|
|
|
| United States Patent | 4109154 |
| Link to this page | http://www.wikipatents.com/4109154.html |
| Inventor(s) | Taumann; Leonhard (Lafayette, CA) |
| Abstract | In an electron accelerator having a target which is exposed to an electron
beam for the production of x-ray deceleration radiation, a conical
compensating member is arranged centrally within a cone pattern of the
x-ray radiation. The compensating member has a decreasing conical shape
toward the target and merges into a cylinder portion. Beam paths within
the cylinder portion which are additional to those in a conventional
purely conical compensating member are compensated by a recess positioned
in a base of the compensating member having an appropriately selected
depth. In another embodiment, a conically shaped compensating member is
arranged within the cone-shaped x-ray pattern such that a tip of the
compensating member is aligned away from the target and a base is aligned
toward the target. A collimator having a conical passageway surrounding
the x-ray radiation has a groove for receiving the base of the
compensating member so as to mount the same within the conical passageway
of the collimator. |
|
|
|
Title Information  |
|
|
|
|
|
Drawing from US Patent 4109154 |
|
|
X-ray beam compensation |
|
|
|
|
|
| Publication Date |
August 22, 1978 |
|
|
|
|
|
| Filing Date |
March 18, 1977 |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Title Information  |
|
|
References  |
|
|
| *references marked with an asterisk below are user-added references |
|
U.S. References |
|
|
|
|
|
|
U.S. References |
|
|
Foreign References |
|
|
|
|
|
|
Foreign References |
|
|
Other References |
|
|
|
|
|
|
Other References |
|
|
|
|
|
References  |
|
|
|
|
|
| Market Size |
|
Estimate the gross annual revenues of the relevant market
sector:
|
| | |
| |
|
|
| Market Share |
|
Estimate the percentage of the relevant market sector this invention will capture:
|
| | |
| |
|
|
| Reasonable Royalty |
|
What percentage of gross sales should the inventor or assignee be paid?
|
| | |
| |
|
|
|
Public's "Guesstimation" of Royalty Value
|
| Market Size | N/A | [No votes] | | x | Market Share | N/A | [No votes] | | x | Reasonable Royalty | N/A | [No votes] |
| | N/A | |
| |
|
|
|
|
|
|
|
|
|
|
|
|
Market Review  |
|
|
Technical Review  |
|
|
Claims  |
|
|
I claim:
1. An electron accelerator comprising:
(a) an electron beam;
(b) a target means exposed to the electron beam for producing x-ray
deceleration radiation in the shape of a cone;
(c) a massive conical compensating means for flattening the radiation
intensity distribution arranged centrally in the cone of the x-ray
radiation, said compensating means having a decreasing conical shape
towards the target means, and a base away from the target means;
(d) said decreasing conical shape merging into a cylindrical portion having
a frontal surface adjacent the target means; and
(e) a recess means positioned adjacent the base of the compensating means
and having a given depth for compensating portions of the x-ray radiation
in the cylindrical portion outwardly from the center of the radiation
cone, said portions being those portions of the x-ray radiation
intercepted by the cylindrical portion which are additional to those
portions intercepted in a conical embodiment of the compensating means.
2. An electron accelerator in accordance with claim 1, characterized in
that the frontal surface of the cylindrical portion of the compensating
means which is turned towards the target has margins which are rounded,
and an outer edge of the recess means protrudes slightly outwardly at the
base of the compensating means for compensating absorption.
3. An electron accelerator in accordance with claim 1, characterized in
that the cylindrical portion extends over approximately one-third of the
overall compensating means height.
4. An electron accelerator in accordance with claim 1 in which the
compensating means is made of stainless steel.
5. An electron accelerator in accordance with claim 1 in which the
compensating means comprises several sections with differing side
inclinations, the inclinations being steeper with increasing distance from
the base.
6. An electron accelerator comprising:
(a) an electron beam;
(b) a target means exposed to the electron beam for producing x-ray
deceleration radiation in the shape of a cone, and a collimator having a
conical passageway with a cylindrical portion for the radiation;
(c) a conical compensating means for flattening the radiation intensity
distribution arranged centrally in the cone of the x-ray radiation, said
compensating means having a tip aligned away from the target and a widened
carrier portion aligned toward the target;
(d) said collimator cylindrical portion having a groove means for receiving
the widened carrier portion of the compensating means and mounting means
for engaging the carrier portion of the compensating means within the
groove means; and
(e) said compensating means having several sections with different side
inclinations, the inclinations being steeper with increasing distance from
the carrier portion.
7. An electron accelerator in accordance with claim 6, characterized in
that the compensating means is made of stainless steel.
8. The accelerator of claim 6 in which the mounting means comprise
adjustable clamping members.
9. The accelerator of claim 8 in which the clamping members have inclined
surfaces which abut inclined surfaces on the carrier portion. |
|
|
|
|
Claims  |
|
|
Description  |
|
|
BACKGROUND OF THE INVENTION
1. Field of the Invention
The invention relates to an electron accelerator comprising a target
exposed to an electron beam for the production of x-ray deceleration
radiation and also comprising a massive cone-shaped compensating member
which is centrally arranged in the x-ray cone.
2. Description of the Prior Art
In the case of electron accelerators x-ray deceleration radiation is
produced due to a deceleration of the electrons in a so-called target. It
is known in the art to balance or compensate the dosage in a given
space-angle range of the x-rays leaving the target by placing a
compensating member into the portion of the x-ray cone of interest. This
compensating member has a conical design. Its contour path is adpated to
the path of the radiation intensity at the place of use. Since the dosage
decreases very markedly with the distance from the center beam behind the
target, the sides of the compensating member are correspondingly steep and
the tip of the compensating member must be positioned very precisely with
respect to the center beam.
In the case of a properly employed compensating member, the intensity
distribution as indicated by broken line 36 in FIG. 1 and which would be
assumed by the beam cone leaving the target at the location plane of a
patient undergoing treatment would be changed flattened continuous line
37. The compensating member absorbs the overly intense radiation in the
center as compared with the margins of a given beam cone. The portion of
beam cone having the intensity distribution represented by the horizontal
portion of curve 37 in FIG. 1 can be used for radiation purposes. It is a
disadvantage, therefore, that, even for exact positioning, misadjustments
of dose compensation can occur due to minor fluctuations of the direction
of the electron beam leaving the accelerator.
In order to decrease the difficulties encountered by adjustment of the
compensating member, it has been previously suggested to place the
compensating member further away from the target in a range of the beam
cone where the latter has already clearly widened. This, however, has the
disadvantage that the compensating member is then arranged closer to the
patient. Also, a portion of the beam which scatters unavoidably in the
compensating member along with its source, has also been placed closer to
the patient. Due to the square distance law, this causes an increased
radiation stress for the patient even with a relatively low-energy beam
component. Furthermore, due to the increase of the spacing between the
compensating member and the target, the entire beam defining system
becomes larger and heavier.
SUMMARY OF THE INVENTION
It is an object of this invention to provide a means of compensating the
dosage distribution in the useful portions of the x-ray cone such that the
alignment of the compensating member to the center beam is less critical.
In the case of an electron accelerator of this invention, the compensating
member decreases conically. Its decreased portion merges into a cylinder
such that the partial beam paths which are also in the cylinder portion of
the compensating member (as compared with the purely conical embodiment)
are compensated by a recess provided in the base of the compensating
member having an appropriate local depth. It thus results that the end of
the compensating member which is turned towards the radiation source is
blunt and thus less sensitive to alignment errors. The portions with
strong changes of the absorption values are placed into a plane
perpendicular to the beam direction at a greater distance from the focal
point and thus into an area where the beam cone has already widened to a
greater extent.
A further reduction of the preciseness with which the compensating member
must be aligned in the beam cone is obtained when, in a further
development of the invention, the front surface of the cylindrical portion
of the compensating member turned towards the target has its margins
rounded and the outer portion of the recess is slightly distorted
outwardly at the base of the compensating member in order to compensate
the absorption. Thus, the alignment of the compensating member becomes
less critical, including that range of the beam cone which corresponds to
the margin of the upper frontal surface of the cylindrical portion.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a diagram of the intensity distributions in the beam cone both
with and without a compensating member;
FIG. 2 is a schematic representation of a partially sectioned beam defining
system comprising a target, a collimator, and a compensating member placed
into the collimator;
FIG. 3 shows an enlarged illustration of the compensating member of FIG. 1;
and
FIG. 4 is another embodiment of a compensating member in a beam defining
system.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
FIG. 2 shows the locations of an exit window 1 of a vacuum tube 2 for the
electron beam, a target 3, a collimator 4, adjustable x-ray shielding
aperture plates 5, 6, 7, and the compensating member 8 in the partially
sectioned beam defining system 9.
The target 3 is arranged in the beam direction directly behind the exit
window 1 of the vacuum tube 2. It is positioned in a boring of a carrier
plate 10. An electron absorption member 11 is positioned in this boring
directly behind the target in the beam direction. The collimator 4 is
positioned in the beam direction directly behind the carrier plate 10 for
the target 3. Its conical passage opening 12 for the radiation has a
diameter of a few mm more than the maximum useful portion of the radiation
cone 13. It is aligned with respect to the center beam 14 of the beam cone
13. The x-ray shielding adjustable aperture plates 5, 6, 7 are arranged
behind the collimator in the beam direction in order to adapt the width of
the beam cone to the respective therapeutically required field magnitude.
An ionization chamber 16 for supervising the exiting beam is arranged
between collimator 4 and the x-ray adjustable screen plates 5, 6, 7. An
iron plate 15 with the compensating member attached thereupon is screwed
to the side of the collimator 4 which is turned away from the target 3.
This compensating member 8 is shown enlarged in FIG. 3. It essentially
comprises an increasingly more pointed conical member whose upper section
(which usually merges into a tip shown as a broken line) has been replaced
by a cylindrical portion 17. The margins of the frontal surfaces of the
cylindrical sections which are turned towards the radiation sources are
rounded. A ring-shaped recess 18 extending at an acute angle into the
compensating member is positioned at the base of the compensating member.
In FIG. 3, several selected beams 14, 19, 20 of the beam cone 13 are shown
as broken lines. These selected beams reveal that the ring-shaped recess
18 is provided in such a way that it compensates those partial paths which
represent x-rays leaving the target 3 divergently. These partial paths are
positioned in the cylindrical section 17 of the compensating member 8 and
are additional to those in a pointed compensating member. It thus results
that the outer margin of the ring-shaped recess must have a bulge 21 in
order to compensate the rounding 22 at the upper margin of the cylindrical
portion.
During the alignment of the compensating member 8, plane 23, which is
perpendicular to the center beam, is of importance since the ring-shaped
recess 18 in the compensating member merges into an acute angle within
this plane. This plane is spaced from the base 24 of the compensating
member at a distance equal to the height of the cylindrical section 17. In
the case of the present embodiment having a cylindrical section
representing one-third of the entire height of the compensating member 8,
this plane 23 is further remote from the target 3 by two-thirds of the
height of the compensating member than in a conventional compensating
member ending in a point. In this plane 23, the beam cone 13 is already
widened to a larger extent so that the alignment becomes less critical to
the same extent.
FIG. 4 shows another solution for the same problem. Here, the compensating
member 36, which is otherwise provided in a manner known to a large extent
in the prior art, is placed upside down, along with an otherwise identical
embodiment of the beam defining system 25. The compensating member 36 is
positioned in the passage opening of the collimator 31 with a tip 37
turned away from the target 30. Thus, the critical alignment plane 39 in
the area of the tip 37 of the compensating member 36 is spaced over the
full height of the compensating member 36 away from the target 30. In the
case of this arrangement, a pointed compensating member 36 can be used
without a ring groove milled into the base. When the compensating member
is rotated 180.degree., due to the divergence of the radiation all sides
of the compensating member 25 must be provided more steeply at twice the
angle of the beam divergence. In order to attach the compensating member
36 within the collimator 31, a conical passage opening 38 has a
cylindrical portion in the center range of the collimator. This
cylindrical portion has at its upper end a ring groove 40 of a larger
diameter. This ring groove is thus arranged in a plane perpendicular to
the symmetrical axis of the collimator 31 which coincides with the center
beam 28. In this ring groove 40 clamping jaws 42, 43 are arranged which
can be adjusted via screw threads 41 (only one is shown) and which are
displaced from one another by 120.degree.. A carrier plate 44 which is
connected with the base of the compensating member 36 can be mounted
between these clamping jaws 42, 43. The margin of the carrier plate 44 is
conically inclined into an angle of 45.degree. in the direction towards
the tip of the compensating member. The clamping surfaces of the clamping
jaws 42, 43 are adapted to meet with this inclination.
Although various minor modifications may be suggested by those versed in
the art, it should be understood that it is intended to embody within the
scope of the patent warranted hereon, all such embodiments as reasonably
and properly come within the scope of this contribution to the art.
* * * * *
|
|
|
|
|
Description  |
|
|
|
|
|