Time Correction for the Experimental CW EPR Time Series.
Source:R/correct_time_Exp_Specs.R
correct_time_Exp_Specs.Rd
Providing more accurate time for EPR spectral line/spectrum appearance. It assumes
that the middle \(B\) (or \(g\), \(\nu_{\text{MHz}}\)...etc.) of the EPR spectrum
is set as the CF (central field
) for the spectrum sweep.
Arguments
- time.s
Numeric value/vector/column in
data frame
, corresponding totime
(ins
) at which the individual EPR spectra were recorded (supplied by the EPR acquisition software).- Nscans
Numeric, number of accumulations (number of scans usually denoted as
AVGS
) for each spectrum in EPR time series.- sweep.time.s
Numeric, time (in
s
) for recording individual EPR spectrum \(\equiv\) one "accumulation".
Value
Numeric value/vector, corresponding to time at which the middle (\(x\)-axis) of EPR spectrum/spectra were recorded during the kinetic measurements (e.g. radical formation, stability, electrochemical and/or photochemical measurements).
Details
The actual time at the middle/crossing point is different from that recorder by the EPR acquisition software, see below. This is especially important in determining the kinetics of radical generation or decay. Time is recorded according to the following scheme, where "^v" in the scheme denotes the derivative form of an EPR spectrum:
EPR Spectr. | EPR Spectr. | ||||
t[1] | ——^v——> | t[2] -delay | —-> | t[2] | ——^v——-> ... |
N_scans *swt | delay | N_scans *swt |
The recorded times are: t[1]
,t[2]
,t[3]
,...
and the N_scans
corresponds to number of scans
, swt
to sweep time
for the individual scan. These parameters can be obtained by the readEPR_params_slct_kin
or other functions which can read the instrumental parameter files.
See also
Other Conversions and Corrections:
convert_A_MHz_2a()
,
convert_B()
,
convert_a_mT_2A()
,
convert_time2var()