a marker of degree of esophageal distension during reflux) at the peak of distension. In addition, CSA of the muscularis propria of the esophagus (as a marker of longitudinal muscle contraction) (8, 9) was measured during randomly selected liquid reflux episodes. The time of lumen opening was identified as the first frame at which the mucosa separated from the edges of the catheter assembly for at least four consecutive frames. The luminal CSA at the peak esophageal distension was measured using graphing software (Sigma Scan Pro, Jandel Scientific, San Rafel, CA). The reflux entry into the esophagus and lumen CSA were determined for all reflux episodes, but the muscle CSA during GER was determined from the 10 randomly selected liquid GER sequences in which the entire circumference of the esophagus was clearly visualized on the US images. The time of onset of muscle CSA increase was when it increased at least 50% of the baseline value for at least 1 s. The muscle CSA was plotted against the esophageal pressure at 5 cm above the LES to determine the temporal correlation between the two. The duration of common cavity and the duration of increase in the muscle CSA during common cavity were determined. Differences in the time of bolus entry by impedance at 5 and 15 cm above the LES and onset of common cavity pressure at 5 and 15 cm above the LES were determined.
Statistical analysis. Synchrony between various physiological events was determined by comparing the time offset between various events against a test value of 0 s (simultaneously occurring events) using the single-value Student's t-test. A paired t-test was used to compare the velocity of bolus movement from 5 to 15 cm above the LES as determined by impedance and common cavity pressure. The duration of the common cavity pressure wave with the duration of the longitudinal muscle contraction events were evaluated by a paired-samples t-test. The Pearson's correlation coefficient was used to evaluate the relationship between luminal CSA and common cavity pressure individually in subjects with three or more GER episodes and the onset of the common cavity pressure wave with the onset of the increase in muscle CSA. Data are shown as means ± SE.
| RESULTS |
|---|
|
|
|---|
|
|
Progression of the common cavity pressure and impedance in the esophagus. The relationship between the progression of common cavity pressure and GER entry by MII criteria along the length of the esophagus, when both were present, was assessed during 55 GER episodes. Common cavity pressure reached the 15-cm site in all 55 episodes, but on the basis of the MII criteria of refluxate entry, GER failed to reach the 15-cm site during six (11%) episodes. Common cavity pressure waves occurred at the same time (simultaneously) between the 5- and 15-cm sites (Fig. 3) above the LES during the majority, 48 of 55 (79%), of GER episodes (time resolution, 0.1 s). On the other hand, GER (by MII criteria) arrived at 5- and 15-cm sites in the esophagus in a retrograde fashion (Fig. 3) in the majority, 47 of 49 (96%), of GER episodes with a mean time interval of 2.4 ± 1.8 s between the two sites. Only 6 of the 55 (11%) common cavity pressure waves were retrograde. However, the velocity of the retrograde movement of the GER bolus, as measured by the MII, was significantly slower than the retrograde velocity of pressure waves (10 ± 13 vs. 30 ± 20 cm/s; P < 0.05). One of the six MII episodes that failed to reach the 15-cm site occurred during the retrograde common cavity events.
Relationship between common cavity pressure and longitudinal muscle contraction of the esophagus. Synchronized M-mode US images and physiological tracings are shown in Fig. 3, A and B. In both figures, an increase in muscle thickness (a marker of longitudinal muscle contraction) coincides with the onset of common cavity pressure wave. The temporal correlation between common cavity pressure wave at 5 cm above the LES and contraction of the longitudinal muscle of the esophagus (changes in muscle CSA) at the same site was determined during 10 GER episodes (Fig. 4). In all of these episodes, there was a close temporal correlation between the onset of the common cavity pressure wave and the increase in esophageal muscle CSA (mean time difference < 0.1 s; Pearson's correlation coefficient = 1; P = 0.01). The muscle CSA remained elevated during the entire duration of the common cavity pressure wave, and it returned to the baseline with the termination of the common cavity (usually by an esophageal contraction wave). The duration of common cavity pressure was the same as the duration of the longitudinal muscle contraction (15.65 ± 2.58 vs. 15.81 ± 2.57; P = 0.061).
|
Simultaneous GER entry and common cavity pressure during air reflux. Five episodes of air reflux, as determined by MII criteria, were observed in three subjects. Three of these episodes occurred during the meal phase of the study and were not part of the postprandial data analysis. During all five air-reflux episodes, air arrived at the 5- and 15-cm sites simultaneously (as recorded by MII), and the onset of pressure wave at the two sites was also simultaneous. However, the onset of common cavity pressure wave occurred earlier than the arrival of air at the corresponding MII recording site during all of these air-reflux episodes. In all five episodes, US images revealed that first, there is an increase in the muscle thickness and muscle CSA, which is then followed by air entry into the esophagus (Fig. 5). Air entry into the esophagus resulted in a loss of US esophageal image during all of these episodes. The onset of common cavity pressure coincided with the increase in muscle thickness and muscle CSA rather than the entry of air into the esophagus.
|
| DISCUSSION |
|---|
|
|
|---|
The common cavity pressure wave is widely felt to be a marker of GER. It is thought to be the result of equalization of gastric pressure with esophageal pressure during GER. However, the equalization of pressure between the two cavities can only occur if there is physical movement of contents between the two cavities. During GER, movement of either air or liquid will be required to equalize pressures between the esophagus and the stomach. MII monitoring is a very sensitive technique to record air as well as liquid reflux. Our findings indicate that there is a significant difference between the onset of common cavity pressure and refluxate entry by MII criteria, arguing against common cavity pressure being directly related to the GER entry into the esophagus.
Could the differences in the timing of pressure and MII waves be related to the fidelity response of sensors and the definition of MII criteria of refluxate entry used in our study? The pressures were measured using solid-state pressure transducers that have high-fidelity response times. Similarly, the MII technique is based on the changes in electrical impedance, which has a high-fidelity response. The frequency of data acquisition was fairly fast, 30 Hz. We used a 50% reduction rather than the onset of reduction of electrical impedance as the MII criteria for the bolus entry in our study, as suggested by the simultaneous fluoroscopic and impedance recording studies of Silny and colleagues (21). It is possible that the MII criteria for refluxate entry may have contributed to the difference in the temporal correlation between the impedance and pressure waves. Changing the MII criteria for bolus entry (e.g., using 10% reduction in impedance signal) would shift the timing of bolus entry backward. The number of events where the impedance and pressure changes occur simultaneously would simply shift to where the onset of the impedance wave occurs before the onset of the pressure wave. Thus the change in MII criteria of determining the onset of bolus entry would further decrease or have little effect on the number of synchronous impedance and pressure reflux events. Furthermore, the observation that common cavity pressure occurs simultaneously, but the MII wave spreads in a retrograde fashion along the length of the esophagus during the majority of the instances, argues against common cavity pressure being related to the movement of gastric contents into the esophagus. It is possible that a small amount of air reflux preceded liquid reflux into the esophagus, which could account for the time differences observed between the propagation of the pressure wave compared with the fluid entry wave by the MII criteria. We think it is unlikely because 1) MII tracings were carefully scrutinized to assess for presence of air in the GER refluxate; 2) we studied subjects in the right decubitus position, which is associated with predominantly liquid reflux (13); and 3) we did not see air reflux preceding liquid reflux on our US images; the latter is very sensitive in detecting air in the esophagus. The choice of subject position in our study also explains the differences in the frequency of air reflux between ours and other studies. MII records reveal that the GER entry into the esophagus during air-reflux episodes can occur simultaneously along the length of the esophagus, which is most likely due to a rapid spread of air along the length of the esophagus compared with the liquid reflux contents. However, even during these air-reflux episodes, the onset of common cavity pressure wave and increase in muscle thickness precedes MII criteria of refluxate entry, further supporting our contention that the onset of common cavity pressure is not related to reflux of gastric contents into the esophagus.
Additional evidence that the common cavity is not due to equalization of gastric and esophageal pressure comes from the close inspection of the manometric recording in which LES pressure was recorded for extended periods of time using a sleeve sensor to determine the mechanism of GER (8, 9). These recordings show that the onset of common cavity pressure wave may precede complete relaxation of the LES by 12 s. Complete LES relaxation would be required if the common cavity were indeed related to equalization of gastric and esophageal pressures unless there is an increase in gastric pressure (stress reflux) during GER, which is not the case during majority of reflux episodes in normal subjects.
If common cavity pressure was related to the physical movement of reflux contents into the esophagus, principles of physics dictate that there would be a direct relationship between the volume of GER and the amplitude of common cavity pressure. We could not measure GER volume using our recording techniques but the CSA of the lumen of the esophagus is likely to be a surrogate for the volume of GER. We did not find a linear relationship between the common cavity pressure and the CSA of the esophagus during GER episodes either in the individual subjects or in the group data. These findings further argue against common cavity pressure being due to physical movement of gastric contents into the esophagus.
If it is not the movement of GER contents, then what causes the so-called "common cavity pressure wave"? We found a close temporal correlation between changes in common cavity pressure waves and the thickness as well as the CSA of the muscularis propria, both of which are measures of longitudinal muscle contraction (7, 11). A gradual increase in muscle thickness with a gradual increase in esophageal pressure seen during some GER episodes also supports our hypothesis that longitudinal muscle contraction is the cause of the increase in esophageal pressure. Longitudinal muscle contraction at the onset of TLESR has been described in several recent reports (17, 20). Because TLESR is the major mechanism of reflux in normal subjects, our finding of longitudinal muscle contraction with the common cavity pressure wave is consistent with those reports. Longitudinal muscle contraction at the onset of a common cavity pressure wave suggests at least two other possibilities as to the cause of the common cavity pressure wave: 1) the esophagus is a closed chamber between the upper and lower esophageal sphincters. The product of pressure and volume is constant in a closed chamber, and as the volume decreases, the pressure will increase (Boyle's Law) (10). Axial shortening of the esophagus as a result of longitudinal muscle contraction would be predicted to increase esophageal pressure. It may be that the change in the dimension of the esophagus, either before or during GER, could cause changes in its pressure. Second, the esophagus is a relatively compliant organ and, as a result, its pressure reflects intrathoracic pressure at rest. It may be that the contraction of longitudinal muscles renders the esophagus relatively less compliant and thereby prevents transmission of intrathoracic pressure to the lumen of the esophagus. Others and we have observed that the inspiratory negative pressure waves during common cavity are smaller in amplitude than either before of after the common cavity events, which would also support our theory of the effects of longitudinal muscle contraction on the compliance of the esophagus. We cannot be sure as to which mechanism is the cause of common cavity pressure, but our data strongly support that the onset of common cavity pressure seen in association with GER is not due to the entry of refluxate into the esophagus. To be technically correct, the term common cavity implies that the esophagus and stomach are one cavity with the same pressures. Our data suggest that the term common cavity pressure, as is being used in the current literature, is technically incorrect because an increase in intraesophageal pressure in association with GER may occur due to reasons other than the true common cavity.
We do not intend to imply that physical movements of gastric contents into the esophagus (GER) cannot increase esophageal pressure. Our data only suggest that the onset of common cavity pressure waves seen in association with GER, in normal subjects, is not due to physical movement of gastric contents into the esophagus. However, it is possible that in patients with GER disease, in whom volume of reflux may be greater than normal subjects (14), some of the common cavity pressure waves might be related to GER. We propose that the common cavity pressure, observed on pressure recordings, cannot be used as a surrogate marker of GER.
| GRANTS |
|---|
|
|
|---|
| FOOTNOTES |
|---|
The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.
| REFERENCES |
|---|
|
|
|---|
This article has been cited by other articles:
![]() |
I. Dogan, V. Bhargava, J. Liu, and R. K. Mittal Axial stretch: a novel mechanism of the lower esophageal sphincter relaxation Am J Physiol Gastrointest Liver Physiol, January 1, 2007; 292(1): G329 - G334. [Abstract] [Full Text] [PDF] |
||||
| ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| HOME | HELP | FEEDBACK | SUBSCRIPTIONS | ARCHIVE | SEARCH | TABLE OF CONTENTS |
| Visit Other APS Journals Online |