GB2099155A - Goniometer - Google Patents

Goniometer Download PDF

Info

Publication number
GB2099155A
GB2099155A GB8208679A GB8208679A GB2099155A GB 2099155 A GB2099155 A GB 2099155A GB 8208679 A GB8208679 A GB 8208679A GB 8208679 A GB8208679 A GB 8208679A GB 2099155 A GB2099155 A GB 2099155A
Authority
GB
United Kingdom
Prior art keywords
sensors
section
goniometer
goniometer according
flexible
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
GB8208679A
Other versions
GB2099155B (en
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
National Research Development Corp UK
National Research Development Corp of India
Original Assignee
National Research Development Corp UK
National Research Development Corp of India
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by National Research Development Corp UK, National Research Development Corp of India filed Critical National Research Development Corp UK
Priority to GB8208679A priority Critical patent/GB2099155B/en
Publication of GB2099155A publication Critical patent/GB2099155A/en
Application granted granted Critical
Publication of GB2099155B publication Critical patent/GB2099155B/en
Expired legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B7/00Measuring arrangements characterised by the use of electric or magnetic techniques
    • G01B7/16Measuring arrangements characterised by the use of electric or magnetic techniques for measuring the deformation in a solid, e.g. by resistance strain gauge
    • G01B7/18Measuring arrangements characterised by the use of electric or magnetic techniques for measuring the deformation in a solid, e.g. by resistance strain gauge using change in resistance
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B7/00Measuring arrangements characterised by the use of electric or magnetic techniques
    • G01B7/30Measuring arrangements characterised by the use of electric or magnetic techniques for measuring angles or tapers; for testing the alignment of axes

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measurement Of The Respiration, Hearing Ability, Form, And Blood Characteristics Of Living Organisms (AREA)

Abstract

A goniometer for use in measuring angular movements of a joint of a human or animal body comprises an elongate body (1, 2, 3, 6) and at least two mercury-in-rubber sensors (5a, 5b, 5c, 5d) extending longitudinally of the body at locations spaced from one another around the body. The electrical resistance of the sensors varies with varying strain thereof, and a circuit (20) is connected to the sensors for converting variations in the resistance into a measure of the relative angular disposition of the ends of the body. Rotational disposition may also be measured using the mercury-in-rubber sensors e.g. over section 6 of the elongate body, or by replacing the section 6 with a rotary potentiometer. <IMAGE>

Description

SPECIFICATION Goniometer This invention relates to a goniometer, and in particular to a goniometer for use in measuring angular movements of joints of a human or animal body.
It is frequently desired to measure the angular movements of a joint of the body, for example in studying changes in behaviour of a joint after an operation. At present no convenient way exists of doing this, and an object of the invention is to remedy this.
According to the invention there is provided a goniometer comprising an elongate body, a plurality of sensors extending longitudinally of the body, at locations spaced from one another around the body, the sensors being such that an electrical property thereof varies with varying strain thereof, and a circuit connected to the sensors for converting variations in the said electrical property into a measure of the relative angular disposition of the ends of the body.
In the accompanying drawings: Figure 1 is a diagrammatic perspective view of an embodiment of the invention; Figure 2 shows part of one modification of the embodiment of Figure 1; and Figure 3 shows part of another modification of the embodiment of Figure 1.
The goniometer illustrated in Figure 1 comprises a rod of thermoplastic material 10 mm in diameter and 240 mm in length. 50 mm lengths 1 and 2 at either end remain rigid and are the sections which are attached to the parts of the body whose rotations are to be measured. The central section 3 of the rod is made flexible by a large number of slots cut into it. The slots are cut in pairs across the rod from opposite sides, each pair leaving a web 4 across the diameter. Adjacent pairs of slots are cut at 900 to each other. This makes the rod very flexible to bending forces in any direction but resistant to torsion about its longitudinal axis. One of the end sections 2 is separate from the rest of the rod and is able to rotate about its long axis.
Transducer elements are provided in the form of four mercury-in-rubber gauges 5a, Sb, Sc and 5d. Each gauge consists of a fine tube of rubber (either natural or synthetic) or similar material, filled with mercury. To protect the gauges the rod is covered with a thin latex tube, of which a portion is shown. The gauges lie in grooves cut along the length of the rod and equally spaced around its circumference. They are attached to the end sections 1 and 2 of the rod and bending in the flexible central section 3 causes differing length changes in the gauges, thereby changing their electrical resistance. From these changes the angle through which the rod bends and the plane in which it does so is derived. This can be achieved by an appropriate electronic circuit 20 connected to the gauges.Thus, the ends of the gauges which terminate in section 2 can be electrically connected together, and circuitry connected to the other ends of the gauges determines the difference between the resistance of gauges 5a and 5c, and the difference between the resistance of gauges Sb and 5d.
If bending takes place about an axis perpendicular to the plane containing gauges 5a and 5c, the length of one of those gauges increases (and consequently its resistance increases) and the length of the other decreases (and consequently its resistance decreases). The gauges Sb and Stare unchanged in length. The changes in the gauges 5a and Sc are interpreted by the electronic circuit as bending of a given amount about the above mentioned axis. The gauges 5b and 5d act correspondingly in the case of bending about an axis perpendicular to the plane containing them. Bending about an axis intermediate the two aforementioned axes causes measurement of the two components of that bending about those two axes.Any bending of the rod in which the two end sections remains parallel leaves the length of the gauges unchanged, and the goniometer is thus unaffected by linear movements of the two ends.
For a 1 5 mm length 6 adjacent the end section 2 the gauges do not lie in grooves but lie on the surface thereof. In the drawings the gauges are shown as extending over this section parallel to the longitudinal axis of the goniometer, but it is preferred that the gauges should be given a spiral twist, for example through 1 800, over the length 6. The length 6 is designed to measure rotation, and in order to assist this the length is preferably cut into a plurality of discs 7 each of which has a central aperture, the disc being carried on a central rod (not shown).
If a torsional force is exerted on the goniometer, the end section 2 rotates about its longitudinal axis with respect to the sections 1 and 3. This causes the gauges to spiral round the length 6 (or, where those gauges already lie in the form of a spiral, causes the angle of that spiral to change), thereby increasing the length of each gauge by the same amount. The electronic circuit 20 connected to the guages detects this increase in resistance and interprets it as torsional movement through a given angle.
Various modifications may be made to the goniometer described above. For example, bending may be measured using just two gauges disposed at 900 to one another. Torsional movement can be detected by a third gauge which is free to spiral around the rod as torsional movement occurs. Another possibility is to use just two gauges at 900 to one another to detect both bending and torsional movement, this being achieved by tapping the gauges at the junction between sections 3 and 6 so as to be able to determine separately the components of electrical resistance attributable to the portions of the gauge on either side of the tapping points.
Another modification is shown in Figure 2.
Here, the torsional movement is measured by a separate rotary potentiometer 9 mounted in place of section 6 with the body of the potentiometer 1 0 rigidly attached to section 3 and its rotating spindle 11 rigidly attached to section 2. In this case the gauges 5 terminate at the end of section 3 and are used to measure the bending movements of section 3 only. In this modification use can be made of just two gauges spaced at 900 from one another, though four gauges may be preferred from the point of view of providing temperature compensation.
Yet another modification is shown in Figure 3 which illustrates how the flexible section 3 may be constructed from a number of separate elements.
Each eiement consists of a rigid disc 12, say 10 mm diameter and 2 mm in thickness. On one face of the disc is a ridge 1 3 2 mm in height on the diameter. On the other face is a correspondingly shaped groove 1 4 1 mm deep also on the diameter but oriented at 90" to the ridge. In each disc there are four holes 15 a short distance from the edge of the disc and equally spaced around its circumference to hold the mercury-on-rubber gauges and a larger central hole 1 6. To construct the flexible section 3 a large number of the discs are threaded onto a spiral spring 17, the ridge on each disc fitting into the groove on the adjacent one. The discs are kept in contact by tension applied to the central spring.
The output of the electronic circuit referred to above may be fed to any suitable means for recording and/or displaying the output in a suitable form. For example, the output of the electronic circuit may be displayed on an oscilloscope or on a pen-and-paper recorder.

Claims (14)

1. A goniometer comprising an elongate body, a plurality of sensors extending longitudinally of the body, at locations spaced from one another around the body, the sensors being such that an electrical property thereof varies with varying strain thereof, and a circuit connected to the sensors for converting variations in the said electrical property into a measure of the relative angular disposition of the ends of the body.
2. A goniometer according to claim 1, wherein the elongate body comprises non-flexible end sections and a flexible section intermediate the end sections, the sensors being secured at one end to one of the end sections and at the other end to the other end sections.
3. A goniometer according to claim 2, wherein the said flexible section has a plurality of pairs of diametrically opposed slots formed thereon, the pairs of slots being spaced longitudinally from one another along the length of the said flexible section.
4. A goniometer according to claim 3, wherein adjacent pairs of slots are orientated at 900 with respect to each other.
5. A goniometer according to any preceding claim, wherein the sensors are in the form of flexible tubes filled with mercury, the electrical resistance of the sensors varying with varying strain thereof.
6. A goniometer according to any preceding claim, wherein four sensors are arranged 900 apart from one another around the said body.
7. A goniometer according to claim 6, wherein the said circuit is arranged to determine the difference in resistance between gauges 1 800 apart, thereby to determine bending of the said body.
8. A goniometer according to claim 2, wherein one of said end sections is free to rotate relative to the said flexible section.
9. A goniometer according to claim 8, which comprises a further section intermediate the flexible section and the rotatable end section, and wherein the sensors run in grooves formed in the surface of the flexible section but do not run in grooves over the said further section, whereby the sensors are free to spiral around the said further section upon rotation of the said rotatable end section, the said spiralling serving as a measure of torsion of the said body.
10. A goniometer according to claim 8, which comprises at least two sensors arranged 900 apart from one another around the said body to detect bending, and a means other than the said two sensors for detecting torsion.
11. A goniometer according to claim 10, wherein the said meansfordetecting torsion comprises a potentiometer having a first member in the form of a body portion and a second member rotatable with respect thereto, one of the members being secured to the flexible section of the said elongate body and the other of the member being secured to the rotatable end section of the elongate body.
12. A goniometer according to claim 2 or any one of claims 5 to 11, as dependent on claim 2, wherein the flexible section comprises a plurality of interengaging discs held together by a resiiient member.
13. A goniometer according to claim 12, wherein each disc has a diametral ridge on one side thereof and a diametral groove on the other side thereof, the ridge and groove being at 900 to one another, the ridge of each disc interengaging with the groove on an adjacent disc.
14. A goniometer substantially as herein described with reference to Figure 1 of the accompanying drawings, with or without the modification of Figure 2 or Figure 3.
GB8208679A 1981-03-27 1982-03-24 Goniometer Expired GB2099155B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
GB8208679A GB2099155B (en) 1981-03-27 1982-03-24 Goniometer

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
GB8109663 1981-03-27
GB8208679A GB2099155B (en) 1981-03-27 1982-03-24 Goniometer

Publications (2)

Publication Number Publication Date
GB2099155A true GB2099155A (en) 1982-12-01
GB2099155B GB2099155B (en) 1985-01-16

Family

ID=26278913

Family Applications (1)

Application Number Title Priority Date Filing Date
GB8208679A Expired GB2099155B (en) 1981-03-27 1982-03-24 Goniometer

Country Status (1)

Country Link
GB (1) GB2099155B (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1986001588A1 (en) * 1984-09-01 1986-03-13 University Of Strathclyde Electrical angular displacement sensor
EP0287149A2 (en) * 1987-03-31 1988-10-19 Hendrikus Herman Schutte Angle measuring device

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1986001588A1 (en) * 1984-09-01 1986-03-13 University Of Strathclyde Electrical angular displacement sensor
EP0287149A2 (en) * 1987-03-31 1988-10-19 Hendrikus Herman Schutte Angle measuring device
EP0287149A3 (en) * 1987-03-31 1990-12-12 Hendrikus Herman Schutte Angle measuring device

Also Published As

Publication number Publication date
GB2099155B (en) 1985-01-16

Similar Documents

Publication Publication Date Title
CA1179123A (en) Goniometer
EP0192694B1 (en) Electrical angular displacement sensor
US3991745A (en) Curvature measurement device
EP1052472B1 (en) Constant pressure mechanism of probe
US3602866A (en) Force transducer
US2316975A (en) Gauge
US6324918B1 (en) Bidirectional force sensor
US4651436A (en) Probe for measuring deviations from linearity
JPH0419862B2 (en)
DE4244189A1 (en) Contact temperature sensor
US3908279A (en) Curvature measurement device
JPH0449644B2 (en)
JP2007500361A (en) Improved deflection system for strain-based instruments
US5070622A (en) Dimension measuring device
US4910877A (en) Tube curvature measuring probe and method
GB2099155A (en) Goniometer
US4053985A (en) Mechanical protractor
US4145921A (en) Vorticity probe utilizing strain measurements
US3995476A (en) Miniature biaxial strain transducer
US4472976A (en) Apparatus for measuring at least one component of the forces applied to a beam
US5044084A (en) Angle sensor element
CN113587842A (en) Shape detection device of superfine endoscope insertion tube and detection sensor manufacturing method
JPS61240133A (en) Torque detector
JPH0972795A (en) Torque sensor
JPS625103A (en) Twist angle gauge

Legal Events

Date Code Title Description
PCNP Patent ceased through non-payment of renewal fee