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Description  |
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BACKGROUND OF THE INVENTION
The invention is concerned with a sound or probe for the determination of
the internal measurements of hollow organs and hollow parts of the body,
such as in a human, especially such which can only be reached by means of
sounds which have a small cross-section, as for example, the uterine
cavity.
The uterine cavity varies in size according to the individual, depending
for example on age, the number of previous pregnancies and childbirths,
and the intake of various hormonal preparations which are, for example,
used for the treatment of dysfunctional bleeding, corpus luteum
insufficiencies, endometriosis, uterine hypoplasia, myomas and also as
oral contraceptives.
The measurement of the uterine cavity occurs thus far with the aid of
sounds, the graduated scale of which makes it possible to determine the
distance between the orifice of the uterus and the fundus, in the
longitudinal direction. These sounds further serve to probe out the side
walls of the uterus.
Other measures such as bi-manual palpation give a subjective estimate of
the size and position of the organ. A contrast x-ray of the uterine cavity
is possible with hysterosalpingography. This system is of limited use for
genetic and fertility risk reasons.
The determination of changes in the interior of the uterus while under
hormonal therapy, as for example, for the prevention of hypoplasia with
resulting reduction in fertility, cannot be adequately performed by means
of the described methods. The measurement of the uterine axis does not
permit one to draw any conclusion regarding the overall change in the
uterine cavity. The evaluation of this measure by itself can, in certain
circumstances, lead to a false representation of the structure of the
uterine cavity. The use of intra-uterine contraceptives or pessaries has
shown a series of adverse effects, including metrorrhagia, endometritis,
gradual perforations of the uterine wall, intracavity and ectopic
pregnancies, as well as multiple laborlike contractions of the uterus
which, based on experience, can be traced back to a dimensional
incompatibility between the uterine cavity and the pessary. The
measurement of the uterine cavity, especially the transverse measurement,
i.e. the distance between both internal tubular os, is therefore a
prerequisite for the use of fitted intrauterine pessaries.
SUMMARY OF THE INVENTION
The object of the invention is to achieve a sound for the determination of
the internal measurements of hollow organs and hollow parts of the body
which, aside from the determination of the longitudinal measurements, also
permits a simple and exact determination of the transverse expansion or
distention of the existing cavity.
This is attained, according to the invention, by means of two rod shaped
spring elements at the head of the sound, which are, in turn, attached in
an axial direction at one end with their unattached ends spreading apart
from each other in one plane upon the release of tension. The invention
also utilizes a thread, under tensile stress, connecting the rod shaped
spring elements and being guided to their base by the sound. By means of
the thread the acutal distance between the rod shaped spring elements is
readable as the relative shift between sound and thread.
The thread can connect the rod shaped spring elements to one another at
suitable opposing locations. Unless the special shape of the hollow organ
to be measured does not allow this, the unattached ends are preferably
connected with one another; since they assume the greatest possible
distance with respect to one another, the relative shift between thread
and sound thus becomes greatest.
The connection of the unattached ends of the rod shaped spring elements
with the thread occurs most practically in such a way that the thread is
attached to one end, while it is guided in sliding fashion in the other
end and from there, extends to the base of the sound.
According to this type of attachment, the relative shift between sound and
thread corresponds just about exactly to the actual distance between the
unattached ends of the rod shaped spring elements.
A further possibility of connecting the unattached ends of the rod shaped
spring elements consists of attaching the thread at both ends and to
select the length of the thread such that it is at least nearly taut in
the spread condition of the rod shaped spring elements. At the midpoint of
the thread, an additional thread is attached and guided to the foot of the
sound. With this type of connection, the relative shift between the thread
and the sound does not have a linear relationship with the change in
distance between the rod shaped spring elements. In the case of distance
changes near the fully expanded state, there results a very great relative
shift while in the case of distance changes near the stressed state, there
results on the other hand only a very small relative shift. In the event
that a reading scale is installed, it must therefore be non-linear. This
type of connection for the unattached ends of the rod shaped spring
elements if above all advantageous in such instances where there is a
question of a very precise determination of the internal measurements of
hollow organs having a diameter which nearly corresponds to the distance
between the spread of the unattached ends of the rod shaped spring
elements.
In all cases, it is best to pass the thread to the foot of the sound
through a canal or passage inside the sound. Other guiding possibilities
are, however, also applicable, e.g. guiding of the thread in its own guide
tube or in guide loops mounted on the sound.
In practical use, the sound must be introduced into the cavity with the rod
shaped spring elements in the taut condition after which the spring
elements can be released inside the cavity. Various preferred designs of
the inventive sound results, depending on how the stressing and relaxing
of the rod shaped spring elements is effected.
This stressing and relaxing can be effected with the aid of a jacket in
which the sound is installed so as to be shiftable. By pulling the head of
the sound into this jacket, the rod shaped spring elements are tensed and
finally drawn along into the jacket. The tensing of the thread can be
brought about by means of a draw spring installed in a housing in the foot
of the sound.
Since the diameter of the sound is somewhat increased as a result of the
jacket, this arrangement presents problems in such applications where the
entrance opening to the cavity is very narrow. In such cases, the force
required for stressing the rod shaped spring elements is brought about by
the thread itself in that it is tightened, for example, by a scroll
installed at the foot of the sound. The thread can also be pulled directly
by hand. This possibility is, above all, advantageous with those inventive
sounds which are to be used as inexpensive one-way or single use devices.
In this case, the sound and the rod shaped spring elements are
advantageously made in one piece, out of plastic.
A reading scale is in all cases placed on the foot of the sound. If a
housing for a worm drive or a draw spring is present, the housing can be
provided with a slit at which the reading scale is located. A pointer
attached to the thread projects through the slit and indicates the
distance between the more or less spread apart unattached ends of the rod
shaped spring elements. The fully relaxed position of the spring elements
is established as the zero position. After the release of tension, the
spring elements spread as far as the cavity in question permits. The
degree of spreading and therewith the transverse measurement of the cavity
is transmitted via the thread to the scale and can be read. Other designs
are possible, however. For example, the housing can be transparent so that
the relative shift of the thread and the sound can be observed in the
interior of the housing insofar that an appropriate mark is placed on the
thread. Finally, it is also possible, for special cases, to adapt the
inventive sound insofar that only one rod shaped spring element is
provided, its counterpart being a rigid rod.
All embodiments of the sound according to the invention allow a simple,
rapid and precise determination of the internal measurements, of hollow
organs and hollow parts of the body. Further advantages are evident from
the examples of the invention hereinafter described.
THE DRAWINGS
FIG. 1 illustrates in cross-section a sound, in a jacket, in an almost
completely tensed state;
FIG. 2 shows the sound according to FIG. 1, partly in section, in the
almost completely relaxed state;
FIG. 3 shows a sound, according to which the tensile force is brought about
by a worm drive;
FIG. 4 shows a sound designed as a single use device;
FIGS. 5 and 6 illustrate other embodiments of the thread connection of the
rod shaped spring elements; and
FIG. 7 shows a section of the uterine cavity with the introduced sound
therein.
DETAILED DESCRIPTION
The embodiment according to FIGS. 1 and 2 consists of a hollow probe or
sound 1, on the head of which, according to the invention, two rod shaped
spring elements 2 are in turn attached at one end in an axial direction.
The unattached ends of the rod shaped spring elements 2 can spread apart
in one plane as illustrated in FIG. 2.
The unattached or free ends of the rod shaped spring elements 2 are
equipped with rounded feelers 3, 4. To the feeler 3 is attached the end of
a thread 5 which is passed through the feeler 4 in a slidable manner and
which extends through the interior of the sound 1 to the latter's foot. A
housing is mounted at the foot of the sound 1 with a draw spring 7 is
attached to the end of the housing to keep the thread 5 taut.
A pointer 8 is attached to the thread 5 near the junction between the draw
spring 7 and the thread 5 with pointer 8 being passed outward through a
longitudinal slit 9 located in the housing 6. The longitudinal slit 9 is
equipped with a scale 10. The thread 5 with the pointer 8 is pulled into
the sound 1 under the force of the draw spring 7 the position thereof
determining how far apart the rod shaped spring elements 2 are permitted
to spread. The path covered by the pointer 8 is, for practical purposes,
directly proportional to the actual spread of the free ends of the rod
shaped spring elements 2. The transverse measurement of the existing
cavity can therefore be read directly on the scale 10. When the rod shaped
spring elements 2 are completely together, the pointer 8 assumes the zero
position on the scale 10 similar to FIG. 1. By moving the sound 1 in an
axial direction outwardly and by actual determination of the internal
measurements, the structure of the inner space of the cavity in question
can be ascertained, point for point, in one plane. If one turns the sound
1 about its axis, the measurements in another plane can be carried out so
that in this manner one can finally measure the entire inner space, point
for point.
The stressing and relaxing of the rod shaped spring elements 2 is effected
by sliding the sound 1 in a jacket 11. The lower end of the jacket 11 is
widened to form a housing 24 for taking up the housing 6 and ends in a
grip ring 12. A corresponding grip ring 13 is placed on the housing 6. The
grip rings 12, 13 serve to limit the sliding movement of the jacket 11 and
allow one-handed manipulation of the device. When the jacket 11 slides
downward toward the foot of the sound 1, the rod shaped spring elements 2
spread apart. Their spread becomes maximal when the grip rings 12 and 13
touch each other. In the upper end position, the rod shaped spring
elements 2 are completely within the jacket 11. The opening of the jacket
11 is thereby sealed by the feelers 3 and 4 in such a way that no tissue
injury can result from the introduction of the device into the cavity to
be measured.
The functioning of the sound according to the invention is illustrated by
means of FIG. 7 using the uterine cavity as an example:
The sound 1 is completely pulled into the jacket 11 before insertion so
that the rod shaped spring elements 2 are located within the jacket 11 and
so that feelers 3, 4 cover the opening of the jacket 11. The device is
introduced, with this setting, through the orifice of the uterus 14 up to
the fundus. This setting is indicated with dotted lines in FIG. 7. Without
moving the sound 1 with the housing 6 the jacket 11 is now pulled back
until the grip rings 12, 13 are next to each other. The rod shaped spring
elements 2 thereby spread apart until the feelers 3, 4 are held by the
interior wall of the uterus. Upon spreading of the rod shaped spring
elements 2, the thread 5 is pulled under the force of the draw spring 7
into the foot of the sound. The path which is thereby covered can be read
on the scale 10 by means of the pointer 8. The reading corresponds to the
distance between the two feelers 3 and 4 and therefore also with the
actual measurement of the inner space in a transverse direction.
Before withdrawing the device the jacket 11 is held firm and the sound 1 is
pulled forward with the housing 6 until the rod shaped spring elements 2
are again inside the jacket 11. The device is then withdrawn.
Another embodiment of the sound according to the invention is shown in FIG.
3. The stressing and relaxing of the rod shaped spring elements is hereby
effected by a worm drive 16 which is mounted in a housing 17 attached to
the foot of the sound 1. The housing 17 is transparent so that the pointer
8 which is located on the thread 5 and which indicates on the scale 10 the
measure of the spread of the rod shaped spring element 2 can be observed.
In the zero position of the pointer 8 the rod shaped spring elements 2 are
held together by the thread 5. By turning the nut 18 the threaded spindle
19 is moved toward the foot of the sound 1 so that the rod shaped spring
elements 2 can spread apart. As soon as the feelers 3 and 4 are held by
the inner wall of the cavity, the pointer 8 stops since the connecting
thread 5 is no longer under tension.
An additional advantageous design of the sound according to the invention
is shown in FIG. 4. This design is especially suited as a one-way device
or single use disposable device. The sound 1, the rod shaped spring
elements 2, the feelers 3, 4 and the housing 20, located at the foot of
the sound 1 are made in one piece from the same material, e.g. plastic.
The eleasticity of the rod shaped spring elements 2 is thereby obtained
through manufacturing steps. The thread 5 connects the rod shaped spring
elements 2 as in the other designs and is attached to a rod 22, equipped
with a scale 21, which is arranged so as to be slidable within the housing
20. The rod 22 projects partially from the housing 20. The measure of the
projection of the rod 22 corresponds, in turn, to the spread of the rod
shaped spring elements 2 and can be controlled by means of the scale 21.
When introducing the sound 1 into the cavity to be measured, the rod 22 is
pulled back to its zero position so that the rod shaped spring elements 2
come together. As soon as the sound 1 is located in the desired position
inside the cavity, the rod 22 is released so that the rod shaped spring
elements 2 spread apart and come to rest against the inner wall of the
cavity.
The distance of the feelers 3 and 4 from each other can then be read on the
scale 21.
FIGS. 5 and 6 show a further possibility for the design of the thread
connection. With the thread connection according to FIG. 5, the thread 5
is attached at the ends of both rod shaped spring elements 2 to the
feelers 3 attached therewith. An additional thread 23 which leads to the
foot of the sound 1 is fastened to the middle of the thread 5. The change
in distance between the feelers 3 does not have, as was the case with the
previous designs, a linear relationship with the shifting of the thread
23. The greater the distance between the feelers 3 becomes the greater the
shifting of the thread 23 with a change in distance. An especially high
measuring sensitivity is hereby obtained in the spread state of the rod
shaped spring elements 2.
With the design according to FIG. 6, it is not the ends of the rod shaped
spring elements which are connected by the thread 5. The connection
occurs, rather, below the ends. This design is advantageous in such cases
where the possibility of introducing the sound in an axial direction is
limited but where the cavity continues sideways from the limitation.
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