This invention relates to medical spirometers, in particular to spirometers using fluidic elements for measurement
Medical spirometers are used for testing/measuring respiratory functions of humans, including instant flow rate during respiration (peak-flow meters) and total volume discharge or vital capacity. Fluidic elements, such as fluidic oscillators are known for their stability, linear characteristics and reliability, and are used in such spirometers.
U.S. Pat. No. 3,714,828 describes a device for measuring the pulmonary function of a patient, comprising a fluid oscillator and a digital counter. In one embodiment, a sample of the flow is diverted by a Pitot tube to the fluid oscillator. The device is designed for measuring expiratory gases from a hospital patient who has been given a volatile anesthetic.
U.S. Pat. No. 4,182,172 discloses a flow meter of fluidic oscillator type designed for measuring the ventilation of a moving human being or an animal. The flow meter is small, light and portable. The pressure drop is described as minimal but the whole flow passes through the oscillator. The flow oscillations are detected by a suitably disposed ultrasonic transmitter and receiver.
U.S. Pat. No. 4,930,357 describes a volumetric flow meter comprising a fluidic oscillator and a plurality of parallel fluid flow bypass channels. Each channel has a special flow restriction to obtain pressure drop equal to the one across the oscillator for easier calculation of the total flow. The oscillating pressure in the feedback channels of the oscillator is measured by two sensing chambers connected to the feedback channels and closed by diaphragms with transducers thereon. The other side of the diaphragms is exposed to the atmosphere.
In accordance with one aspect of the present invention, there is provided a medical spirometer comprising a housing with a flow inlet and a flow outlet and a measurement unit (MU) for measuring rate of total flow between the inlet and the outlet when a user exhales through the spirometer. The MU comprises one fluidic jet oscillator adapted to generate oscillating flow characterized by an oscillating parameter with frequency dependent on rate of flow through said jet oscillator, and a transducer adapted to convert said oscillating parameter into an oscillating electric signal. The fluidic oscillator may be implemented as a sandwich of two or more parallel jet oscillators for obtaining stable osclillations.
The MU is disposed within the housing so as to form a bypass flow path defined between an outer surface of the MU and an inner surface of the housing. A measurement flow path is defined through the fluidic jet oscillator such that the total flow is divided into a bypass flow and a measurement flow.
The measurement flow rate may be less than the bypass flow rate at least by an order of magnitude. Preferably, the bypass flow path is free of obstructions increasing its pressure drop.
The spirometer may be a pocket-size stand-alone device or a miniature instrument used in mobile or stationary measurement circuits.
The MU further comprises an electronic circuit (processor) adapted to measure the frequency of the oscillating signal and to derive the total flow rate therefrom. Preferably, the electronic circuit is adapted to store coefficients obtained in previous calibration of the spirometer and to use them for deriving the total flow rate. Preferably, the electronic circuit is adapted to measure the frequency by counting pulses of the oscillating parameter.
The electronic circuit may be further adapted to integrate the total flow rate, thereby measuring the total flow volume per predetermined time.
The oscillating parameter may be the flow velocity which can be measured by a hot wire. Alternatively, the oscillating parameter may be the flow pressure which can be measured by a pressure transducer.
Preferably, the pressure transducer is of differential type, for example with a chamber divided by a flexible membrane and a piezoelectric element mounted on the membrane. The jet oscillator has two feed-back channels, each with a pressure port, and one of the pressure ports is connected to one side of the membrane, while the other of the pressure ports is connected to the other side of the membrane. Thus the registration of each pulse is facilitated as the pressures in the feed-back channels oscillate in opposing phases.
The spirometer may comprise valve means such that a measurement flow through the jet oscillator is created also when the user inhales through the spirometer, thereby enabling measuring of total flow rate at inhale. Alternatively, the jet oscillator or the MU can be made movable to assume a second position with respect to the housing, such that a measurement flow through the jet oscillator would be created when the user inhales.
The MU may comprise a second fluidic jet oscillator similar and parallel to the first one but oppositely orientated and defining a second measurement flow path within the MU, such that a second measurement flow is created when the user inhales through the spirometer. The spirometer further may comprise valve means such that the first measurement flow path is open only when the user exhales while the second measurement flow path is open only when the user inhales. The valve means may include one check valve associated with the first measurement flow path and one check valve associated with the second measurement flow path.
The second jet oscillator may be connected to the same pressure transducer as the first jet oscillator, so that the MU may have no other pressure transducers.
Alternatively, the spirometer may comprise a second transducer adapted to convert an oscillating flow parameter of the second jet oscillator into a second oscillating electric signal. In a variation of this embodiment, the first and second measurement flow paths have no valve means and are open both when the user inhales and exhales, such that at exhaling the first jet oscillator works in straight flow while the second jet oscillator works in reverse flow and vice-versa. The electronic processor is adapted to recognize whether the user inhales or exhales by different patterns of the respective first and the second oscillating signals.
The signal patterns may differ in that at exhaling the first (straight) oscillating signal has regular pulse structure while the second (reverse) oscillating signal is irregular (hereinafter ‘noise’). The front edge of the recognizable first pulse in the first oscillating signal comes before the noise is recognized, which is used by the processor for the distinction between the signals. Correspondingly, at inhaling the second oscillating signal has regular pulse structure while said first oscillating signal is noise, the front edge of the first pulse in the second oscillating signal coming before the noise.
The spirometer further may comprise a means to display flow measurement results to the user.
The spirometer may comprise means for storing measurement data and communicating the data to an external device, preferably bi-directionally.
The communication means may include interface to a cellular phone enabling transmission of the data through the cellular phone network. The spirometer housing may be designed for mounting to the housing of the cellular phone. The spirometer may further include program means transferable to or resident in the cellular phone allowing to display flow measurement results on the display of the cellular phone. Alternatively, the spirometer may include a built-in cellular phone enabling transmission of the data through a cellular phone network.
The spirometer may further comprise means for identifying a medical condition using the flow measurement results, and for warning the user. The spirometer further comprises input means for entering personal data of the user, which data may be used for identifying the medical condition. The spirometer may also comprise means for suggesting preventive measures to the user upon identifying the medical condition.
The spirometer may be designed to have a housing adapted to accommodate a dispenser with medicine for inhaling. The housing preferably has a channel for delivery of the medicine to the user's mouth, connecting an outlet of the dispenser to the flow inlet.
The bypass channel may be formed as an annular channel with the delivery channel opening within the bypass channel, for forming a jet of dispersed medicine in the core of the airflow.
The spirometer may further comprise a second fluidic jet oscillator defining a second flow path such that a second oscillating flow is created when the user inhales through the spirometer. The medicine delivery channel may then connect the outlet of the dispenser to the inlet of the second jet oscillator, such that the medicine passes through the second flow path for enhanced mixing. A surrounding bypass channel may be formed in the body of the second fluidic jet oscillator.
According to another aspect of the present invention, there are provided inhaler-dispenser devices with improved aerodynamic features.
One example of such inhaler-dispenser comprises a housing adapted to accommodate a dispenser with medicine for inhaling. The housing further has an inhaling passage with inlet air opening and outlet mouthpiece such that upon inhaling, airflow runs from the inlet to the outlet, this housing further having a delivery channel for delivery of the medicine into the airflow. An outlet end of the delivery channel is disposed such that, at inhale, a dose of said medicine is delivered to a central core of the airflow.
The inhaling passage may include a fluidic jet oscillator with an inlet connected to the inlet opening and an outlet connected to the mouthpiece, the delivery channel opening into the inlet of the fluidic jet oscillator, for enhanced mixing of the medicine. An annular bypass channel may be formed in the body of the fluidic jet oscillator such that, upon inhaling, the outlet jet flow of the fluidic jet oscillator carrying said medicine is surrounded by a parallel flow through the bypass channel.
According to a still further aspect of the present invention, there is provided a method for measurement of a user's inhale and exhale rate of flow by means of two fluidic jet oscillators, each having an inlet and an outlet defining ‘straight’ flow direction used for measurement, and defining an inoperative ‘reverse’ flow, and adapted to generate oscillating flow characterized by an oscillating parameter dependent on rate of straight flow through the jet oscillator, with two respective transducers used to convert the oscillating parameters into oscillating electric signals having different signal patterns for ‘straight’ and ‘reverse’ flows. The method comprises:
The pattern difference may be in that the ‘reverse’ oscillating signal is noise while the ‘straight’ oscillating signal has regular pulse structure with the front edge of the first pulse coming before the noise.
The spirometer of the present invention may have miniature size, minimum pressure drop (no obstructions to breathing during measurement), precise and simple digital measurement (count of pulses), temperature independence, cheap production, convenient usage, disinfection and practically no maintenance. The spirometer may be handy, easy to carry around, for example as a key-holder, yet robust and reliable. It can be integrated with other pocket-size objects like mobile phones or medicine dispensers.
In order to understand the invention and to see how it may be carried out in practice, different embodiments will now be described, by way of non-limiting examples only, with reference to the accompanying drawings, in which:
With reference to
With reference also to
The fluidic pulse generator 28 is a bi-stable jet element with positive feedback. With reference to
With reference to
The output of the electronic processor 32 is connected to the input of the indicator block 34 where the measured airflow rate and/or volume is presented by a suitable indication—as a color, number, geometrical, or another code.
In operation when conducting a test on the respiratory function of a patient, the exhaled air enters the inlet port 14 of the housing 12 and the airflow passes through the bypass channels 22, 24. A small portion of the airflow—measurement flow—enters the fluidic pulse generator 28 through the measurement inlet 26. The measurement airflow enters the inlet nozzle 42 and then the diffuser 44. In accordance with the Coanda effect, the air jet in the diffuser 44 sticks with one of the walls, for example 46, and proceeds towards the outlet channel 54. Part of the jet enters the feedback channel 50 and returns back to the inlet of the diffuser 44. This part of the jet disturbs (turbulizes) the boundary layer on the wall 46. As a result, the air jet is detached from the wall 46 and jumps to the opposite wall 48. Now a part of the jet enters the opposite feedback channel 52 and the cycle is repeated. The frequency of these jet swaps is roughly proportional to the flow rate through the FPG.
The pressure differential between the pick-up ports 58 and 60, which oscillates with the same frequency, is converted into oscillating electric signal by the piezoelement 68 in the pneumo-electric transducer 30. The oscillating signal is then fed to the electronic processor 32 for calculation of the flow rate and the total flow volume for a given time. The obtained data are sent to the indicator block 34 for display to the user.
A quantitative measure of the airflow rate and/or the volume of air passing through the spirometer is obtained in the electronic processor 32. Assuming that the relationship between the measured frequency generated in the FPG and the total flow rate through the spirometer is linear, a “pulse weight” coefficient Pw may be obtained by calibration of the spirometer. Methods of flow meters calibration per se are known in the art of aerodynamics. The Pw coefficient determines the volume of air passing through the spirometer as a whole (bypass channels and the FPG) per one pulse of the generated frequency. Thus, by counting the number of pulses, the whole volume of air passing through the spirometer for a predetermined time may be calculated, as well as the volume passing for a unit of time (flow rate).
Alternatively, if the above relationship is not assumed linear, then the Pw coefficient will be a function of the frequency. The non-linear relationship may be described by more coefficients obtained by calibration and stored in the electronic processor 32. Methods of non-linear calibration are also known per se.
Generally speaking, the proportion between the rate of the measurement flow passing through the FPG and the bypass flow rate is also dependent on the total flow rate. In the area of industrial/utility gas flow meters, attempts to keep this proportion constant have been made by dividing the bypass channel into a plurality of narrow channels, each with pressure drop equal to the pressure drop of the FPG However, this leads to a high total pressure drop which is not desirable in spirometry.
The spirometer may further include storage (memory) for measurement data and a communication device such as IR port or radio-frequency device (for example BlueTooth) for data exchange with an external device such as personal computer, preferably bi-directionally. Thus the measurement data mat be transferred over the internet and used in telemedicine. The communication device may include interface (wired or wireless) to a cellular phone enabling transmission of the data through the cellular phone network. Moreover, the miniature size of the spirometer allows its housing to be designed for mounting to the housing of a cellular phone. Alternatively, the spirometer and the cellular phone may be accommodated in an integral housing. Such combined device may share common microprocessor, software and display.
According to another embodiment of the present invention shown in
With reference to
The inlet and outlet channels of the two FPGs 28, 108 are located opposite the ports 94 and 96 of the housing, in mutually opposing directions. Each FPG has a check valve connected to it, such that FPG 28 with check valve 112 operates during exhale, while the FPG 108 with check valve 114 operates during inhale.
As shown in
A scheme where each FPG has its own transducer, may work without check valves 112, 114, the inlet and outlet channels of both FPGs being always open. When, for example, the user exhales, the FPG 28 operates in its normal mode (straight flow) generating regular pressure pulses. The FPG 108 will also operate but in reverse flow, creating noise instead of regular pressure pulses. Similarly, if the user inhales, the FPG 108 will operate in its normal mode, while the FPG 28 will create noise. The front edge of the first regular pulse always comes before the noise—thus the processor 32 can always identify which of the FPGs is working in normal mode, i.e. whether the user is inhaling or exhaling. Accordingly, the processor will select the identified FPG for further measurement, until the flow through the spirometer keeps its direction.
According to another embodiment of the present invention, the jet spirometer may include a medicine dosage dispenser. With reference to
After making a measurement and reading the display 34, the patient may immediately and conveniently inhale the necessary dosage of medicine.
As seen in
An alternative structure is shown in
The above two aerodynamic arrangements may be used in any kind of dispenser, with or without measurement functions.
The spirometer of the present invention may be used as a constituent part of larger mobile or stationary measurement schemes as, for example, shown in
As flowmeters 144 and 146, the spirometers of the present invention may be used, for example, the spirometer 10 of
Although a description of specific embodiments has been presented, it is contemplated that various changes could be made without deviating from the scope of the present invention. For example, the present invention could be modified such that pulses of flow velocity could be counted instead of pressure pulses, by means of hot-wire anemometer or other means known per se in the art.
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/IL2004/001057 | 11/17/2004 | WO | 00 | 3/13/2007 |
Publishing Document | Publishing Date | Country | Kind |
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WO2005/046426 | 5/26/2005 | WO | A |
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Number | Date | Country |
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135902 | Jun 2005 | IL |
Number | Date | Country | |
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20070239058 A1 | Oct 2007 | US |