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1 nations of four kilovolt (80-140 kV) and six milliampere (200-300 mA) levels.
2 ments increased with increasing kilovolt and milliampere levels for all stone types.
3  specific and mass activities that reach 7.8 milliampere (mA) per centimeter squared and 4.3 ampere p
4 r pitch-normalized current density-above 0.9 milliampere per micrometer at a low supply voltage of 0.
5 ammonia is produced at 1.2 volts (V) under 2 milliamperes per centimeter squared (mA cm(-2)) of appli
6 n 100 hours at photocurrent densities of >30 milliamperes per square centimeter and ~100% Faradaic ef
7 r gram of Pt and a specific activity of 11.5 milliamperes per square centimeter for ORR (at 0.9 volts
8 verpotential (191 millivolts) reported at 10 milliamperes per square centimeter in alkaline electroly
9                      Electron emission of 10 milliamperes per square centimeter was observed at appli
10 e nanoflakes show a current density of 18.95 milliamperes per square centimeter, CO faradaic efficien
11 iting photocurrent densities of 14.3 and 3.4 milliamperes per square centimeter, respectively, for wa
12 At charge-discharge current densities of 275 milliamperes per square centimetre, the cells cycled at
13 harged at current densities as high as 1,000 milliamperes per square centimetre.
14 w = (0.162 mGy/mA +/- 0.002) x tube current (milliampere) (r2 = 0.999).
15 w = (0.391 mGy/mA +/- 0.004) x tube current (milliampere) (r2 = 0.999); in body mode, CTDI100w = (0.1
16 as performed with six CT scanners at various milliampere second and kilovolt peak settings.
17 h calcified cylinders was scanned at various milliampere second settings (20-160 mAs).
18 0, and 15 cm in diameter, respectively, when milliampere second values of 0.557, 0.196, and 0.054 of
19  13 cm, respectively, can involve the use of milliampere second values of 0.572 and 0.366 of those us
20                            Kilovolt peak and milliampere second values were analyzed for phototimed e
21 lues of 0.557, 0.196, and 0.054 of the adult milliampere second values were used.
22 ses, 5-mm collimation, 120-140 kVp, variable milliampere-second settings) performed in 2872 patients
23 energy (120 kVp) and (b) the total reference milliampere seconds (ie, 110 mAs) split up in a way that
24 ickness) was the benchmark for assessing the milliampere seconds and corresponding radiation dose nec
25  reducing milliampere seconds or by reducing milliampere seconds and increasing the kilovolt peak, wh
26 ted radiographs were obtained after reducing milliampere seconds or by reducing milliampere seconds a
27               Tube current-time products (in milliampere seconds) at various noise indexes were compa
28 ter fit, and pediatric CT technique factors (milliampere seconds) necessary to maintain the contrast-
29 spectrum and an increase in tube output (ie, milliampere seconds) of about 50%, a chest radiograph ca
30 unction of kilovolt peak and tube output (in milliampere seconds), contrast resolution assessed in te
31 lts, and the mean quantity of x radiation in milliampere-seconds increased from 220 mAs for children
32 ickness (2, 4, 8 mm), pitch (1.0, 1.5, 2.0), milliampere setting (100, 175, 250 mA), and overlap of r
33                                          The milliampere setting had only a minor effect on image qua
34 uli at CT increases with higher kilovolt and milliampere settings, with higher kilovolts being partic
35 lovolt settings and up to 1.08-fold at lower milliampere settings.
36                               By using a low-milliampere technique and the quick-check method, CT flu
37                                     The mean milliampere value was 13.2 mA (range, 10--50 mA).
38 d and included site, depth, target diameter, milliampere value, kilovolt peak, fluoroscopic time, and
39                                     Current (milliampere) was increased stepwise during non-REM sleep

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