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We use the unique data set of Ulysses-SWICS which provides data in a wide rage of mass per charge, 2 ≤ m/q ≤ 9.33.
The flux of low energy ions detected in the alpha channel (mass per charge, m/q, of 2) is more intense than further tailward.
The mass per charge of observed ions is determined through a magnetic deflection system and a micro-channel plate based position detection system.
A mass per charge of 43 for PEI and a mass per phosphate of 325 Da for DNA were used to calculate the N/P ratio.
In Fig. 3(a) a mass spectrum in units of mass per charge versus counts per second obtained from the μ-APPJ connected via a tube made from polyamide (PA) is shown.
Individual compounds were identified based on retention time, UV spectra and their mass per charge ratio using LC-MS as described previously [18].
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Although it is difficult to identify the charge state of these ions definitively using SMS, which is a mass-per-charge analyzer, decomposition of the broad mass peak results in a reasonable ratio of O7+/O6+ to that in the solar wind.
Then, the mass-per-charge (M/q) of the incident ions is deduced with a combination of E/q and TOF values.
Fig. 13 Mass-per-charge (m/q) table of the 16 SV steps and 512 TOF channels used for the allocation of the 8 m/q bins in the Normal mode.
The output of the LC MS process is a set of peaks, characterized by their mass per unit charge and their chromatographic retention time.
X_{50} = A times [PF]^{ - 0.8} times Me^{0.167} times left( {frac{115}{RWSanfo}} right)^{0.633} (1 where X50: Mean size of fragments (m); PF: Specific charge (kg/m3); Me Charge mass per blast holes (kg); RWSanfo: The relative weight strength of the explosive to ANFO ; A: Rock coefficient, which is assumed to be 10.
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