GOES (Geostationary Operational Environmental Satellite) X-ray sensors observe the Sun continuously in two broadband soft X-ray channels. These data are collected in real time and are used operationally to detect the onset and the intensity of solar flares. For these purposes it is usually sufficient to monitor only the soft channel (1–8 Å). The second, harder channel (0.5–4 Å) provides additional information on the state of the coronal plasma. The dual X-ray measurement data are archived and made available to external users for basic research.The GOES X-ray sensors operate on the ion-chamber principle: measured ion-chamber electric current is proportional to the net ionization rate caused by incident X-ray flux on encapsulated noble gases. The ratio of the outputs of the two channels in electric current, therefore, is uniquely a function of the color temperature of the emitting plasma, and the magnitude of each of the currents is proportional to a quantity, known as the emission measure, that convolves the volume and the density of the emitting plasma.This paper provides a detailed description of the procedure used for computing color temperature and emission measure from GOES X-ray data, including a table of constants for SMS and GOES X-ray sensors that are necessary for reducing the archived data from these satellites. Temperature and theoretical current tables were constructed, for individual GOES sensors, from laboratory calibrations of instrument responses and from synthetic solar X-ray spectra generated by two models of solar thermal X-ray emission: Raymond-Smith and Mewe-Alkemade. Example tables are shown and others are available on request.Errors that may be incurred from the use of GOES X-ray data in the computation of flare temperatures and emission measures may be classified under four major groups: instrumentinduced errors, including errors of calibration and random measurement errors; environmentally induced errors, due primarily to the ambient energetic electron background; solar influences, including the consequences of the isothermal assumption and the single-source assumption; and uncertainties in the modelled solar synthetic spectrum. These error sources are discussed separately, and a rough estimation of the collective error is made where this is quantitatively feasible. Finally, temperatures and emission measures are computed from GOES data and are compared with those derived from SMM andHinotori soft X-ray spectrometer data and from broadband photometric data from the PROGNOZ satellite.
[1]
Allen S. Krieger,et al.
Identification and analysis of structures in the corona from X-ray photography
,
1973
.
[2]
Constantino Macías Garcia,et al.
Social Behavior and Operational Sex Ratios in the Viviparous Fish Girardinichthys multiradiatus
,
1994
.
[3]
R. Mewe.
Calculated solar X-radiation from 1 to 60 Å
,
1972
.
[4]
J. Culhane.
Thermal Continuum Radiation from Coronal Plasmas at Soft X-ray Wavelengths
,
1969
.
[5]
I. Craig,et al.
Fundamental limitations of X-ray spectra as diagnostics of plasma temperature structure.
,
1976
.
[6]
C. Crannell,et al.
Expressions to determine temperatures and emission measures for solar X-ray events from GOES measurements
,
1984
.
[7]
Ester Antonucci,et al.
The energetics of chromospheric evaporation in solar flares
,
1984
.
[8]
Katsuo Tanaka.
Solar flare X-ray spectra of Fe XXVI and Fe XXV from the Hinotori satellite
,
1986
.
[9]
R. Rosner,et al.
Dynamics of the quiescent solar corona
,
1978
.
[10]
P. McIntosh,et al.
High-temperature flares observed in broadband soft X-rays
,
1991
.
[11]
F. Fárník,et al.
Flare plasma diagnostics based on the soft X-ray photometric data from GOES and PROGNOZ
,
1992
.
[12]
R. Kreplin,et al.
The NRL SOLRAD X-ray detectors: A summary of the observations and a comparison with the SMS/GOES detectors
,
1991
.
[13]
W. Tucker,et al.
Radiation from a high-temperature, low-density plasma - The X-ray spectrum of the solar corona
,
1971
.
[14]
J. Lemen,et al.
Calculated X-radiation from optically thin plasmas. VI - Improved calculations for continuum emission and approximation formulae for nonrelativistic average Gaunt actors.
,
1986
.
[15]
P. Bornmann.
Limits to derived flare properties using estimates for the background fluxes - Examples from GOES
,
1990
.
[16]
J. Culhane,et al.
A Simplified Thermal Continuum Function for the X-ray Emission from Coronal Plasmas
,
1970
.