AU2003229121B2 - Measuring tissue mobility - Google Patents
Measuring tissue mobility Download PDFInfo
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- AU2003229121B2 AU2003229121B2 AU2003229121A AU2003229121A AU2003229121B2 AU 2003229121 B2 AU2003229121 B2 AU 2003229121B2 AU 2003229121 A AU2003229121 A AU 2003229121A AU 2003229121 A AU2003229121 A AU 2003229121A AU 2003229121 B2 AU2003229121 B2 AU 2003229121B2
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- tissue
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- mobility
- force
- oscillatory
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- 230000003534 oscillatory effect Effects 0.000 claims description 37
- 238000000034 method Methods 0.000 claims description 17
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- 238000012545 processing Methods 0.000 claims description 4
- JGFZNNIVVJXRND-UHFFFAOYSA-N N,N-Diisopropylethylamine (DIPEA) Chemical compound CCN(C(C)C)C(C)C JGFZNNIVVJXRND-UHFFFAOYSA-N 0.000 claims description 3
- 230000000007 visual effect Effects 0.000 claims 1
- 238000009527 percussion Methods 0.000 description 6
- 208000007123 Pulmonary Atelectasis Diseases 0.000 description 3
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- 241000239290 Araneae Species 0.000 description 1
- 206010003598 Atelectasis Diseases 0.000 description 1
- 241001465754 Metazoa Species 0.000 description 1
- 206010048334 Mobility decreased Diseases 0.000 description 1
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- Investigating Or Analysing Biological Materials (AREA)
Description
icT A, aoo3 Ioo q9 R~c~vd 1e-b oo h MEASURING TISSUE MOBILITY Field of the Invention This invention relates to a method of measuring tissue mobility. It relates particularly but not exclusively to a method of measuring tissue mobility by applying an oscillatory force to a region of tissue and measuring the velocity with which the tissue moves in response to the oscillatory force, and a system of doing the same.
Background to the Invention Percussion has been used routinely during chest examination for many years. Using this technique, a trained clinician is able to distinguish underlying clinical abnormalities by observing the characteristic sounds radiated in response to a sharp tap to the body surface at the point being examined. Using this technique, a great deal of information can be obtained which relates to the condition of the lung, abdominal and other organs. Clinical abnormalities such as complete lung collapse (pneumo-thorax), regional lung collapse (atelectasis) and gas trapping in the bowel can be detected.
When percussion is performed over different areas of the body, the sound radiated is variously described as dull (over the liver) or stony dull (associated with a pleural effusion) or as resonant (over the lung) or hyper-resonant (over the bowel). The mechanism by which the variation in radiated sound occurs is not fully understood. However, it seems likely that the observed "resonance" following percussion of the lung, bowel or other tissue results from the presence of gas, and that the high compliance of the gas decreases the mechanical damping of the overlying tissue. This has the effect of increasing the mobility of the overlying tissue and allowing it to resonate following the percussive tap. Conversely, where the subtissue environment contains principally fluid, the tissue damping will be increased and the mobility decreased, resulting in a "duller" percussive sound.
In infants, the tissue in the chest is highly compliant and percussion is more difficult to perform. This is in part due to the fact that the force delivered in each tap must be limited to avoid causing injury to the infant. Further, the adult finger that is used both as a coupling device and sounding board between the infant's body surface and the percussing finger is too large to be used in tiny infants. Currently, no method exists which can be safely applied to the newborn infant and which provides useful information similar to that which is obtained using traditional percussive techniques which are applicable for adults.
AMENDED SHEET
IPENAU
PeT/A aCO3 i 0o691 tRe_,. S reb ooq 2 Summary of the Invention According to a first aspect of the invention, there is provided a method of measuring tissue mobility including the steps of: applying an oscillatory force to a region of tissue using a vibrating mass having an oscillatory velocity u, and determining an oscillatory velocity u, with which the tissue moves in response to the applied force; wherein tissue mobility is determined by a ratio of the tissue velocity u t to the velocity of the vibrating mass, ii,.
The oscillatory force may be constant, or its frequency may vary over a period of time. Accordingly, the oscillatory force may consist of a series of discrete frequencies applied sequentially, or it may correspond to pseudo-random noise or white noise wherein a range of frequencies are applied simultaneously.
In a preferred embodiment, the oscillatory force is applied using a vibrating mass which is set in motion with an oscillatory velocity, The vibrating mass may be set in motion using an electromagnetic driver which is coupled to the tissue via a coupling device. In such an embodiment, the mobility of the tissue can be determined using: z1 20 zt(f =1 220f mf!! Mv mf where u t is the oscillatory velocity of the tissue which is coupled to the vibrating mass; m, is the mass of the vibrating mass; and m i f is the mass of the coupling device.
In an alternative embodiment, tissue transfer mobility may be determined. In such an embodiment, a force, oscillatory or otherwise, may be applied to a region of tissue and the velocity with which the tissue moves in response to that force is measured at a site which is spatially distinct from the point of force application.
Such a measurement may be useful for determining joint mobility in humans or other animals.
AMENDED SHEET
IPEA/AU
Pcl I Aac 66q1 3 According to a second aspect of the present invention, there is provided apparatus for measuring mobility of a region of tissue including: a force generator which drives a vibrating mass with an oscillatory velocity, u, for application of an oscillatory force to a region of tissue; tissue velocity determining means for producing a tissue velocity signal u, which corresponds to the velocity with which the tissue moves in response to the applied oscillatory force; and a processing device for processing the tissue velocity signal u, and the vibrating mass velocity signal, u,; wherein the tissue's mobility can be determined using a ratio of the tissue velocity, u t to the velocity of the vibrating mass, u,.
A single frequency may be applied over a period of time, or the frequency may be varied sequentially. Alternatively many different frequencies may be applied simultaneously in the form or pseudo-random noise or white noise. The oscillatory force generator may be a magnet supported within a set of concentric field coils, the field coils being driven with a swept frequency current. However, any other appropriate force-generating device suitable for generating an oscillatory force could be used.
It is preferred that the oscillatory force generator is a vibrating mass which is set in motion with an oscillatory velocity, This may be achieved using an electromagnetic driver as described, which is coupled to the tissue using a coupling device. Accordingly, the mobility of the tissue can be determined using the equation: zt 1 2;f !t m v Mf SUt where u, is the oscillatory velocity of the tissue which is coupled to the vibrating mass; inm is the mass of the vibrating mass; and mf is the mass of the coupling device.
AMENDED SHEET IPPIA/AI I Pcr AJlccIql ~Cc1 VSez 2c~u~ 4 In another embodiment, the apparatus may be used to determine tissue transfer mobility, wherein the oscillatory velocity at which the tissue moves in response to the applied force is measured at a location which is spatially distinct from the region of tissue to which the oscillatory force is applied.
The apparatus may also include a display device for displaying a representation of mobility of the region of tissue, wherein the representation of mobility includes a graph of mobility versus frequency.
The character of the sound which is radiated following percussion is determined, at least in part, by the mechanical mobility and resonant frequency of the tissue interface at the percussion site. This is, in turn, influenced by the damping effect of underlying fluid or gas. Accordingly, the apparatus of the present invention, which is designed to measure mobility as a function of frequency, is likely to be of clinical value.
The present invention provides an advantage in that it requires the use of a smaller peak force than is applied with the impulse method for determining tissue mobility. Accordingly, it is safer for use in infants. A further advantage of the present invention over traditional percussive techniques is that it is less dependent on the clinical experience of the practitioner and does not require a quiet environment.
Brief Description of the Drawings The invention will herein after be described in greater detail by reference to the attached drawings. It is to be understood that the particularity of the drawings does not supersede the generality of the preceding description of the invention.
Figure 1 illustrates a transducer for use in an embodiment of the invention where an oscillatory force is applied to the tissue.
Figure 2 indicates tissue mobility in a plot of Mobility (mm.sl.N 1 against Frequency (Hz).
Detailed Description In principle, mobility can be measured by applying an impulsive force to tissue and examining the temporal change in velocity that follows. However, AMENDED
SHEET
WO 03/101295 PCT/AU03/00691 equivalent information can also be obtained by using a smaller oscillatory force.
This is preferable for testing tissue mobility in infants, as the highly compliant tissue of an infant's chest can withstand low magnitude oscillating forces, whereas single impulse forces which are applied in adult percussive techniques are likely to cause injury.
In the preferred embodiment illustrated in Figure 1, a small oscillatory force is applied to the surface of the tissue using a broad range of frequencies which are.applied for a burst of approximately 5 seconds, although the burst of frequencies may last for a longer or a shorter period. Mobility can then be determined at each frequency by measuring simultaneously the applied oscillatory force and the resultant tissue velocity. The frequencies may be applied sequentially, or simultaneously in the form of pseudo-random or "white" noise. When pseudo-random frequencies are used, a range of frequencies are applied at once. Accordingly, the mobility of the tissue can be determined more quickly.
Referring to the illustration in Figure 1, a vibrating mass 102 of mass in is set in motion using an electromagnetic driver. The force generated by the acceleration of vibrating mass 102 appears as a reactive force. This reactive force is coupled via coupling device 104 to tissue 106, the mobility of which is being tested. In the example illustrated in Figure 1, coupling device 104 is a light-weight frame, the mass of which includes the mass of field coils 114 which are used to excite vibrating mass 102. Tissue velocity transducer 108 is used to measure the velocity, of tissue 106 which is in contact with frame 104.
Vibrating mass velocity transducer 110 is used to measure the velocity, of the vibrating mass. However, tissue velocity transducer 108 and vibrating mass velocity transducer 110 may measure acceleration from which a value for velocity may be derived mathematically.
In such an embodiment, where an oscillatory force is applied to tissue 106, it can be shown that the magnitude of the combined mobility of tissue 106 and frame 104, as a function of frequency denoted by z,(f)can be determined using the following expression.
U U (equation 1) FSC 2funmv WO 03/101295 PCT/AU03/00691 6 where: is the oscillatory force applied to tissue 106; in, is the mass of vibrating mass 102; and f is the frequency of oscillation.
By using the known mass of frame 104, it is possible to deduce the mobility of tissue 106 alone, denoted by z, using the following expression: 1 zt (equation 2) 2af Unmv mf} Ut where: mf is the mass of frame 104.
In general z,(f)is a complex value and its phase varies with frequency.
Energy is stored in tissue as a consequence of its mass and stiffness.
This results in the presence of resonant frequencies which may then be used to characterise different parts of the body's surface. Accordingly, analysis of the magnitude and phase of mobility as a function of frequency can give information about the nature of the tissue under test. Therefore, periodically measuring tissue mobility and monitoring the changes in tissue mobility with time may indicate the presence or development of underlying disease and/or may be used to identify changes in the fluid or gas content of the underlying tissue.
In the embodiment of Figure 1, reactive mass 102 is a cylindrical magnet forming part of a motor assembly. Reactive mass 102 is suspended on two flexible spider supports 112 within a concentric set of field coils 114. Field coils 114 are driven with a swept frequency current so that the reactive mass 102 is set in motion at the driving frequency. The reactive force generated by the motion of the reactive mass 102 is coupled to tissue 106 via frame 104 as previously described.
In the embodiment of Figure 1, tissue velocity transducer 108 and vibrating mass transducer 110 are accelerometers. The output from these WO 03/101295 PCT/AU03/00691 7 accelerometers is sent to a processor where the magnitude and phase of the tissue mobility is calculated using equation 2 and then displayed. A typical display of values which are obtained in a mobility measurement in accordance with the present invention is shown in Figure 2.
It is to be understood that a number of other motor types could be used to provide vibrating mass 102. These motor types include but are not limited to electrostatic and pneumatic types. Further, the size of the part of the apparatus which contacts the tissue is readily scalable for different applications in both paediatric and adult medicine, depending on the types of transducers used.
Moreover, it is to be understood that, by characterising the motor or by using electronic feedback to regulate the velocity of vibrating mass 102, it is possible to eliminate vibrating mass velocity transducer 110, thereby simplifying the apparatus. In a further adaptation, tissue velocity transducer 108 may be made mobile so that the mobility of tissue at one part of the body can be measured in response to vibration at a spatially different part of the body, providing a measurement of tissue transfer mobility.
The present invention may also be used to measure and/or analyse tissue impedance, Zt(f), where impedance is the inverse of tissue mobility, z, as shown in equation 3.
1 Z, (equation 3) z, (f) Various alterations, additions and/or modifications may be made to the parts previously described without departing from the ambit of the present invention.
Claims (9)
1. A method of measuring tissue mobility including the steps of: applying an oscillatory force to a region of tissue using a vibrating mass having an oscillatory velocity um; and determing an oscillatory velocity u, with which the tissue moves in response to the applied force; wherein tissue mobility is determined by a ratio of the tissue velocity u t to the velocity of the vibrating mass, ur.
2. A method of measuring tissue mobility according to claim 1 wherein the frequency of the oscillatory force is varied over a period of time.
3. A method of measuring tissue mobility according to claim 1 or claim 2 wherein the oscillatory force corresponds to pseudo-random noise or white noise.
4. A method of measuring tissue mobility according to any preceding claim wherein the force is applied using a vibrating mass which is set in motion, with oscillatory velocity u,,m using an electromagnetic driver which is coupled to the tissue via a coupling device. A method of measuring tissue mobility according to claim 4, wherein the mobility of the tissue, z t is given by: 25 1 zt(f) 1 2t 7 fmv mf where nm, is the mass of the vibrating mass; and mi is the mass of the coupling device.
6. A method of measuring tissue mobility according to any preceding claim wherein the velocity at which the tissue moves in response to the applied force AMENDED SHEE IPEA/AU crA cO joc 69 Rcce, _5 eb ccl, 9 is determined at a location which is spatially distinct from the region of tissue to which the force is applied.
7. A method of measuring tissue mobility according to any preceding claim including the additional step of providing a visual representation of the velocity at which the tissue moves in response to the applied force.
8. Apparatus for measuring mobility of a region of tissue including: a force generator which drives a vibrating mass with an oscillating velocity u t for application of an oscillatory force to a region of tissue; tissue velocity determining means for producing a tissue velocity signal u t which corresponds to the velocity with which the tissue moves in response to the applied oscillatory force; and a processing device for processing the tissue velocity signal u t and the vibrating mass velocity signal wherein the tissue's mobility can be determined using a ratio of the tissue velocity u t to the velocity of the vibrating mass, um.
9. Apparatus for measuring tissue mobility according to claim 8 wherein the force generator is a vibrating mass which is set in motion with an oscillatory velocity u.n, using an electromagnetic driver which is coupled to the tissue via a coupling device. Apparatus for measuring tissue mobility according to claim 9, wherein the mobility of the tissue, z t at a frequencyf is given by: 1 z t (f)
27.f Ut M 2a' m v mf} where Mn~ is the mass of the vibrating mass; and mf is the mass of the coupling device. AMENDED SHEEI IPPIAl I f--ij AJ~y-? 10069 Recd 25 2^ 2coLe 11. Apparatus for measuring tissue mobility according to any one of claims 8 to 10 wherein the force generator applies an oscillatory force to a region of tissue which is spatially distinct from the location of the tissue velocity determining means. 12. Apparatus for measuring tissue mobility according to claim 10 or claim 1'1 further including a display device for displaying a representation of mobility of the region of tissue, wherein the representation of mobility includes a graph of mobility versus frequency. AMENDED SHEET IPEA/AU
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| AU2003229121A AU2003229121B2 (en) | 2002-06-03 | 2003-06-03 | Measuring tissue mobility |
Applications Claiming Priority (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| AUPS2741 | 2002-06-03 | ||
| AUPS2741A AUPS274102A0 (en) | 2002-06-03 | 2002-06-03 | Measuring tissue mobility |
| AU2003229121A AU2003229121B2 (en) | 2002-06-03 | 2003-06-03 | Measuring tissue mobility |
| PCT/AU2003/000691 WO2003101295A1 (en) | 2002-06-03 | 2003-06-03 | Measuring tissue mobility |
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| Publication Number | Publication Date |
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| AU2003229121A1 AU2003229121A1 (en) | 2003-12-19 |
| AU2003229121B2 true AU2003229121B2 (en) | 2007-05-24 |
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| AU2003229121A Ceased AU2003229121B2 (en) | 2002-06-03 | 2003-06-03 | Measuring tissue mobility |
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| AU (1) | AU2003229121B2 (en) |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO1997000643A1 (en) * | 1995-06-23 | 1997-01-09 | Trustees Of The Stevens Institute Of Technology | Non-invasive technique for bone mass measurement |
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Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO1997000643A1 (en) * | 1995-06-23 | 1997-01-09 | Trustees Of The Stevens Institute Of Technology | Non-invasive technique for bone mass measurement |
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| AU2003229121A1 (en) | 2003-12-19 |
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