METHOD AND DEVICE FOR THE INSPECTION OF A CONDITION OF A CANNULA MOUNTED ON A SYRINGE

Abstract

A method for the inspection of a condition, in particular for the detection of defects, of a cannula (or injection needle) mounted on a syringe, which is located under a protective cap, and devices for carrying out such methods. A method includes measuring a magnetic field, in particular a magnetic field distribution, in the vicinity of the cannula. The presence of a ferromagnetic cannula causes a local change in the course of the magnetic field lines. This can be measured and used to determine whether the cannula, as desired, is arranged straight and coaxially to the syringe longitudinal axis, or whether it has a defect, such as being bent, kinked, compressed, broken/severed, oblique to the longitudinal axis of the syringe or eccentric to the longitudinal axis of the syringe.

Claims

1. Method for the inspection of a condition of a cannula which is mounted on a syringe and located in a cannula protective cap, wherein the method comprises the measuring of a magnetic field in the vicinity of the cannula.

2. Method according to claim 1, wherein one or more magnetic field sensors are used to measure the magnetic field.

3. Method according to claim 2, wherein the one or more magnetic field sensors are designed as one-, two- or three-axis magnetic field sensors to measure the magnetic field in one, two or three dimensions.

4. Method according to claim 2, wherein for measuring the magnetic field the cannula is moved relative to the one or more magnetic field sensors, wherein the syringe is rotated about its longitudinal axis and/or moved along its longitudinal axis, or the one or more magnetic field sensors are moved parallel to the longitudinal axis of the syringe.

5. Method according to claim 1, wherein the magnetic field is generated, at least in part by the earth's magnetic field, by an arrangement comprising one or more permanent magnets, or by an arrangement comprising one or more electromagnets, wherein the arrangement also comprises one or more iron cores.

6. Method according to claim 1, wherein a magnetic shield is used to suppress magnetic interference fields.

7. Method according to claim 1, comprising a comparison of the measured magnetic field for the cannula with the measured magnetic field for a reference syringe with a mounted reference cannula located in a cannula protective cap having a desired condition, and a determination of the condition of the mounted on the syringe based on the comparison.

8. Method according to claim 7, wherein the determination of the condition of the cannula mounted on syringe is based on the comparison of an amplitude and/or phase position of the measured magnetic field for the reference cannula with an amplitude and/or phase position of the measured magnetic field for the cannula.

9. Method according to claim 1, comprising a transformation of a measured time course of the magnetic field from the time domain to the frequency domain.

10. Method according to claim 1, wherein the condition of the cannula is at least one of straight, bent, kinked, compressed, broken/severed, coaxial to the syringe longitudinal axis, oblique to the syringe longitudinal axis, eccentric to the syringe longitudinal axis.

11. Device for the inspection of a condition of a cannula mounted on a syringe, which is located in a cannula protective cap, wherein the device comprises one or more magnetic field sensors for measuring a magnetic field in the vicinity of the cannula.

12. Device according to claim 11, wherein the one or more magnetic field sensors are designed as one-, two- or three-axis magnetic field sensors to measure the magnetic field in one, two or three dimensions.

13. Device according to claim 11, further comprising a means for moving the cannula relative to the one or more magnetic field sensors for rotating the syringe about its longitudinal axis and/or for moving the syringe along its longitudinal axis, or for moving the one or more magnetic field sensors parallel to the longitudinal axis of the syringe.

14. Device according to claim 11, further comprising an arrangement having one or more permanent magnets and/or an arrangement having one or more electromagnets for generating a magnetic field, wherein the arrangement also comprises one or more iron cores.

15. Device according to claim 11, further comprising a magnetic shield for suppressing magnetic interference fields.

16. Device according to claim 11, further comprising a comparator unit for the comparison of the measured magnetic field for the with the measured magnetic field for a reference syringe with a mounted reference cannula located in a cannula protective cap having a desired condition, and for the determination of the condition of the cannula mounted on the syringe based on the comparison.

17. Device according to claim 16, wherein the comparator unit is designed to perform a comparison of an amplitude and/or phase position of the measured magnetic field for the reference cannula with an amplitude and/or phase position of the measured magnetic field for the cannula, and to determine therefrom the condition of the cannula mounted on the syringe.

18. Device according to claim 11, further comprising a unit for performing a transformation of a measured time course of the magnetic field from the time domain to the frequency domain.

19. Device according to claim 11, further comprising an output for providing an output signal, which is designed to indicate the condition of the cannula as at least one of straight, bent, kinked, compressed, broken/severed, coaxial to the syringe longitudinal axis, oblique to the syringe longitudinal axis, eccentric to the syringe longitudinal axis.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0033] Non-limiting exemplary embodiments of the present invention are explained in further detail below with reference to figures, wherein:

[0034] FIG. 1 shows an X-ray image (according to the prior art) of a syringe with a protective cap in place, under which there is a bent cannula;

[0035] FIG. 2 shows an example of the field line progression of the earths magnetic field (with an inclination of 64°) in the vicinity of a curved steel injection needle;

[0036] FIG. 3 shows a schematic side view of an embodiment variant of a device according to the invention; and

[0037] FIG. 4 shows a schematic side view of a further embodiment variant of a device according to the invention with a Helmholtz coil.

[0038] In the figures, the same reference numerals stand for the same elements.

DETAILED DESCRIPTION OF THE INVENTION

[0039] In the assembly process of medical syringes, such as single-use insulin syringes, the cannula or injection needle is mounted on or attached to the syringe, e.g. glued in place, and then a protective cap is mounted on or attached to the cannula. The cannula must penetrate the material of the protective cap.

[0040] Accordingly, this process takes place with a certain force, so that the cannula can be bent, kinked, compressed, or can break or break off. These defects pose a multiple risk, e.g. there is a risk of injury during use and/or sterility is no longer ensured.

[0041] FIG. 1 shows an X-ray image of a syringe 1 with a mounted/attached optically opaque protective cap 3, under which a bent cannula 2 is located, as recorded in a prior art process.

[0042] The present invention utilizes the effect that ferromagnetic materials influence an external magnetic field in their environment. Thus, ferromagnetic materials tend to draw magnetic fields into themselves. The field lines of an external magnetic field end on the surface of the ferromagnetic body and run inside it. Thus, the presence of a steel injection needle causes a local change in the course of the magnetic field lines. An intact, i.e. straight needle will cause a different change in the magnetic field lines than a needle which has a kink, for example.

[0043] FIG. 2 schematically illustrates an example of the field line progression F of the earths magnetic field in the vicinity of a bent injection needle or cannula 2. Depending on the latitude, the earths magnetic field inclines differently in the direction of the earth. For example, the earths magnetic field shown in FIG. 2 has an inclination of 64° downward corresponding to the 47th degree of latitude. The magnetic field lines F are focused by the steel injection needle 2 and the field lines further out are deflected towards the injection needle 2. This deformation of the field lines compared to the case where the injection needle 2 is straight can be detected by measuring the magnetic field, in particular the magnetic field distribution, in a vicinity of the cannula 2. Based on the measurement of the magnetic field at one or more points, e.g. on or along the measuring section S, it is then possible to infer the condition of the cannula 2, i.e., whether it has a particular defect such as a kink.

[0044] One or more magnetic field sensors, such as an induction sensor, a fluxgate magnetometer, a Hall sensor, a magnetoresistive sensor, such as an AMR (anisotropic magnetoresistive), CMR (colossal magnetoresistance), GMR (giant magnetoresistance) or TMR (tunnel magnetoresistance) sensor, can be used to measure the magnetic field or the magnetic field distribution. These magnetic field sensors can be designed as one-, two- or three-axis magnetic field sensors to measure the magnetic field or the magnetic field distribution in one, two or three dimensions. In this process, the cannula 2 can be moved relative to one or more magnetic field sensors, or conversely one or more magnetic field sensors can be moved relative to the cannula 2, e.g. vertically along the measuring section S, so that the magnetic field or the magnetic field distribution can be determined over the entire length of the cannula 2.

[0045] FIG. 3 shows a schematic side view of an embodiment variant of a device for inspecting injection needles according to the invention. The syringe 1 is clamped in a syringe holder 5, which is arranged on a rotating device 6, by means of which the syringe 1 can be rotated about its longitudinal axis a. As a result of the rotation, the cannula 2 periodically changes the earths magnetic field in the vicinity of the cannula 2. The earths magnetic field is measured with the aid of the magnetic field sensor arrangement 4.sub.A, which consists of five magnetic field sensors 4.sub.1, □, 4.sub.5, which are arranged vertically one above the other parallel to the longitudinal axis a of the syringe. Alternatively, a single magnetic field sensor could also be used, which is moved up or down along the measuring section S.

[0046] The time course of the measured magnetic field is then transformed into the frequency domain. This can be carried out for individual frequencies e.g. by means of discrete Fourier transformation. The rotation frequency of the syringe 1 and its second harmonic (=double rotation frequency) are particularly relevant here. If the cannula 2 has a kink, the magnetic field is directed through it once per rotation in the direction of the magnetic field sensor arrangement 4.sub.A, i.e. closer to it, so that the magnetic field strength periodically increases and decreases at the rotation frequency. The distribution of the magnetic field along the cannula 2 will therefore have a larger maximum at the rotation frequency for the kinked tip than for a straight cannula 2. Also, due to the kink, there will be a different phase position of the magnetic field compared to the situation with a straight cannula 2. Based on the amplitude and/or phase position of the measured magnetic field, it is therefore possible to draw conclusions about the condition of the cannula 2, in particular when this is compared with the previously measured magnetic field in the vicinity of an intact, i.e. straight, reference cannula 2. The difference in the phase of the magnetic field at two spaced magnetic field sensors 4.sub.1□5 (e.g. two adjacent magnetic field sensors 4.sub.i & 4.sub.i-1 of the magnetic field sensor arrangement 4.sub.A) can also be used as the phase position.

[0047] During measurements, notice should be taken to avoid magnetic interference fields. For example, electric servomotors generate such interference fields, which are modulated with the speed of the servomotor. To minimize their influence on the measurements, a gear can be used, for example, so that syringe 1 rotates many times faster or slower than the servomotor. For example, if the speed of the servomotor is three times the speed of rotation of the syringe (i.e., gear ratio 3:1), the magnetic field to be measured at the rotation frequency of syringe 1 will be hardly disturbed by the interference field generated by the servomotor at three times the rotation frequency of syringe 1. Alternatively, a magnetic shield can be used to suppress magnetic interference fields.

[0048] Instead of using the earths magnetic field for the measurements, a magnetic field formed by an arrangement with one or more permanent magnets, or by an arrangement with one or more electromagnets, such as a Helmholtz coil, can also be used, wherein the arrangement can in particular also have one or more iron cores. In this way, for example, a strong homogeneous magnetic field can be generated.

[0049] FIG. 4. schematically shows a side view of such an embodiment variant with a Helmholtz coil. One coil each of the Helmholtz coil pair 7.sub.1, 7.sub.2 is arranged to the left and right of the cannula 2 to be inspected. A homogeneous, horizontally aligned magnetic field is formed between the two coils 7.sub.1, 7.sub.2, which (as in FIG. 3) can be measured with the magnetic field sensor arrangement 4.sub.A.

LIST OF REFERENCE NUMERALS

[0050] 1 Syringe

[0051] 2 Cannula, needle

[0052] 3 Cannula protective cap

[0053] 4.sub.1□5 Magnetic field sensor

[0054] 4.sub.A Magnetic field sensor arrangement with several magnetic field sensors

[0055] 5 Syringe holder

[0056] 6 Rotating device (optionally with lifting device)

[0057] 7.sub.1,2 Helmholtz coil

[0058] a Syringe longitudinal axis

[0059] F Magnetic field line

[0060] S Sensor line, measuring section