Models SRJ-7 and HRJ-7 Juno Survey Meters
Models SRJ-7 and HRJ-7 Juno Survey Meters
Models SRJ-7 and HRJ-7 Juno Survey Meters
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OPERATING TEMPERATURE<br />
RANGE :<br />
35OF. TO 135OF.<br />
<strong>SRJ</strong> -7<br />
<strong>HRJ</strong> -7<br />
CASE :<br />
HANDLE :<br />
WE I GHT :<br />
HARD-CHROME PLATED ALUMINUM WITH ENGRAVED MARKINGS<br />
ON TOP OF CASE; GASKETED, DUST AND MOISTURE RESIST-<br />
ANT. DIMENSIONS: 11 1/2" L. x 5 3/4" W. x 6 1/2"<br />
H. e<br />
ALUMINUM ESPECIALLY CAST LOW-POROSITY, SMOOTHLY<br />
POL I SHED.<br />
6 LBS. 11 oz. NET.<br />
I l l . THEORY OF OPERATION<br />
A. IONIZATION CHAMBER.<br />
THE IONIZATION CHAMBER IS A RECTANGULAR ALUMINUM CASE, (THE INSIDE<br />
OF WHICH is COATED WITH AQUADAG) LOCATED IN THE FORWARD END, BOTTOM OF<br />
THE JUNO CASE. AIR AT ATMOSPHERIC PRESSURE IS THE IONlZATtON MEDIUM.<br />
THE COLLECTOR, AN ALUMINUM ROD COATED WITH AQUADAG, IS EXTREMELY WELL<br />
INSULATED BY MEANS OF A<br />
TEFLON SUPPORT BUSHING.<br />
ALPHA,<br />
BETA AND/OR<br />
GAMMA RADIATION, WHEN PASSING THROUGH THE CHAMBER, COLLIDES WITH INDIVID-<br />
UAL MOLECULES OF AIR. A COLLISION CAUSES AN ELECTRON TO BE DISPLACED<br />
FROM ITS NORMAL ENERGY LEVEL. ONCE REMOVED SUFFICIENTLY FAR FROM ITS<br />
NORMAL ENERGY LEVEL IT IS SUBJECTED TO STATIC ELECTRIC FORCE. THIS<br />
FORCE PULLS THE FREE ELECTRON TO THE COLLECTOR WHICH IS 90 VOLTS POSI-<br />
TIVE WITH RESPECT TO THE CHAMBER WALLS. THE MOLECULE, OR ATOM, AFTER<br />
LOSING AN ELECTRON ASSUMES A POSITIVE POTENTIAL (SUCH A CHARGED ATOM IS<br />
CALLED AN ION) AND IS ATTRACTED BY THE NEGATIVELY CHARGED WALLS. SINCE<br />
THE COLLECTOR IS WELL INSULATED THE ELECTRONS WHICH LAND ON ITS SURFACE<br />
BUILD UP A CHARGE, RESULTING IN A MORE NEGATIVE POTENTIAL. THIS NEGA-<br />
TIVE SHIFT IN THE COLLECTOR IS WHAT IS DETECTED BY THE ELECTROMETER CIR-<br />
CUIT. THE REASON FOR CHOOSING ALUMINUM COATED WITH AQUADAG IS TO DUPLI-<br />
CATE THE PERFORMANCE OF A<br />
HYFOTHETICAL A I R WALL CHAMBER AS NEARLY AS POS-<br />
SIBLE. IN ORDER TO GIVE A RELATIVELY CORRECT READING ON ALL TYPES OF<br />
RADIATION AND ALL ENERGIES, THE SOLID MATERIAL OF WHICH A CHAMBER IS<br />
MADE MUST NEARLY DUPLICATE THE<br />
IONIZING PROPERTIES OF AIR AND THEREFORE<br />
HAVE APPROXIMATELY THE SAME ATOMIC WEIGHT. AQUA~AG APPROACHES THIS<br />
CLOSELY AND ALUMINUM IS THE MOST ACCEPTABLE OF THOSE METALS WHICH HAVE<br />
SATISFACTORY STRUCTURAL PROPERTIES.<br />
B. ELECTROMETER TUBE AND GRID RESISTORS.<br />
VERY<br />
THE ELECTROMETER TUBE IS A SPECIALLY CONSTRUCTED, HIGH VACUUM PENTODE<br />
WHICH IS OPERATED AS A TRIODE. IT REQUIRES A VERY LOW POWER SIGNAL ON<br />
ITS GRID TO CONTROL ITS PLATE CURRENT. THE LOW POWER INPUT PERMITS THE<br />
USE OF AN EXTREMELY HIGH GRID RESISTOR, (R-I, R-2, OR R-3). HENCE, A<br />
VERY SMALL CURRENT THROUGH THE GRID RESISTOR WILL MAKE A<br />
READILY OBSERVED<br />
CHANGE IN THE PLATE CURRENT. IN TURN, THE PLATE CURRENT IS CONDUCTED<br />
THROUGH A 20 MICROAMPERE METER WHICH PROVIDES THE VISUAL INDICATION OF<br />
THE LEVEL OF RADIATION IN THE CHAMBER.<br />
THE CK 5886 ELECTROMETER TUBE<br />
FILAMENT OPERATES ON 10 MA., 1.25 VOLTS. THE PLATE VOLTAGE IS 6.5' AND<br />
THE PLATE CURRENT (WITH NO RADIATION) IS 80 MICROAMPS. THE TUBE IS<br />
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