ライフサイエンスコーパス: watt

1 ielding a power efficiency of 1.7 Gflops per Watt.

2 ork (median, range, % change) increased 17.5 watts (-13 to +44 watts, 46%, p < 0.05), maximal oxygen

3 r men and women in Harlem, 4.11 and 3.38; in Watts, 2.92 and 2.60; in central Detroit, 2.79 and 2.58;

4 (0.58 +/- 0.30 versus 0.76 +/- 0.32 L/min), Watts (45 +/- 48 versus 71 +/- 59), V E/MVV (88 +/- 33 v

5 , % change) increased 17.5 watts (-13 to +44 watts, 46%, p < 0.05), maximal oxygen consumption increa

6 wedge pressure, left ventricular dimensions, watts achieved during exercise, heart rate, maximum syst

7 Resting systolic blood pressure, watts achieved, peak VO2, VO2 at the ventilatory thresho

8 s determined by van't Hoff as well as D'Arcy/Watt analyses of the isotherms at 5, 15, and/or 25 degre

9 on further to less than half a US dollar per watt and to minimize the environmental impact.

10 ic capacity and muscle strength (measured in watts and newtons per kilogram of body weight, respectiv

11 trated adequate efficiencies (1 to 15 lumens/watt) and lifetimes (>5000 hours) for practical use; how

12 sma can be formed with very low power (a few watts) and overlapped with the glow discharge.

13 and 275 mW (effectively >6,000 frames/s per Watt), and (iii) can be specified and trained using back

14 approximately 0.80 watt at 80 kelvin to 0.2 watt at 200 kelvin has been demonstrated in a superlatti

15 peak powers ranging from approximately 0.80 watt at 80 kelvin to 0.2 watt at 200 kelvin has been dem

16 piratory (TI) and expiratory (TE) times, and watts at rest and during maximal exercise, before and 3

17 nd a high output power densities of over 2.1 Watt cm(-2) at the temperature difference of 700 K.

18 PFT over the 30 year lifetime of a 1000 mega watt coal fired plant.

19 Mean total energy delivered was 1271 J (2-watt continuous power mode).

20 later using either a surgical blade or a 150-Watt continuous-wave CO2 laser deflected by an x-y galva

21 with photoresponsivity above 0.1 ampere per watt (corresponding to an external quantum efficiency of

22 l pleural surface using 1 min of exposure (5 watts, defocused to 70 W/cm2 power density for both lase

23 Lynne Mofenson and Heather Watts discuss the context and implications of the study

24 ewidth (0.2 +/- 0.1 angstrom), high-power (3 watts) emission that could be varied in different device

25 ted using van't Hoff analyses and the D'Arcy/Watt equation.

26 Watts et al. introduced a metric of landscape pattern ca

27 rive from fossil fuels (approximately 10(13) watts), even with improvements in energy efficiency.

28 Ergometer work increased 20 Watt every 2 min; expiratory threshold loading (4 cm H2O

29 tiative has set cost-reduction targets of $1/watt for central-station solar technologies.

30 Patients exercised at 53.7 +/- 4.1 watts for 10.4 +/- 1.4 min.

31 Power was delivered at 30 watts for 60 seconds, when either catheter/tissue contac

32 the same trend reported by Millner-White and Watts for the effectiveness of various monovalent anions

33 um are analyzed with the Kohlrausch-Williams-Watts formalism, the exponent beta decreases with increa

34 was calculated using the Kohlrausch-Williams-Watts function and found to be 0.39.

35 tance of 200 F/g, a specific energy of 30-47 Watt-hour/kilogram (Wh/kg), a specific power of 200,000

36 citors and can store a specific energy of 41 watt-hours per kilogram (19.5 watt-hours per liter).

37 c energy of 41 watt-hours per kilogram (19.5 watt-hours per liter).

38 4 beats per minute), W(peak) (1.6 versus 2.7 watts/kg), AT (11.1 versus 18.0 ml O(2)/kg/minute) and W

39 ml O(2)/kg/minute) and W(AT) (0.6 versus 1.4 watts/kg), compared to controls (P <or= 0.05 for each).

40 omega, T), and a general Kohlrausch-Williams-Watts (KWW) form for time-domain relaxation.

41 functions as well as the Kohlrausch-Williams-Watts (KWW) stretched exponential model.

42 -infrared (mid-IR) spectral range, achieving watt-level continuous wave operation in a compact packag

43 re well described by the Kohlrausch-Williams-Watts model, from which a characteristic rate constant,

44 was quantified with the Kohlrausch-Williams-Watts model.

45 onducting glasses could reduce the price per watt of perovskite photovoltaic modules.

46 bias fields, and for low-input power (micro-Watts or lower).

47 during normal walking [generating up to 7.4 watts, or a 300-fold increase over previous shoe devices

48 49% (median increase 17 watts, range 6 to 44 watts, p < 0.05) and maximal minute ventilation (VEmax)

49 A key goal is to achieve operation at sub-watt peak power levels and on sub-picosecond timescales.

50 e is estimated to be no more than about -0.3 watt per square meter (cooling), compared with +2.45 wat

51 aerosol climate forcings of as much as -0.8 watt per square meter cooling and +0.3 watt per square m

52 n for climate sensitivity and -0.30 to -0.95 watt per square meter for the net aerosol forcing.

53 nal negative radiative forcing of about -0.1 watt per square meter from 1960 to 1990.

54 (5)CF(3) to have a radiative forcing of 0.57 watt per square meter per parts per billion.

55 -0.8 watt per square meter cooling and +0.3 watt per square meter warming.

56 rosol changes over this period of about -0.1 watt per square meter, reducing the recent global warmin

57 to endogenic heat fluxes locally reaching 1 watt per square meter.

58 ray laser, high-intensity radiation (>10(17) watts per cm(2), previously the domain of optical lasers

59 ice produced a specific cooling power of 2.8 watts per gram and a COP of 13.

60 discharge/regeneration power of 1,061/1,425 watts per kilogram at a 50 per cent state of charge and

61 Stretching coiled yarns generated 250 watts per kilogram of peak electrical power when cycled

62 ernating W and Se layers is as small as 0.05 watts per meter per degree kelvin at room temperature, 3

63 ioxide support is still as high as about 600 watts per meter per kelvin near room temperature, exceed

64 (kappa) of suspended graphene, 3000 to 5000 watts per meter per kelvin, exceeds that of diamond and

65 an enhanced thermal conductivity up to 1290 watts per meter per kelvin.

66 a thermal conductivity of approximately 0.6 watts per meter per kelvin.

67 impact, as expressed by radiative forcing in watts per meter squared, of individual chemical species.

68 245T2/10(7)) - (3.407T3/10(11)), in units of watts per meter-kelvin, if Fe2+ is present.

69 the low end of previous estimates, at 18-44 watts per metre per kelvin.

70 ed extremely high power densities of about 2 watts per square centimeter at 650 degrees C along with

71 tailored intense laser fields (about 10(13) watts per square centimeter) can dynamically Stark shift

72 ielding stable power densities of 0.3 to 0.6 watts per square centimeter.

73 for example, at 900 degrees C they deliver 2 watts per square centimetre of power in humidified hydro

74 intense (with intensities approaching 10(20) watts per square centimetre), hard (with photon energies

75 mely high peak intensities (exceeding 10(20) watts per square centimetre).

76 ase in S from 1983 to 2001 at a rate of 0.16 watts per square meter (0.10%) per year; this change is

77 square meter (cooling), compared with +2.45 watts per square meter (warming) due to anthropogenic gr

78 ivities should not exceed 2.5 (range: 1.7-4) watts per square meter (Wm(-2)) of the Earth's surface.

79 urement Missions and is found to average 1.8 watts per square meter between 30 degrees S and 30 degre

80 ke instantaneous forcing of climate from -28 watts per square meter in cloud-free conditions to +8 wa

81 es that Earth is now absorbing 0.85 +/- 0.15 watts per square meter more energy from the Sun than it

82 ive forcing during the first year (34 +/- 31 Watts per square meter of burned area), but to decrease

83 imum power density using acetate reached 5.6 watts per square meter of cathode surface area, which wa

84 square meter in cloud-free conditions to +8 watts per square meter once the reduction of cloud cover

85 eased atmospheric heating locally by about 3 watts per square meter per decade (similar in magnitude

86 ck had a magnitude of 0.54 +/- 0.74 (2sigma) watts per square meter per kelvin, meaning that it is li

87 d to increase with SST at a rate of 13 to 15 watts per square meter per kelvin.

88 ls that the model underestimates by 25 to 30 watts per square meter the amount of solar energy absorb

89 ows a noontime radiative cooling power of 93 watts per square meter under direct sunshine.

90 without the dialysis stack, and 3.0 +/- 0.05 watts per square meter with domestic wastewater.

91 ged over an 80-year fire cycle (-2.3 +/- 2.2 Watts per square meter) because multidecadal increases i

92 equire local surface heat flux changes (+/-4 watts per square meter) much larger than the basinwide a

93 ve flux at the top of the atmosphere was -15 watts per square meter, comparable to the aerosol indire

94 reflected sunlight decreased by less than 2 watts per square meter, in the tropics over the period 1

95 ly summer from BC in Arctic snow was about 3 watts per square meter, which is eight times the typical

96 alent to a radiative forcing of -0.5 +/- 0.4 watts per square meter, which suggests that reaching low

97 d by Earth to space increased by more than 5 watts per square meter, while reflected sunlight decreas

98 eat across the ocean surface of 0.4 +/- 0.05 watts per square meter.

99 temperature, and has a cooling power of 40.1 watts per square metre at ambient air temperature.

100 global-mean radiative forcing of around -0.2 watts per square metre for September to October 2014.

101 this leads to an increase of an average 3.4 watts per square metre in the surface longwave fluxes.

102 hen exposed to direct sunlight exceeding 850 watts per square metre on a rooftop, the photonic radiat

103 ncreased a median of 49% (median increase 17 watts, range 6 to 44 watts, p < 0.05) and maximal minute

104 eLife deputy editor Fiona M Watt recounts some of her personal experiences as a seni

105 three-photon input was used to manipulate a Watt-scale beam at a speed exceeding 500 gigahertz.

106 hmic increasing intensities from 13.5 to 214 Watt seconds (Ws).

107 The average power is nearly 20 watts, several orders of magnitude higher than any exist

108 evention Trial (BCPT) Symptom Checklist; the Watts Sexual Functioning Questionnaire (WSFQ); and subsc

109 the reconstructed neutron spectra resembled Watt spectra, which gave confidence that the interrogate

110 We use three network models, Erdos-Renyi, Watts-Strogatz and structured nodes, to generate network

111 However, the Watts-Strogatz model reproduces very well the topologica

112 e biologically appealing modification of the Watts-Strogatz model to describe residue networks is pro

113 scale-free, and is best approximated by the Watts-Strogatz model, which generates "small-world" netw

114 , and these patterns are consistent with the Watts-Strogatz model.

115 0 kg) and consumed less energy (300 vs. 1000 watts) than that for PV-CPR.

116 We show that approximately 10(12) watts--that is, 1 TW, representing 25-30% of the total d

117 In 1961, Crick, Barnett, Brenner, and Watts-Tobin designed an elegant experimental strategy to

118 We were able to transfer 60 watts with approximately 40% efficiency over distances i

119 wer at 6 months than at baseline, both at 20 watts workload (mean 32 mm Hg [SD 8] at baseline vs 29 m