| Literature DB >> 30950761 |
Catriona M Steele1,2, Melanie Peladeau-Pigeon1, Carly A E Barbon1,2, Brittany T Guida1, Melanie S Tapson1,2, Teresa J Valenzano1,2, Ashley A Waito1,2, Talia S Wolkin1, Ben Hanson3, Jane Jun-Xin Ong4, Lisa M Duizer4.
Abstract
Purpose During swallowing, the tongue generates the primary propulsive forces that transport material through the oral cavity toward the pharynx. Previous literature suggests that higher tongue pressure amplitudes are generated for extremely thick liquids compared with thin liquids. The purpose of this study was to collect detailed information about the modulation of tongue pressure amplitude and timing across the range from thin to moderately thick liquids. Method Tongue pressure patterns were measured in 38 healthy adults (aged under 60 years) during swallowing with 4 levels of progressively thicker liquid consistency (International Dysphagia Diet Standardisation Initiative, Levels 0 = thin, 1 = slightly thick, 2 = mildly thick, and 3 = moderately thick). Stimuli with matching gravity flow (measured using the International Dysphagia Diet Standardisation Initiative Flow Test; Cichero et al., 2017 ; Hanson, 2016 ) were prepared both with/without barium (20% weight per volume concentration) and thickened with starch and xanthan gum thickeners. Results After controlling for variations in sip volume, thicker liquids were found to elicit significantly higher amplitudes of peak tongue pressure and a pattern of higher (i.e., steeper) pressure rise and decay slopes (change in pressure per unit time). Explorations across stimuli with similar flow but prepared with different thickeners and with/without barium revealed very few differences in tongue pressure, with the exception of significantly higher pressure amplitudes and rise slopes for nonbarium, starch-thickened slightly and mildly thick liquids. Conclusions There was no evidence that the addition of barium led to systematic differences in tongue pressure parameters across liquids with closely matched gravity flow. Additionally, no significant differences in tongue pressure parameters were found across thickening agents. Supplemental Material https://doi.org/10.23641/asha.7616537.Entities:
Year: 2019 PMID: 30950761 PMCID: PMC6437699 DOI: 10.1044/2018_JSLHR-S-18-0229
Source DB: PubMed Journal: J Speech Lang Hear Res ISSN: 1092-4388 Impact factor: 2.297
Flow characteristics of the stimuli used in the study.
| IDDSI level | Barium | Thickener type | Thickener amount (g/100 ml) | Flow test residual fluid (ml) | Viscosity at 50/s (mPa·s) | Density (g/ml) |
|---|---|---|---|---|---|---|
| 0 = TN0 | Nonbarium | None | None | 0.0 | 1 | 1.00 |
| Barium | None | None | 0.0 | 3 | 1.16 | |
| 1 = ST1 | Nonbarium | Starch | 4.15 | 1.9 | 75 | 1.01 |
| Nonbarium | Xanthan gum | 0.65 | 1.9 | 48 | 1.00 | |
| Barium | Starch | 2.85 | 1.8 | 120 | 1.16 | |
| Barium | Xanthan gum | 0.40 | 1.7 | 51 | 1.17 | |
| 2 = MT2 | Nonbarium | Starch | 4.77 | 5.0 | 141 | 1.02 |
| Nonbarium | Xanthan gum | 1.10 | 5.2 | 128 | 1.02 | |
| Barium | Starch | 3.75 | 4.9 | 273 | 1.17 | |
| Barium | Xanthan gum | 0.90 | 5.3 | 157 | 1.15 | |
| 3 = MO3 | Nonbarium | Starch | 5.85 | 9.4 | 338 | 1.03 |
| Nonbarium | Xanthan gum | 2.10 | 9.1 | 290 | 1.02 | |
| Barium | Starch | 5.10 | 9.5 | 850 | 1.17 | |
| Barium | Xanthan gum | 2.20 | 9.6 | 361 | 1.16 |
Note. IDDSI = International Dysphagia Diet Standardisation Initiative; TN0 = thin; ST1 = slightly thick; MT2 = mildly thick; MO3 = moderately thick.
Results represent mean values across three repeated tests per stimulus at 25 °C. Additional details regarding the testing methods and results can be found in Ong et al. (2018).
Figure 1.Illustration of tongue pressure waveforms and parameter derivation.
In this schematic illustration, time-synchronized pressure waveforms for anterior and posterior tongue–palate pressure are displayed. For the current study, peak pressure was defined as the highest pressure amplitude obtained across both signals. The pressure rise phase was defined as the interval between the earliest pressure onset (Onset 1) and the earliest pressure peak (Peak 1). Pressure rise slope was calculated as the difference in pressure amplitude between these two events, divided by the duration of the rise phase. Pressure decay slope was derived similarly as the difference in pressure amplitude between the terminal pressure peak (Peak 2) and the terminal pressure offset (Offset 2), divided by the duration of the decay phase.
Figure 2.Means and 95% confidence interval boundaries for sip volume by stimulus. Significantly smaller sip volumes (p < .05) were seen for thicker liquids. TN0 = thin; ST1 = slightly thick; MT2 = mildly thick; MO3 = moderately thick; Ba = barium.
Figure 3.Means and 95% confidence interval boundaries for peak pressure amplitude by liquid flow level (within array). Significant increases in peak tongue pressure amplitude (p < .017) were seen for thicker liquids. Additional details regarding pairwise comparisons can be found in Table 2. TN0 = thin; ST1 = slightly thick; MT2 = mildly thick; MO3 = moderately thick; Ba = barium.
Figure 4.Means and 95% confidence interval boundaries for pressure rise slope by liquid flow level (within array). An overall pattern of increased pressure rise slope (p < .017) was seen for thicker liquids. Details regarding pairwise comparisons can be found in Table 2. TN0 = thin; ST1 = slightly thick; MT2 = mildly thick; MO3 = moderately thick; Ba = barium.
Figure 5.Means and 95% confidence interval boundaries for pressure decay slope by liquid flow level (within array). An overall pattern of increased pressure decay slope (p < .017) was seen for thicker liquids. Details regarding pairwise comparisons can be found in Table 2. TN0 = thin; ST1 = slightly thick; MT2 = mildly thick; MO3 = moderately thick; Ba = barium.
Summary of results for the within-array repeated-measures analyses of variance (ANOVAs).
| Parameter | Array | ANOVA result | Pairwise comparisons | Cohen's |
|---|---|---|---|---|
| Log peak tongue pressure per ml (mmHg) | 1 (Non–barium starch) |
| Level 0 < (1, 2, & 3); Level (1 & 2) < 3 | 0.33 (small) to 0.71 (medium) |
| 2 (Non–barium xanthan) |
| Level 0 < 1 & 3; Level 2 < 3 | 0.39 (small) to 0.77 (medium) | |
| 3 (Barium starch) |
| Levels 0, 1, & 2 < 3 | 0.55 (small) to 0.99 (large) | |
| 4 (Barium xanthan) |
| Levels 0, 1, & 2 < 3 | 0.59 (small) to 0.96 (large) | |
| Log rise slope per ml (mmHg/s) | 1 (Non–barium starch) |
| Level 0 < 1, 2, & 3 | 2.0 (large) |
| 2 (Non–barium xanthan) |
| Level 2 < 3 | 0.52 (medium) | |
| 3 (Barium starch) |
| Levels 0, 1, & 2 < 3 | 0.41 (small) to 1.0 (large) | |
| 4 (Barium xanthan) | n.s. | Trend of higher slopes with thicker consistencies | ||
| Log decay slope per ml (mmHg/s) | 1 (Non–barium starch) | n.s. | Trend of higher slopes with thicker consistencies | |
| 2 (Non–barium xanthan) |
| Level 2 < 3 | 0.63 (medium) | |
| 3 (Barium starch) | n.s. | Trend of higher slopes with thicker consistencies | ||
| 4 (Barium xanthan) |
| Level 2 < 3 | 0.45 (small) |
Note. n.s. = not significnant.
Figure 6.Means and 95% confidence interval boundaries for peak pressure amplitude by liquid flow level (across arrays). When peak pressures were compared across the different stimulus arrays within IDDSI flow levels, few differences were seen across stimuli that were closely matched for gravity flow. In the slightly thick (*a) and mildly thick (*b) categories, significantly higher (p < .17) peak pressure amplitudes were seen for the nonbarium, starch-thickened stimuli. TN0 = thin; ST1 = slightly thick; MT2 = mildly thick; MO3 = moderately thick; Ba = barium.