| Literature DB >> 29368184 |
Ollie Jay1,2, Nathan B Morris3.
Abstract
Cold water or ice slurry ingestion during exercise seems to be an effective and practical means to improve endurance exercise performance in the heat. However, transient reductions in sweating appear to decrease the potential for evaporative heat loss from the skin by a magnitude that at least negates the additional internal heat loss as a cold ingested fluid warms up to equilibrate with body temperature; thus explaining equivalent core temperatures during exercise at a fixed heat production irrespective of the ingested fluid temperature. Internal heat transfer with cold fluid/ice is always 100% efficient; therefore, when a decrement occurs in the efficiency that sweat evaporates from the skin surface (i.e. sweating efficiency), a net cooling effect should begin to develop. Using established relationships between activity, climate and sweating efficiency, the boundary conditions beyond which cold ingested fluids are beneficial in terms of increasing net heat loss can be calculated. These conditions are warmer and more humid for cycling relative to running by virtue of the greater skin surface airflow, which promotes evaporation, for a given metabolic heat production and thus sweat rate. Within these boundary conditions, athletes should ingest fluids at the temperature they find most palatable, which likely varies from athlete to athlete, and therefore best maintain hydration status. The cooling benefits of cold fluid/ice ingestion during exercise are likely disproportionately greater for athletes with physiological disruptions to sweating, such as those with a spinal cord injury or burn injuries, as their capacity for skin surface evaporative heat loss is much lower; however, more research examining these groups is needed.Entities:
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Year: 2018 PMID: 29368184 PMCID: PMC5790850 DOI: 10.1007/s40279-017-0842-8
Source DB: PubMed Journal: Sports Med ISSN: 0112-1642 Impact factor: 11.136
Fig. 1Changes in dry heat loss [DHL = conduction (K) + convection (C) + radiation (R)] and the required evaporation (EVAP) to achieve a total heat loss (total HL) of 700 W with increasing air temperature under still [air velocity (v): 0.5 m·s−1] and windy (v: 5.0 m·s−1) conditions and no solar load (a). Parallel whole-body sweat rates required to achieve the levels of EVAP depicted in (a) are shown in (b) for dry [relative humidity (RH) 25%] and humid (RH 60%) conditions
Fig. 2Determinants of body heat storage with cold fluid ingestion during exercise
Studies reporting sweat losses and core temperature (TC) responses during steady-state (fixed-intensity) exercise over a fixed time with ingestion of at least two water temperatures, or one water temperature compared with ice slurry ingestion
| References, year |
| RH (%) | End-trial | Volume (mL) | Sweat loss (g) | ||||
|---|---|---|---|---|---|---|---|---|---|
| Gisolfi and Copping, 1974 [ | 6 | 33.5 | 36 | 10, 38 | 39.2, 39.4 | 1200 | 147, 1 | 3124, 3154 | 7591, 7664 |
| Wimer et al., 1997 [ | 7 | 26 | 40 | 0.5, 19, 38 | 38.0, 38.0, 38.1 | 1353 | 212, 108, 1 | 471, 551, 649 | 1144, 1339, 1571 |
| Lee and Shirreffs, 2007 [ | 9 | 25.4 | 61 | 10, 37, 50 | 38.2, 38.2, 38.3 | 1000 | 118, 5, − 49 | 1230, 1260, 1320 | 2989, 3062, 3208 |
| Lee et al., 2008 [ | 8 | 25 | 60 | 10, 37, 50 | 38.1, 38.1, 38.2 | 1200 | 141, 6, − 59 | 1090, 1230, 1350 | 2649, 2989, 3281 |
| Bain et al., 2012 [ | 9 | 23.6 | 23 | 1.5, 10, 37, 50 | 38.0, 37.9, 38.0, 38.1 | 1030 | 141, 104, 3, − 49 | 465, 488, 531, 575 | 1129, 1184, 1288, 1396 |
| Morris et al., 2014 [ | 8 | 23.7 | 32 | 1.5, 50 | 37.4, 37.4 | 705 | 106, − 37 | 630, 745 | 1530, 1810 |
| Lamarche et al., 2015 [ | 10 | 25.9 | 25 | 1.5, 50 | 38.0, 37.9 | 1014 | 150, − 54 | 560, 634 | 1358, 1538 |
| Burdon et al., 2013 [ | 10 | 32.1 | 40 | Ice, 37 | 38.2, 38.3 | 1560 | 600, 8 | 500, 600 | 1215, 1458 |
| Hailes et al., 2016 [ | 12 | 35.5 | 50 | Ice, 35.5 | 38.1, 38.2 | 1330, 2660 | 511, 30 | 2517, 2703 | 6116, 6568 |
| Morris et al., 2016 [ | 9 | 33.5 | 24 | Ice, 37 | 37.7, 37.7 | 729 | 201, 1 | 568, 720 | 1829, 2211 |
RH relative humidity, T ambient temperature
aInternal heat transfer (Hfluid) calculated using fluid volume, the specific heat capacity of water (4.186 J·g−1·°C−1), the enthalpy of fusion of ice (334 J/g) if required and the difference between fluid temperature (Tfluid) and TC
bEvaporative potential from the skin (E) calculated using sweat loss, the latent heat of vaporisation of sweat (2430 J/g) and assuming 100% evaporation
Fig. 3Association between changes in evaporative potential from the skin surface with changes in internal heat loss with ingested fluid/ice. Dotted line indicates line of identity. A best fit line is provided for water ingestion trials only
Fig. 4Association between the differences in end-trial core temperature relative to control fluid conditions within each study with net differences between internal heat loss and evaporative potential with ingested fluid/ice. A best-fit line is provided for water ingestion trials only
Fig. 5Estimated environmental boundary conditions at which cold water and ice slurry ingestion provides a net cooling effect for running at 10, 14 and 18 km/h (a) and cycling on a flat surface at an external power of 180, 240 and 300 W (b). Rates of metabolic heat production at different running speeds and cycling power outputs were estimated using standard American College of Sports Medicine equations [79]. Maximum skin wettedness at high air speeds was equal to 0.30 [80]. Boundaries were estimated assuming equivalent reductions in the evaporative heat loss potential from the skin with increases in internal heat loss with cold water/ice ingestion
Aggregate of studies using cold water or ice ingestion as a pre-cooling intervention prior to an exercise performance trial
| References, year |
| RH (%) | End-trial | Δ | Volume (mL) | Sweat rate (g·h−1) | ||||
|---|---|---|---|---|---|---|---|---|---|---|
| Lee et al., 2008 [ | 8 | 35 | 60 | 4, 37 | 36.9, 36.9 | 36.4, 36.8 | 39.5, 39.5 | 0.049, 0.052 | 300 | 1220, 1400 |
| Byrne et al., 2011 [ | 7 | 32 | 60 | 2, 37 | 37.3, 37.3 | 36.9, 37.1 | 38.2, 38.6 | 0.043, 0.050 | 900 | 770, 980 |
| Siegel et al., 2010 [ | 10 | 34 | 55 | Ice, 4 | 37.2, 37.1 | 36.5, 36.8 | 39.4, 39.1 | 0.058, 0.057 | 599 | 1890, 2050 |
| Siegel et al., 2012 [ | 8 | 34 | 52 | Ice, 37 | 37.1, 37.1 | 36.7, 37.1 | 39.8, 39.5 | 0.059, 0.051 | 586 | 2060, 2280 |
| Yeo et al., 2012 [ | 12 | 28 | 75 | Ice, 31 | 37.5, 37.4 | 37.0, 37.3 | 40.2, 39.8 | 0.071, 0.055 | 511 | 1130, 1110 |
| Naito and Ogaki, 2015 [ | 9 | 35 | 30 | Ice, 4 | 37.1, 37.2 | 36.8, 37.1 | 38.9, 38.9 | 0.042, 0.043 | 768 | 1800, 1700 |
| Gerrett et al., 2016 [ | 12 | 31 | 41 | Ice, 23 | 37.3, 37.3 | 36.7, 37.3 | 38.5, 38.9 | 0.058, 0.052 | 551 | 500, 510 |
| Stevens et al., 2016 [ | 11 | 33 | 46 | Ice, 22 | 37.2, 37.2 | 36.9, 37.2 | 39.0, 39.1 | 0.080, 0.073 | 548 | NA |
| Naito et al., 2017 [ | 7 | 35 | 30 | Ice, 4 | 37.1, 37.1, 37.1 | 36.6, 36.7, 37.0 | 38.8, 38.7, 38.6 | 0.048, 0.052, 0.050 | 530 | 820, 1200, 720 |
NA not applicable, RH relative humidity, T ambient temperature, T core temperature, T fluid temperature