ftp://spdf.gsfc.nasa.gov/pub/data/omni/high_res_omni/HRO_format.txt

This files gives the format of the High Resolution OMNI (HRO)
data set.  The content of the HRO data set is much more fully explained
at http://omniweb.gsfc.nasa.gov/html/HROdocum.html

The common format for the 1-min and 5-min* OMNI data sets is

Year			        I4	      1995 ... 2006
Day			        I4	1 ... 365 or 366
Hour			        I3	0 ... 23
Minute			        I3	0 ... 59 at start of average
ID for IMF spacecraft	        I3	See  footnote D below
ID for SW Plasma spacecraft	I3	See  footnote D below
# of points in IMF averages	I4
# of points in Plasma averages	I4
Percent interp		        I4	See  footnote A below
Timeshift, sec		        I7
RMS, Timeshift		        I7
RMS, Phase front normal	        F6.2	See Footnotes E, F below
Time btwn observations, sec	I7	DBOT1, See Footnote C below
Field magnitude average, nT	F8.2
Bx, nT (GSE, GSM)		F8.2
By, nT (GSE)		        F8.2
Bz, nT (GSE)		        F8.2
By, nT (GSM)	                F8.2	Determined from post-shift GSE components
Bz, nT (GSM)	                F8.2	Determined from post-shift GSE components
                                   See  footnote "gsm" below

RMS SD B scalar, nT	        F8.2	                
RMS SD field vector, nT	        F8.2	See  footnote E below
Flow speed, km/s		F8.1
Vx Velocity, km/s, GSE	        F8.1
Vy Velocity, km/s, GSE	        F8.1
Vz Velocity, km/s, GSE	        F8.1
Proton Density, n/cc		F7.2
Temperature, K		        F9.0
Flow pressure, nPa		F6.2	See  footnote G below		
Electric field, mV/m		F7.2	See  footnote G below
Plasma beta		        F7.2	See  footnote G below
Alfven mach number		F6.1	See  footnote G below
X(s/c), GSE, Re		        F8.2
Y(s/c), GSE, Re		        F8.2
Z(s/c), GSE, Re		        F8.2
BSN location, Xgse, Re	        F8.2	BSN = bow shock nose
BSN location, Ygse, Re	        F8.2
BSN location, Zgse, Re 	        F8.2

              Ancilary Data
AE-index, nT                    I6      See  footnote H below
AL-index, nT                    I6      See  footnote H below
AU-index, nT                    I6      See  footnote H below
SYM/D index, nT                 I6      See  footnote H below
SYM/H index, nT                 I6      See  footnote H below
ASY/D index, nT                 I6      See  footnote H below
ASY/H index, nT                 I6      See  footnote H below
PC(N) index,                    F7.2    See  footnote I below
Magnetosonic mach number        F5.1    See  Footnote K below



The data may be read with the format statement
(2I4,4I3,3I4,2I7,F6.2,I7, 8F8.2,4F8.1,F7.2,F9.0,F6.2,2F7.2,F6.1,6F8.2,7I6,F7.2, F5.1)

* Note For 5-min data  we added fluxes from GOES at the end of each record
 in format:
  Proton Flux >10 MeV, 1/(cm**2-sec-ster)  F9.2 See  footnote J below
  Proton Flux >30 MeV, 1/(cm**2-sec-ster)  F9.2
  Proton Flux >60 MeV, 1/(cm**2-sec-ster)  F9.2

Footnote A:

Percent interp: The percent (0-100) of the points contributing to 
the 1-min magnetic field averages whose phase front normal (PFN) 
was interpolated because neither the MVAB-0 nor Cross Product 
shift techniques yielded a PFN that satisfied its respective tests 
(see detailed documentation for these).

Footnote C: 

The DBOT (Duration Between Observing Times) words: For a 
given record, we take the 1-min average time shift and estimate, 
using the solar wind velocity and the location of the observing 
spacecraft, the time at which the corresponding observation 
would have been made at the spacecraft. Then we take the 
difference between this time and the corresponding time of 
the preceding 1-min record and define this as DBOT1. This 
difference would be one minute in the absence of PFN and/or 
flow velocity variations. When this difference becomes negative, 
we have apparent out-of- sequence arrivals of phase planes. 
That is, if plane A is observed before plane B at the spacecraft, 
plane B is predicted to arrive at the target before plane A. 
Searching for negative DBOT enables finding of such cases.

DBOT2 is like DBOT1 except that the observation time for 
the current 1-min record is compared to the latest (most time-
advanced) previous observation time and not to the observation 
time of the previous record. Use of DBOT2 helps to find 
extended intervals of out-of-sequence arrivals.

We do not capture out-of-sequence-arrival information at 15-s 
resolution but only at 1-min resolution. The standard deviation 
in the 1-min averaged time shifts may be used to help find cases 
of out-of-sequence 15-s data. 

Footnote gsm:
The computation of standard By and Bz, GSM is taken from the GEOPACK-2008 
at http://geo.phys.spbu.ru/~tsyganenko/Geopack-2008.html)
software package developed by Drs. Nikolai Tsyganenko. 

Footnote D: 

The following spacecraft ID's are used:
	ACE	71
	Geotail	60
	IMP 8	50
	Wind	51

Footnote E: 

Note that standard deviations for the two vectors are given
as the square roots of the sum of squares of the standard deviations
in the component averages.  The component averages are given in
the records but not their individual standard deviations.

Footnote F: 

There are no phase front normal standard deviations in the 5-min
records.  This word has fill (99.99) for such records.

Footnote G: 

Derived parameters are obtained from the following equations.

Flow pressure = (2*10**-6)*Np*Vp**2 nPa (Np in cm**-3, 
Vp in km/s, subscript "p" for "proton")

Electric field = -V(km/s) * Bz (nT; GSM) * 10**-3

Plasma beta = [(T*4.16/10**5) + 5.34] * Np / B**2 (B in nT)

Alfven Mach number = (V * Np**0.5) / (20 * B)

For details on these, see http://omniweb.sci.gsfc.nasa.gov/ftpbrowser/bow_derivation.html

Footnote H:
Provisional high res. Indices where taken from World Data Center for Geomagnetism, 
Kyoto: http://swdcwww.kugi.kyoto-u.ac.jp/aeasy/

Footnote I:
PC(N) index was taken from World Data Center for Geomagnetism, Copenhagen:
href="ftp://ftp.space.dtu.dk/WDC/indices/pcn/PCN_definitive/"

Footnote J: 
Proton fluxes from GOES were taken from http://satdat.ngdc.noaa.gov/sem/goes/data/new_avg/

Footnote K: Magnetosonic Mach Number = V/Magnetosonic_speed
            Magnetosonic speed = [(sound speed)**2 + (Alfv speed)**2]**0.5
            The Alfven speed = 20. * B / N**0.5 
            The sound speed = 0.12 * [T + 1.28*10**5]**0.5 
            About Magnetosonic speed check  http://ftpbrowser.gsfc.nasa.gov/bow_derivation1.html also
            

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