U.S. patent number 3,643,096 [Application Number 04/802,832] was granted by the patent office on 1972-02-15 for radioactive source shield with safe position indicator.
This patent grant is currently assigned to General Nuclear, Inc.. Invention is credited to Luther R. Jeffries, Jr., Charles F. Thompson.
United States Patent |
3,643,096 |
Jeffries, Jr. , et
al. |
February 15, 1972 |
RADIOACTIVE SOURCE SHIELD WITH SAFE POSITION INDICATOR
Abstract
Apparatus for indicating when a radioactive source capsule is in
a safe position within its shield comprises a gamma-sensitive
photoconductor located in the shield in close proximity to the safe
location of the radioactive source. The photoconductor operates a
visual indicator through electrical circuitry designed so that a
positive indication is given when the radioactive source is in its
safe position.
Inventors: |
Jeffries, Jr.; Luther R.
(Medford Lakes, NJ), Thompson; Charles F. (Millville,
NJ) |
Assignee: |
General Nuclear, Inc. (Houston,
TX)
|
Family
ID: |
25184833 |
Appl.
No.: |
04/802,832 |
Filed: |
February 27, 1969 |
Current U.S.
Class: |
250/370.01;
250/506.1; 250/497.1 |
Current CPC
Class: |
G01T
1/26 (20130101); A61N 2005/1008 (20130101) |
Current International
Class: |
G01T
1/00 (20060101); G01T 1/26 (20060101); G01t
001/26 (); G21f 005/00 () |
Field of
Search: |
;250/108,16S,83.3 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Lawrence; James W.
Assistant Examiner: Frome; Morton J.
Claims
We claim:
1. A shield for storing a radioactive source comprising a mass of
radiation-shielding material having a passage extending within said
material through which the source may be moved between a safe
storage location and a position for use, said passage being
tortuous so that the safe storage location is one from which
radiation cannot be emitted to the exterior of said mass of
shielding material, radiation detecting means located closely
adjacent to said safe storage location for providing an electrical
response to radiation, for indicating the intensity of the
radiation received by said detecting means, and an electrical
connection between said detecting means and said indicating means
for actuating said indicating means in response to the intensity of
radiation received by said detecting means from the source, said
electrical connection comprising means for decreasing the
sensitivity of the indicating means, in the high range of radiation
intensities, to variations in the intensity of the detected
radiation, below that sensitivity which would exist in the absence
of said decreasing means.
2. A shield according to claim 1, in which said detecting means
comprises a photoconductor, in series with a source of electric
current and said indicating means, and said means for decreasing
the sensitivity of said indicating means comprises a resistor in
series with said photoconductor, said source of electric current
and said indicating means.
3. A shield according to claim 1, in which said means for
decreasing the sensitivity of the indicating means comprises a
bridge circuit, means responsive to the detecting means for varying
the resistance of one branch of said bridge, and wherein said
indicating means is responsive to the output of said bridge.
4. A shield for storing a radioactive source comprising a mass of
radiation-shielding material having a passage extending within said
material through which the source may be moved between a range of
storage positions and a position for use, means for preventing
radiation from a radioactive source from escaping to the exterior
of said mass of shielding material when said radioactive source is
located within said range of storage positions, radiation detecting
means located closely adjacent said range of positions within said
passage for providing an electrical response to radiation,
indicating means, and an electrical connection between said
detecting means and said indicating means for actuating said
indicating means in response to the intensity of radiation received
by said detecting means from the source, said electrical connection
comprising means for decreasing the sensitivity of the indicating
means, in the high range of radiation intensities, to variations in
the intensity of the detected radiation below that sensitivity
which would exist in the absence of said decreasing means.
5. A shield according to claim 4, in which said detecting means
comprises a photoconductor, in series with a source of electric
current and said indicating means, and said means for decreasing
the sensitivity of said indicating means comprises a resistor in
series with said photoconductor, said source of electric current
and said indicating means.
6. A shield according to claim 4 in which said means for decreasing
the sensitivity of the indicating means comprises a bridge circuit,
means responsive to the detecting means for varying the resistance
of one branch of said bridge, and wherein said indicating means is
responsive to the output of said bridge.
Description
BACKGROUND OF THE INVENTION
This invention relates to radioactive source position indicators
for use in conjunction with source capsule storage shields. The
purpose of these indicators is to provide a visual indication when
the radioactive source is in a safe position within its shield so
that the user can know when it is safe to approach and handle the
shield.
In the past 15 years, the usage of radioactive isotopes for
industrial radiography has replaced the usage of X-ray equipment in
many radiographic operations performed in the field. The use of
radioactive isotopes has also become important in medicine.
The principal disadvantage of the use of radioactive isotopes is
the fact that they emit gamma radiation continuous and thus must be
shielded by a covering of dense material when not in use. Because
of the dangers to personnel which are involved, it is desirable to
make a survey of a radioactive exposure device when each exposure
is completed in order to make sure that the radioactive source is
in a safe, shielded position. This survey must be made with an
instrument capable of detecting gamma radiation. In fact,
government regulations require these precautions.
Even though precautions are required, and the prescribed procedures
should be foolproof, many instances are reported each year where
technicians and others are exposed to overdoses of radiation
through the failure of the technician to follow the proper survey
procedures.
Several attempts have been made in the prior art to overcome the
problem of accidental exposure by the incorporation of mechanical
and electromechanical indicators in the exposure device.
In most exposure devices, a radioactive source capsule is pushed or
pulled through a tortuous passage in a shield by a control cable.
In some devices, air pressure is used to move the radioactive
source capsule. In the case of cable-controlled source capsules, it
is common to rely on the position of the cable as an indication of
the position of the source within the shield. Indicators have been
provided which are activated by the control cable or by some other
part which should move with the radioactive source capsule. In the
case of air pressure control, microswitches have been arranged to
be activated by the source capsule when it is in a safe
position.
Several dangers are inherent in source position indicators in the
prior art. As most of these indicators are complicated devices with
several moving parts built as small as possible to conserve space
and weight, they have a tendency to fail at inopportune times.
Another serious fault of such indicators is the fact that they are
activated not entirely by the source, but by some other part that
should move with the source, for example, the control cable. If,
for some reason, a source capsule became separated from its control
cable it could remain exposed when the indicator is indicating a
safe condition. Exposure devices which are equipped with indicators
controlled by cables and other parts which move with the source
capsule become more dangerous and hazardous than devices without
source position indicators since technicians tend to rely on
indicators on the device, and tend not to use an external survey
meter such as a Geiger counter.
SUMMARY OF THE INVENTION
In accordance with the invention, a cable-controlled source capsule
is used. Its presence at a safe position in the tortuous passage
within a shield is detected by a gamma-sensitive photoconductor
buried in the shield material in close proximity to the safe
location of the radioactive source. The detector can only be
activated by the source in the safe position. The principal
advantage of the use of a gamma-sensitive detector buried in the
shield material is the fact that it cannot be activated by the
control cable or by anything other than the source capsule. In
addition the gamma-sensitive detector has the advantage of
extremely high reliability.
The detector activates an indicating device, for example a meter,
through extremely simple circuitry which is designed so that the
failure of any component will result in a readily recognized
indication on the meter or other indicator that such a failure has
occurred. The principal object of the invention, therefore, is to
provide a source position indicator which is "fail safe" in its
operation.
Since some of the radioactive sources used in industrial
radiography have short half-lives, it is necessary to provide
compensation for source strength variations in the indicating
circuitry. Accordingly, a further object of the invention is to
provide such compensation so that similar indications are provided
when radioactive sources are in their safe position even though
their strength may differ considerably.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a vertical section of a radioactive source shield in a
carrying case, the figure also showing an external control cable
and a tube for transporting a source capsule from the shield to the
position at which an exposure is to take place;
FIG. 2 is a schematic diagram of an electrical circuit for
controlling an indicating meter in accordance with the
invention;
FIG. 3 is a schematic diagram of an electrical circuit provided
with means for compensating for variations in source strength;
and
FIG. 4 is a schematic diagram of an alternative electrical circuit
having compensating means.
DESCRIPTION OF THE PREFERRED EMBODIMENT
FIG. 1 shows a carrying case 2 provided with a carrying handle 4.
Within case 2, there is mounted a massive shield 6 consisting of
lead or other dense material which cannot be penetrated by alpha,
beta or gamma radiation. An S-shaped passage 8 extends through the
shield material from an opening 10 to a threaded opening 12.
A radioactive source capsule 14, which is of conventional design,
is shown in what is termed a "safe" position in the S-shaped
passage 8. The passage is so shaped that radiation emanating from
the radioactive isotope within capsule 14 cannot escape through
openings 10 and 12 when the capsule is in this position.
A short length 16 of cable is attached at one end to the capsule
and terminated at its other end in a connector 18, which extends
into a passage 20 provided in a block 22 which is an integral part
of the wall of the carrying case. The outer end of passage 20 is
threaded at 24, the threads being provided so that member 26 can be
connected to the carrying case. Member 26 has an internal passage
28, through which control cable 30 passes. A connector 32 on cable
30 is adapted to be engaged with connector 18 on cable 16 so that
the position of the source capsule 14 can be controlled from a
remote position through cables 30 and 16. A lock 34, having an
extendible plunger 35 prevents the source capsule from moving
downwardly to an unsafe position because of the engagement of
plunger 35 with connector 18. In order to engage connectors 32 and
18, connector 18 is pulled outwardly so that it clears threads 24.
A stop 37, attached to cable 16 and engageable by plunger 35,
prevents connector 18 from being pulled so far outwardly as to
expose the source capsule.
A tube 36 is provided with a threaded connector 38, which is
adapted to be connected at opening 12. Tube 36 carries the
radioactive source capsule to the position in which a radiographic
exposure is to be made.
A plug, indicated generally at 40 is preferably made from lead or
another suitable shielding material. Plug 40 is an integral element
comprising a cylindrical portion 42, a larger cylindrical portion
44, and a cap portion 46, which has an annular face 48 which
engages the external wall of the shield. Plug 40 fits into a
conforming opening in shield 6, the opening extending from the
exterior of the shield to the interior passage 8. The differences
between the diameters of cylindrical portions 42 and 44, and the
annular portion 48 of the cap provide a stepped configuration of
the plug which prevents the leakage of radiation. A tortuous
passage 49 is provided in the plug elements 44 and 46 for an
electrical cable.
Within cylindrical portion 42 a passage 50 is provided. Within
passage 50 there is located a gamma-sensitive photoconductor 52.
This photoconductor is preferably a cadmium sulphide or cadmium
selenide cell, which is sensitive to gamma radiation, but may be
any other device providing an electrical response, i.e., either a
change in electrical characteristics or an electrical output, to
alpha, beta or gamma radiation. A two-conductor cable 54 extends
from detector 52 and through passage 49 in the plug elements 44 and
46 to the circuitry at 56. A single-conductor cable can be used as
well if the circuit is completed through the shield material. A
battery is indicated at 58. An electrical cable 60 extends from the
circuitry indicated at 56 to an indicating meter 62, mounted in the
cover of the carrying case.
From FIG. 1, it will be apparent that detector 52 will only respond
to radiation from the radioactive isotope within capsule 14 when
capsule 14 is in close proximity with detector 52. If capsule 14
were moved to a position such that radiation could be emitted
through one of openings 10 and 12, it would be so remote from
detector 52 that the detector would not respond to a significant
degree. The tortuous configuration of passage 8 not only prevents
the escape of radiation but also shields the detector 52 from
external light.
In the electrical diagrams, primed reference numerals indicate
elements which correspond to elements shown in FIG. 1.
FIG. 2 shows a simple, uncompensated circuit comprising battery
58', milliammeter 62', and photoconductor 52' connected in series.
Photoconductor 52' is a cadmium sulphide cell or another
photoconductor which has the characteristic that its resistance
decreases as the intensity of radiation impinging upon it
increases. In its operation, when the source capsule is in its safe
position, the resistance of detector 52' is greatly decreased, and
meter 62' gives a positive indication of the safe condition. In the
use of the circuit of FIG. 2, a minimum meter indication should be
established. If the technician operating the device observes a
meter reading lower than this minimum when he expects the source
capsule to be in its safe position, he should make a check with an
external Geiger counter. It may be that the low reading is due to
battery age, but, in no case, will the meter give the expected
reading when the source capsule is not in its safe position. A
short circuit across detector 52' will produce an extraordinarily
high indication on the meter which may be protected by a series
resistance. In either case, the meter will provide a readily
recognizable indication of a malfunction.
When the technician is returning the radioactive source capsule to
is safe position, he can observe the meter indication passing
through its maximum as the source capsule approaches and moves past
the detector. The continuous variation of the meter indication
gives absolute assurance to the technician that the source capsule
is in the vicinity of the detector. The technician simply adjusts
the position of the source capsule until the meter gives a maximum
reading. The lock 34 is then operated to extend plunger 35, and
connector 32 is disconnected from connector 18. The meter can be at
a remote location from the shield if desired.
It should be noted at this point that the electrical circuit of
FIG. 2 is perfectly suitable where radioactive sources having
relatively long half-lives are used. However, in the case of a
radioisotope having a short half-life, for example, Iridium 192,
which has a half-life of 74 days, consideration must be made for
variations in source strength which occur over a period of time. In
practice, the strength of the radioactive source might decrease
over a period of time by a factor of 100. FIGS. 3 and 4 show
alternative circuits by which these source strength variations are
taken into account so that the meter indication, when the source is
in its safe position, is approximately the same regardless of the
source strength.
Referring particularly to FIG. 3 a battery 58", a meter 62", a
detector 52" and a resistor 66 are connected in series. Detector 52
" is located adjacent the safe position of the source within the
shield. The circuit of FIG. 3 operates similarly to that shown in
FIG. 2 in that the presence of the radiation source in proximity
with detector 52" causes its resistance to decrease, and causes an
increase in current through meter 62". However, while the circuit
of FIG. 2 is highly sensitive to differences in detector
resistances, especially in the range of low resistances, in the
case of FIG. 3, the inclusion of resistor 66 in series with the
detector 52" decreases the sensitivity of the circuit to
differences in detector resistance in the low resistance range. The
circuit of FIG. 3 consequently exhibits similar meter readings for
radiation sources in the safe location regardless of their
radiation intensities, and it is therefore capable of accommodating
radiation sources having short half-lives.
The circuit of FIG. 4 produces a result similar to that produced by
the circuit in FIG. 3, and, in addition, it provides amplification
so that relatively insensitive detectors can be used, and weak
radiation sources will be accommodated.
A battery 58'" has its positive end connected to line 68, and its
negative end connected to line 70. Resistors 72 and 74 are
connected in series between lines 68 and 70. The emitter-collector
circuit of PNP-transistor 76 is connected in series with resistor
78 between lines 68 and 70, the emitter of the transistor being
connected to line 68. Resistors 72, 74 and 78, along with
transistor 76 form the arms of a Wheatstone bridge. Milliammeter
62'" is connected between the junction of transistors 72 and 74 and
the connection between the collector of transistor 76 and resistor
78 to form the bridge. Photoconductor 52'" is connected at one
terminal to line 68, and its other terminal is connected through
resistor 79 to line 70. NPN-transistor 80 has its emitter connected
to line 70, and its collector is connected directly to the base of
transistor 76, and through resistor 82 to line 68. The base of
transistor 80 is connected to the junction between resistor 78 and
photoconductor 52'".
The parameters of the various components are desirably selected so
that the bridge is in a balanced condition when the resistance of
photoconductor 52'" is high. As the resistance of the
photoconductor decreases as a result of radiation, both transistors
become increasingly conductive, and the bridge becomes unbalanced
so that a current is registered by meter 62'".
A Wheatstone bridge has the characteristic that it is most
sensitive to variations in the resistance of one of its arms when
it is near its balanced condition, and less sensitive when it is
brought further away from its balanced condition. Accordingly weak
and strong radiation sources are responded to similarly. Further
compensation can be accomplished, if desired, by operating one or
both of the transistor near saturation.
In summary, the radioactive source position indicator in accordance
with the invention is "fail safe" in that it is impossible for it
to indicate that the radioactive source is in its safe position
when it is not. Malfunctions in the electrical circuitry will
produce readily recognizable indications warning the operator that
they exist. High reliability is achieved because of the simplicity
of the apparatus and the absence of moving parts (with the
exception of the meter movement). The auxiliary circuitry permits
the apparatus to provide consistent responses to radioactive
sources having short half-lives.
* * * * *