ライフサイエンスコーパス: milliampere

1 nations of four kilovolt (80-140 kV) and six milliampere (200-300 mA) levels.

2 estry, smoking status, pack-years, CT model, milliamperes, and total lung volume.Measurements and Mai

3 The addition of 1 milliampere contralesional motor cortex transcranial dir

4 o light emitting diode displays, in terms of milliampere driving current, and large ON/OFF current ra

5 er a wide injection current range (65 to 300 milliamperes), exhibiting a side-mode suppression ratio

6 es, while existing cathodes achieve only ~50 milliampere hour per gram and ~100 cycles.

7 cathode delivers a specific capacity of 200 milliampere hour per gram over 665 discharge/charge cycl

8 eter (mW/cm(2))] and high areal capacity [25 milliampere hour per square centimeter (mA.hour/cm(2))].

9 , even at quite high areal capacity (6 to 20 milliampere hour per square centimeter).

10 material, achieving a high capacity of 148.2 milliampere hours per gram at 0.2 C over 100 cycles with

11 atteries, which affords a capability of 72.5 milliampere hours per gram at an ultrahigh rate of 200 a

12 LiFePO(4)-shows a high capacity of about 164 milliampere hours per gram of LiFePO(4), and almost no d

13 ter (mA/cm(2)), capacities between 20 and 82 milliampere hours per square centimeter (mA.hour/cm(2))

14 ng at 1 milliampere per square centimeter [6 milliampere hours per square centimeter (mA.hour/cm(2))]

15 cells with areal capacities of more than 2.5 milliampere hours per square centimetre retain 75 per ce

16 composite electrodes with a capacity of 243 milliampere-hours per gram (for the total weight of the

17 The LNO@NMC811 cathode retains 116 milliampere-hours per gram after 200 cycles, showing exc

18 hium intercalation capacities (less than 200 milliampere-hours per gram) of typical transition-metal-

19 des offer high theoretical capacities (3,860 milliampere-hours per gram)(1), but rechargeable batteri

20 ~ 11 ampere-hours per liter) and areal (108 milliampere-hours per square centimeter) energy density,

21 nic electrochemical transistor, resulting in milliampere-level signals.

22 ments increased with increasing kilovolt and milliampere levels for all stone types.

23 specific and mass activities that reach 7.8 milliampere (mA) per centimeter squared and 4.3 ampere p

24 the brain, is presently fixed at 800 or 900 milliamperes (mA) without clinical or scientific rationa

25 r pitch-normalized current density-above 0.9 milliampere per micrometer at a low supply voltage of 0.

26 nt range of 6 picoampere per millimeter to 5 milliampere per millimeter.

27 ZWP interphases show >2000-hour cycling at 1 milliampere per square centimeter [6 milliampere hours p

28 ty with the best T(50) of 267 minutes at 1.0 milliampere per square centimeter was also achieved.

29 In electrodialysis at 5 milliampere per square centimeter, the resulting membran

30 ammonia is produced at 1.2 volts (V) under 2 milliamperes per centimeter squared (mA cm(-2)) of appli

31 of 197 millivolt in acidic electrolyte at 10 milliamperes per geometric square centimeter (mA cm(geo)

32 ecord-high ON-state current density of ~2.30 milliamperes per micrometer.

33 drain bias with an on-state current of 1.23 milliamperes per micrometre, an on/off ratio over 10(8)

34 At 5 milliamperes per square centimeter (mA/cm(2)), capacitie

35 a low overpotential of 353 millivolts at 10 milliamperes per square centimeter and a low degradation

36 n 100 hours at photocurrent densities of >30 milliamperes per square centimeter and ~100% Faradaic ef

37 anode demonstrated a current density of 2000 milliamperes per square centimeter at 2.47 volts (Nafion

38 at 2.47 volts (Nafion 115 membrane) or 4000 milliamperes per square centimeter at 3.00 volts (Nafion

39 66 +/- 5% toward propylene epoxidation at 50 milliamperes per square centimeter at ambient temperatur

40 r gram of Pt and a specific activity of 11.5 milliamperes per square centimeter for ORR (at 0.9 volts

41 verpotential (191 millivolts) reported at 10 milliamperes per square centimeter in alkaline electroly

42 This catalyst achieves 10 milliamperes per square centimeter in an acidic oxygen e

43 Electron emission of 10 milliamperes per square centimeter was observed at appli

44 e nanoflakes show a current density of 18.95 milliamperes per square centimeter, CO faradaic efficien

45 Cs deliver a maximum current density of 3.85 milliamperes per square centimeter, power density of 0.6

46 iting photocurrent densities of 14.3 and 3.4 milliamperes per square centimeter, respectively, for wa

47 pure H(2)O(2) at current densities up to 200 milliamperes per square centimeter, which represents an

48 high CO partial current densities up to 300 milliamperes per square centimeter.

49 Cu) is achieved at a current density of 400 milliamperes per square centimetre (at 1.5 volts versus

50 nd a partial current density greater than 10 milliamperes per square centimetre at -0.94 volts with r

51 per cent at a partial current density of 230 milliamperes per square centimetre in a liquid-electroly

52 0 per cent at a partial current density of 7 milliamperes per square centimetre in the best catalyst

53 efficiency of more than 99.9 per cent at 40 milliamperes per square centimetre with no apparent deca

54 At charge-discharge current densities of 275 milliamperes per square centimetre, the cells cycled at

55 rsion efficiency of 55 +/- 2 per cent at 150 milliamperes per square centimetre.

56 harged at current densities as high as 1,000 milliamperes per square centimetre.

57 ity injected into human skin is around 79.58 milliamperes per square meter, far below the safety thre

58 w = (0.162 mGy/mA +/- 0.002) x tube current (milliampere) (r2 = 0.999).

59 w = (0.391 mGy/mA +/- 0.004) x tube current (milliampere) (r2 = 0.999); in body mode, CTDI100w = (0.1

60 as performed with six CT scanners at various milliampere second and kilovolt peak settings.

61 h calcified cylinders was scanned at various milliampere second settings (20-160 mAs).

62 0, and 15 cm in diameter, respectively, when milliampere second values of 0.557, 0.196, and 0.054 of

63 13 cm, respectively, can involve the use of milliampere second values of 0.572 and 0.366 of those us

64 Kilovolt peak and milliampere second values were analyzed for phototimed e

65 lues of 0.557, 0.196, and 0.054 of the adult milliampere second values were used.

66 ses, 5-mm collimation, 120-140 kVp, variable milliampere-second settings) performed in 2872 patients

67 energy (120 kVp) and (b) the total reference milliampere seconds (ie, 110 mAs) split up in a way that

68 ickness) was the benchmark for assessing the milliampere seconds and corresponding radiation dose nec

69 reducing milliampere seconds or by reducing milliampere seconds and increasing the kilovolt peak, wh

70 ted radiographs were obtained after reducing milliampere seconds or by reducing milliampere seconds a

71 Tube current-time products (in milliampere seconds) at various noise indexes were compa

72 ter fit, and pediatric CT technique factors (milliampere seconds) necessary to maintain the contrast-

73 spectrum and an increase in tube output (ie, milliampere seconds) of about 50%, a chest radiograph ca

74 unction of kilovolt peak and tube output (in milliampere seconds), contrast resolution assessed in te

75 lts, and the mean quantity of x radiation in milliampere-seconds increased from 220 mAs for children

76 ickness (2, 4, 8 mm), pitch (1.0, 1.5, 2.0), milliampere setting (100, 175, 250 mA), and overlap of r

77 The milliampere setting had only a minor effect on image qua

78 uli at CT increases with higher kilovolt and milliampere settings, with higher kilovolts being partic

79 lovolt settings and up to 1.08-fold at lower milliampere settings.

80 By using a low-milliampere technique and the quick-check method, CT flu

81 The mean milliampere value was 13.2 mA (range, 10--50 mA).

82 d and included site, depth, target diameter, milliampere value, kilovolt peak, fluoroscopic time, and

83 Current (milliampere) was increased stepwise during non-REM sleep