| Literature DB >> 30539131 |
Masatoshi Nakamura1, Ryo Hirabayashi1, Shuhei Ohya2, Takafumi Aoki2, Daichi Suzuki2, Mitsuki Shimamoto2, Takanori Kikumoto3, Wataru Ito3, Emi Nakamura1, Tomoya Takabayashi1, Mtsuaki Edama2.
Abstract
This study aimed to clarify the acute effect of static stretching (SS) with superficial cooling on dorsiflexion range of motion (DF ROM) and muscle stiffness. Sixteen healthy males participated in the cooling condition and a control condition in a random order. The DF ROM and the shear elastic modulus of medial gastrocnemius (MG) in the dominant leg were measured during passive dorsiflexion. All measurements were performed prior to (PRE) and immediately after 20 min of cooling or rested for 20 min (POST), followed by 2 min SS (POST SS). In cooling condition, DF ROM at POST and POST SS were significantly higher than that at PRE and DF ROM at POST SS was significantly higher than that at POST. In addition, the shear elastic modulus at POST was significantly higher than that at PRE and the shear elastic modulus at POST SS was significantly lower than those at PRE and POST. However, there were no significant differences in the percentage changes between PRE and POST SS between the cooling and control conditions. Our results showed that effects of SS with superficial cooling on increases in ROM and decrease in muscle stiffness were no more beneficial than those of SS alone.Entities:
Keywords: range of motion; shear elastic modulus; stretch tolerance; superficial cooling
Year: 2018 PMID: 30539131 PMCID: PMC6259457 DOI: 10.1055/a-0684-9375
Source DB: PubMed Journal: Sports Med Int Open ISSN: 2367-1890
Fig. 1Experimental protocol of this study. SS: static stretching
Fig. 2Typical example of measurement of shear elastic modulus by ultrasonic shear wave elastographic imaging. The quadrangular region of interest (ROI) within the color-coded area of the elastographic images was set, and the average value of Young’s modulus in the quadrangular ROI was automatically calculated. In addition, the shear elastic modulus was calculated by dividing the obtained Young’s modulus by three.
Table 1 Changes in DF ROM, passive torque at DF ROM, and shear elastic modulus of MG.
| Cooling condition | Control condition | Interaction effect | ||||||
|---|---|---|---|---|---|---|---|---|
| PRE | POST | POST SS | PRE | POST | POST SS | p value | partial η 2 | |
| DF ROM (degree) | 36.2±4.8 | 40.4±5.1 ** | 43.0±6.2** ## | 37.0±4.2 | 36.6±3.9 | 41.8±4.7** ## | P<0.01 | 0.506 |
| Passive torque at DF ROM (Nm) | 24.5±4.7 | 30.1±7.4** | 32.1±8.9** | 24.8±4.3 | 23.4±4.6 | 29.4±7.7** ## | P<0.01 | 0.409 |
| Shear elastic modulus of MG (kPa) | 15.9±7.2 | 21.3±8.3* | 10.1±5.5** ## | 17.0±9.5 | 18.0±9.8 | 11.1±5.6** ## | P=0.014 | 0.247 |
*: P<0.05, ** : P<0.01; significant difference between PRE and POST; ##: P<0.01; significant difference between POST and POST SS; SS=static stretching; ROM=range of motion; MG=medial gastrocnemius
Table 2 Comparison of the percent changes between cooling condition and control condition.
| The percent change between PRE and POST SS (%) | Cooling condition | Control condition | P value |
|---|---|---|---|
| DF ROM | 18.9±6.9 | 13.3±10.0 | P=0.077 |
| passive torque at DF ROM | 30.3±21.8 | 18.4±18.4 | P=0.152 |
| shear elastic modulus of MG | -35.5±17.5 | -29.1±26.4 | P=0.391 |
SS; static stretching, ROM; range of motion, MG; medial gastrocnemius