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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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