Animals
Five recently weaned hooded seal pups were captured on the pack ice of the Greenland Sea in late March 2014. The animals were kept on board RV “Helmer Hanssen” and brought to the approved animal research facility of the Department of Arctic and Marine Biology at UiT-The Arctic University of Norway. On board of RV “Helmer Hanssen” the ambient air temperature was around 0 °C and the animals had ad lib access to snow that was provided on a daily basis. Upon arrival at the research facilities, 12 days after capture, the animals were introduced to a 42,000-L seawater pool under continuous water flow until the end of the experiment, 33 days after capture. While four of the five animals seemed healthy throughout the experiment, one of the animals died on the 28th day of the experiment for unknown reasons. The temperature at the research facility was kept around 6 °C and the day length was simulated as at 70°N. The animals went through a period of post-weaning fast and were therefore not fed. All experiments were conducted in accordance with the Norwegian Animal Welfare Act and were approved by the National Animal Research Authority of Norway (approval #6216).
Sample collection
The ingestion of snow and seawater, as well as other water influx rates, total body water and body composition were measured with the tritiated water method. Blood samples were repeatedly collected to measure changes in plasma parameters. Prior to tritiated water injections and blood sampling, the animals were loosely restrained on a specially designed board. A dose of 0.25 mL tiletamine-zolazepam (50 mg mL−1 tiletamine, 50 mg mL−1 zolazepam, Zoletil Forte Vet, Virbac Laboratories, France) was administered intramuscularly to anaesthetize the animal. An incubation time of at least 10 min was permitted for the anaesthesia to immobilize the animal before further handling.
The tritium isotope (Perkin Elmer, Boston, USA) was diluted in physiological saline (0.9% (w.v) sodium chloride, B. Braun Melsungen AG, Melsungen, Germany). 8–9 mL tritiated water (13 µCi mL−1-) was injected on the day of capture into the intravertebral extradural vein through a 16-cm long catheter (Selacon-T™ 16G/1.70 × 160 mm, The Hague, The Netherlands) at the level of the fourth lumbar vertebra. Prior to the injection of tritiated water a blood sample was collected to measure the plasma’s background level of radioactivity. After an equilibration period of 60 and 90 min two other blood samples were collected to calculate total body water. Additional blood samples were collected 3, 5, 12, 19, 26 and 33 days after capture. Tritiated water was reinjected (8–9 mL, 50 µCi mL−1) 12 days after capture, to calculate changes in total body water, body composition, and water influx during snow exposure. A third and final tritiated water injection (8–9 mL, 50 µCi mL−1-) was given 33 days after capture to calculate changes in total body water, body composition and water influx during seawater exposure.
After each blood sampling the animals were weighed with a DHS crane weight (Scaleit, Norway), with a precision of ±0.15%. All blood samples were collected in 10.0 mL vacutainers (BD, LH 170 I.U., Plymouth, UK). The samples were stored on ice and centrifuged for 15 min at 2500-rpm within 2 h after sampling. The plasma was separated from the precipitate and transferred to 2 mL cryovials (VWR, Leuven, Belgium). All plasma samples were frozen in liquid nitrogen and stored at −80 °C until further analyses. About half of the plasma of each sampling moment was used to measure osmolality and urea concentrations. The other half of the plasma was deproteinized using 70% perchloric acid (HClO4 ACS reagent 70%, Sigma–Aldrich, St. Louis, USA). The tritium concentration of the deproteinized plasma sample was determined by standard liquid scintillation techniques using a beta liquid scintillation counter (1900 TR Packard, A Canberra Company, Oslo, Norway). The plasma samples were deproteinized to avoid quenching.
\(r_{{{\mathbf{H}}_{2} {\mathbf{O}}}}\) and r
W calculations and corrections
The concentration of the tritium isotope measured by the scintillation counter was corrected for the water content of the plasma prior to further calculations. Total body water was calculated following Eq. 1 where N is total body water in mL, i.d. the injected dose of the tritium isotope and S.A. the specific activity of the isotope in the body water.
$$N = \frac{{{\text{i}} . {\text{d}} .}}{{{\text{S}} . {\text{A}} .}}.$$
(1)
The natural logarithm of the S.A. of tritium in the plasma was plotted against time (Fig. 1). The inclination of the decay (–K2H*) of the S.A. in the plasma is the fractional turnover rate of the isotope (Eq. 2). \(H_{1}^{*}\) and \(H_{2}^{*}\) are the initial and final specific activities of the tritium isotope in the body water and t is the elapsed time (Nagy and Costa 1980).
$$K_{2H*} = \frac{{{ \ln }(H_{1}^{*} /H_{2}^{*} )}}{\Delta t}.$$
(2)
The daily change in body water (K
N
) was calculated with Eq. 3 where N
0 and N
1 is the initial and final total body water in mL, respectively.
$$K_{N} = \frac{{\ln N_{0} - \ln N_{1} }}{\Delta t}.$$
(3)
It was assumed that total body water decreased exponentially over time since the animals’ body mass decreased exponentially, due to their fast (Ortiz et al. 1978). Equation 16 from Lifson and McClintock (1966) was used to calculate the average daily water efflux rate (\(r_{{{\text{H}}_{ 2} {\text{O}}}}\)) in mL day−1 (Eq. 4). The final estimates for \({\text{r}}_{{{\text{H}}_{2} {\text{O}}}}\) were corrected for exchange and fractionation (Lifson and McClintock 1966; Nagy and Costa 1980).
$$r_{{{\text{H}}_{ 2} {\text{O}}}} = \frac{{N_{0} K_{N} (K_{2H*} - K_{N} )\Delta t}}{{1 - \exp ( - K_{N} \Delta t)}}.$$
(4)
The average daily water influx rate (r
w) in mL day−1 was calculated with Eq. 5, according to Lifson and McClintock (1966) and Ortiz et al. (1978). The total water influx rate can be divided in respiratory water influx (H2Orespiratory), metabolic water (H2Ometabolic) and the ingestion of snow or seawater (H2Osnow/seawater).
$$r_{\text{w}} = |r_{{{\text{H}}_{ 2} {\text{O}}}} | - \frac{\Delta N}{\Delta t}.$$
(5)
H2Orespiratory
The respiratory water influx rates (in mL day−1) were calculated with Eq. 6, according to Folkow and Blix (1987), with a known ambient air temperature and assuming a 100% relative humidity of the air. MW is the mass of evaporated water in mg s−1 kg−0.75, P
W the water vapour pressure in the inhaled air in mmHg, V
L the respiratory minute volume in L min−1 kg−0.75, M the molar mass of water, T
g the gas temperature in °K, R the gas constant (62.63 mmHg L °K−1 mol−1) and t the time constant (60 s min−1).
$$M_{\text{W}} = \frac{{P_{\text{W}} V_{\text{L}} M}}{{T_{\text{g}} R t}}.$$
(6)
The respiratory minute volume (V
L) was calculated following Eq. 7 (Folkow and Blix 1987). Where MR is the metabolic rate based on the caloric equivalent of fat and protein loss. Protein and fat loss are obtained using Eqs. 8 and 9.
$$V_{\text{L}} = 0.042 \cdot {\text{MR}} + 0.119.$$
(7)
H2Ometabolic
Metabolic water (in mL day−1) was calculated as the water derived from fat and protein oxidation. Total body fat (TBF) and total body protein (TBP), as percentages of body mass, were calculated following Eqs. 8 and 9, respectively (Reilly and Fedak 1990). %N is total body water as percentage of total body mass. The metabolic water was subsequently calculated using Eq. 10
$$\% {\text{TBF}} = 105.1 - 1.47 \cdot\% N,$$
(8)
$$\% {\text{TBP}} = 0. 4 2 \cdot \% N - 4. 7 5 ,$$
(9)
$$\begin{aligned} {\text{H}}_{2} {\text{O}}_{{{\text{metabolic }}}} & = 1.071\cdot\left( {{\text{TBF}}_{1} - {\text{TBF}}_{2} } \right) \\ & \quad + 0.396\cdot\left( {{\text{TBP}}_{1} - {\text{TBP}}_{2} } \right). \\ \end{aligned}$$
(10)
H2Osnow/seawater
The water influx rate through the ingestion of snow or seawater (in mL day−1) was calculated as the difference between the total daily water influx rate and the metabolic and respiratory water influx rates:
$${\text{H}}_{ 2} {\text{O}}_{\text{snow/seawater}} = r_{\text{W}} - ({\text{H}}_{ 2} {\text{O}}_{\text{respiratory}} {\text{ + H}}_{ 2} {\text{O}}_{\text{metabolic}} ).$$
(11)
Blood samples
Right after blood sampling an aliquot of blood was used to determine the haematocrit percentage. A capillary vial (Aris, Soda Lime glass 80iu mL−1, Am-Heparinized Vitrex, Herlev, Denmark) was filled with blood and centrifuged for 10 min at 3000 rpm using a microcentrifuge (Hettich-Zentrifugen, Tuttlingen, Germany). The haematocrit percentage was read on the haematocrit scale.
Plasma samples were analysed for urea concentrations and the osmolality. The plasma samples were thawed up over night. Urea concentrations were measured with a Reflotron system (Reflotron, Mannheim Boehringer, Mannheim Germany). The osmolality was determined by freezing-point osmometry (Osmomat030, Gonotec, Berlin, Germany).
Statistics
Total body water, water influx rates and blood parameters obtained throughout the experiment were compared using a paired Student’s t test using SPSS statistics (IBM version 22). Values are given as averages ± standard deviation.