This invention relates to a method and apparatus for delivering a supply of air at positive pressure to a patient for treating sleep disordered breathing. The invention relates to a method of improved model accuracy of the patient circuit. In one case, the invention relates to a method and apparatus which provides improved accuracy of the delivered pressures throughout a breathing cycle. Another case of the inventions application is in the use of an algorithm that determines open and closed apneas. This invention is applicable to all algorithms that must estimate the dynamic characteristics of the patient circuit.
Since the invention of nasal Continuous Positive Airway Pressure (nasal CPAP) for treatment of Obstructive Sleep Apnea (OSA) and other forms of Sleep Disordered Breathing (SDB) by Sullivan, as taught in U.S. Pat. No. 4,944,310, much effort has been directed towards improving the comfort of patients using the devices by controlling the pressure supplied to masks such as the MIRAGE® and ULTRA MIRAGE® manufactured by ResMed Limited.
Some CPAP blower devices, such as the S7™ and S8™ device by ResMed Limited, provide a supply of air at a fixed positive pressure throughout the respiratory cycle of a patient, for example, 15 cm H2O. A blower comprising an electric motor and fan can be constructed to deliver a particular pressure to a patient interface, such as a mask. When the patient breathes in with such a system, the pressure in the mask may reduce by a small amount. When the patient breathes out with such a system, the pressure in the mask may increase by a small amount. These fluctuations in mask pressure are referred to as “swing”. Some blowers use feedback in a pressure controller which counterbalances the effect of patient effort on the mask pressure to reduce the swing. These devices require measuring and monitoring the mask pressure and flow and adjusting the flow generator control to maintain the mask pressure at a constant value.
What is required for each of these devices is a method to determine the pressure and flow at the patient interface. In order to accurately determine pressure and flow at a mask, one either measures them at the mask or measures them near the pressure generator and corrects for various factors, one of which is the pressure loss in a length of tubing between a pressure sensor and the mask.
i. Pressure Correction Due to Losses in the Tubing
U.S. patents that have discussed the pressure loss in tubing of CPAP devices are U.S. Pat. No. 6,817,361 entitled “Administration Of CPAP Treatment Pressure In Presence Of Apnea”, U.S. Pat. No. 6,8101,876 entitled “Assisted Ventilation To Match Patient Respiratory Need”, U.S. Pat. No. 6,688,307 entitled “Methods And Apparatus For Determining Instantaneous Elastic Recoil And Assistance Pressure During Ventilatory Support”, U.S. Pat. No. 6,675,797 entitled “Determination Of Patency Of The Airway”, U.S. Pat. No. 6,575,163 entitled “Method For Calculating The Instantaneous Inspired Volume Of A Subject During Ventilatory Assistance”, U.S. Pat. No. 6,532,957 entitled “Assisted Ventilation To Match Patient Respiratory Need”, U.S. Pat. No. 6,502,572 entitled “Administration Of CPAP Treatment Pressure In Presence Of APNEA”, U.S. Pat. No. 6,484,719 entitled “Method For Providing Ventilatory Assistance In A Spontaneously Breathing Subject”, U.S. Pat. No. 6,367,474 entitled “Administration Of CPAP Treatment Pressure In Presence Of APNEA”, U.S. Pat. No. 6,363,933 entitled Apparatus And Method For Controlling The Administration Of CPAP Treatment”, U.S. Pat. No. 6,138,675 entitled “Determination Of The Occurrence Of An Apnea”, U.S. Pat. No. 6,029,665 entitled “Determination Of Patency Of Airway”, U.S. Pat. No. 5,704,345 entitled “Detection Of Apnea And Obstruction Of The Airway In The Respiratory System”, and U.S. Pat. No. 5,551,419 entitled “Control For CPAP Apparatus”.
These patents propose an alternative to measuring air flow and mask pressure at or near the mask by mounting flow and pressure transducers near the air pressure generator and then calculating the pressure loss along the tubing from the air pressure generator to the mask from the flow through the tubing and a knowledge of the pressure-flow characteristic of the tubing, for example, by table lookup. The pressure at the mask is then calculated by subtracting the tube pressure drop from the pressure at the pressure generator.
The pressure loss from a pressure measuring point to the mask has been calculated from the flow at the blower and the (quadratic) resistance from the measuring point to the mask according to the formula
ΔP=R*Q{circumflex over ( )}2,
where ΔP is the hose pressure drop, R is the hose resistance, and Q is the flow. The mask pressure is then calculated by subtracting the hose pressure drop from the measured sensor pressure. In order to use this technique, a flow sensor is necessary, for example, a pneumotachograph and differential pressure transducer. See, e.g., U.S. Pat. No. 6,810,876 at col. 17, lines 25-50.
U.S. Pat. No. 5,551,419 also recognizes that the air pressure in the mask is a function of the pressure inside the base unit housing, the pressure generator and the pressure drop in the delivery hose. It describes the latter as a function of the flow through the hose and concludes that it is necessary to combine the pressure signal and the flow signal to produce a signal that accurately represents the pressure at the mask. See U.S. Pat. No. 5,551,419 at column 5, lines 7-12.
In order to maintain a steady mask pressure the pressure drop along the tube is added to the desired set pressure at the mask to yield the desired instantaneous pressure at the pressure generator. In some cases the controller of the pressure generator has a negative feedback input from the pressure transducer so that the desired pressure is achieved more accurately. See, e.g., U.S. Pat. No. 5,704,345 at col. 8, lines 26-55.
ii. Failure to Manage Swing
One important factor for patient comfort that must be managed is the swing. For example, for the ResMed S8 inhalation and respiratory therapy devices to ensure particular pressure stability requirements are met, the pressure difference between the inspiration and expiration phases, i.e. the swing, must not exceed 0.5 hPa (“hectopascals”) to meet German MDS specifications. 1 hPa=1.04 cm H2O. The tolerance limits for inspiration and expiration fluctuations from set ventilation pressure are
Ventilation pressure<10 hPa:*p<=0.5 hPa
Ventilation pressure>=10 hPa:*p<=1 hPa.
The prior art techniques for determining mask pressure when the pressure sensor is not at the mask have failed to control swing consistent with these requirements. What is needed is a more accurate determination of mask pressure so that the information may be fed back to the pressure generator in order to achieve better control of swing.
iii. Failure to Predict Dynamics
The mask pressure measurement can also be used in other therapy and control related algorithms One such algorithm is the discrimination of closed and open respiratory apneas using forced oscillations (e.g. David Bassin's “Discriminating Closed and Open Respiratory Airway Apneas by Forced Oscillation Measurements at the Flow Generator” U.S. Provisional Application 60/823,973). This algorithm requires accurate determination of the mask pressure and flow. The hose drop model presented in the prior art fails to accurately model the dynamic characteristics of the air delivery system and as such fails to accurately model the mask pressure and flow.
It has been determined that a discrepancy exists with prior art CPAP devices between the estimation of the mask pressure based upon measurements of flow and pressure at or near the location of the flow generator and the true mask pressure as accurately measured at the mask using a quality pressure transducer. This discrepancy is significant during changes in the mask pressure and flow which can be caused by patient breathing and forced oscillation.
The estimated pressure loss in the air delivery system is better modeled as
Pdrop=K1Q2+K2Q+KLdQ/dt
Where Q is the flow through the hose, K1 and K2 are empirically determined constants and KL is the analytically determined flow inertance.
In the case of higher frequency changes such as during forced oscillation (˜4 Hz) this model models the pressure loss much more accurately.
If the pressure and flow oscillations are represented as complex numbers and we linearise about the operating point we can calculate the pressure oscillations as
Pdrop,AC=(2K1
Where
By careful observation and measurement it has unexpectedly been determined that the discrepancy is most significant when the derivative of flow is positive as measured at or near the location of the flow generator, and is not significant when the derivative of flow at that location is negative. Furthermore, the discrepancy ΔP, when the derivative of the flow dQ/dt is positive, has been found to be proportional to the derivative of the flow with respect to time
ΔP=(k)dQ/dt
i. Empirical Understanding of Pressure Inertance
It has also been found that the magnitude of the discrepancy is related to the physical effect of the inertia of the flowing air, which resists the acceleration caused by pressure differences. If one neglects the compression of the air and all thermodynamic effects
ΔP=(ρl/A)dQ/dt.
where ρ is the air density, l is the length of tubing, A is the cross sectional area of the tubing and Q is the flow as a function of time. Although the air is compressible and subjected to temperature changes due to compression, the above formula gives a very good fit to the observed data for positive dQ/dt, which suggests that the effect is inertance of the air. The formula must however be considered empirical since it does not explain why there is no similar discrepancy for negative flow derivatives.
In accordance with one aspect of the invention there is provided a method and apparatus for improving the determination of mask pressure based upon the estimation of pressure at the flow generator of a CPAP device.
In accordance with another aspect of the invention there is provided a CPAP apparatus for treatment of sleep disordered breathing that reduces pressure during exhalation from a first level accurately to a second level so as to maintain the swing between preset limits.
In accordance with another aspect of the invention there is provided a method of controlling the pressure developed by the electric motor of a blower by freewheeling the motor when the pressure developed by the blower exceeds a threshold and regulating the pressure so as accurately to maintain the swing between preset limits. See copending U.S. patent application Ser. No. 10/871,970, filed Jun. 18, 2004, which is incorporated herein by reference.
In another aspect of the invention, the first pressure level is determined in accordance with an automatic algorithm in which the derivative of flow is calculated at runtime, clipped to not go negative, and is bounded above by a predetermined value. The purpose of the bound is to avoid some detrimental effects of leaks in the mask.
The flow and pressure sensors 28, 30 provide data to a microcontroller 14. Suitable microcontrollers include the HITACHI SH 7032/34 which are 32-bit RISC devices, with a clock rate of 2-20 MHz, 8 by 10 bit A-D converters and a variety of Input and Output features. The microcontroller 14 uses the Nucleus Plus Real-time Operating System (RTOS) by Accelerated Technologies Incorporated. In one form of the invention, the apparatus delivers a predetermined CPAP pressure; such a device is the S7 ELITE by ResMed Limited. In another form of the invention, the microcontroller 14 is programmed to deliver CPAP therapy in accordance with U.S. Pat. No. 5,704,345 (Berthon-Jones) which teaches a method and apparatus for detection of apnea and obstruction of the airway in the respiratory system. The contents of U.S. Pat. No. 5,704,345 are hereby incorporated by cross-reference.
The apparatus includes a display 22, for example, a 2 line by 16 character LCD or similar display device. The apparatus includes a keypad 26, such as one using backlit silicone switches. The device also includes a power supply which provides 40 W at 24V with Class II isolation manufactured by SKYNET. The apparatus may include an interface 20 to enable communication with external devices. For example, a suitable interface chip is the MAX3130/MAX3131 from MAXIM. These chips provide both IrDA and RS-232 communication.
A CPAP device such as the S7 ELITE manufactured by ResMed Limited may be adapted to incorporate our invention. Generally, the controller of the CPAP apparatus according to an embodiment of our invention is programmed to deliver a CPAP pressure in the range of 4 to 25 cm H2O. In an automatically adjusting form of the apparatus, such as the AutoSet SPIRIT and as taught in the abovementioned U.S. Pat. No. 5,704,345, the CPAP apparatus is programmed to increase the CPAP pressure to overcome or prevent partial or complete obstructions of the airway as indicated by the presence of snoring, apneas or flow flattening.
ΔP=(ρl/A)dQ/dt.
As may be seen in the figure, the swing depicted as “1 minute swing” is everywhere below the 0.5 cm H2O limit. Note that 0.5 cm H2O meets the 0.5 hPa standard for swings.
The correction for flow inertance was calculated with the following values:
ρ=Air Density (1.19 kg/m{circumflex over ( )}3)
l=length (2 m)
A=cross section area (d=0.019 m),[A=πd{circumflex over ( )}2/4].
These values yield dQ/dt=1.6 L/s{circumflex over ( )}2, and ΔP=13.43 Pa=1.4 mm H2O.
A theoretical basis follows for the equation used to include the effect of the inertia of the air mass that is accelerated as the result of an increase in the pressure as the flow generator accelerates to increase mask pressure. The calculation is based upon the change of momentum of a mass of air flowing under the differential pressure. Consider, as shown in
m=ρlA.
The mass m is flowing to the left with a velocity v that is related to the flow Q by
v=Q/A.
The momentum Γ of the mass m is my, i.e.,
Γ=ρ|Q.
There is a pressure difference .ΔP across the mass m due to the fact that the flow generator has increased the pressure behind the mass. This exerts a force AΔP on the mass, causing it to accelerate and increase its momentum.
AΔP=dΓ/dt=ρldQ/dt
ΔP=(ρl/A)dQ/dt.
We note, from actual measurement, that this formula only gives correct values when the flow derivative is positive.
The derivative of the flow is calculated as a converted value at runtime. The converted value differs from the derivative by being set to zero for negative values of the derivative and cut off at a maximum positive value of the derivative. This is referred to in
i Pressure Reduction Algorithm
In general, the sequencing takes the following steps:
(i) Upon detection of the transition from inhalation to exhalation, less energy is input to the motor and dQ/dt is negative.
(ii) When the pressure in the patient mask (or whatever interface is utilized) reaches a minimum pressure level during exhalation, more energy is input to the motor so to maintain the pressure at a level suitable for exhalation.
(iii) Upon detection of the transition from exhalation to inhalation, the motor current is altered to control the pressure, as a result of which the motor speed is increased. This causes an increase in flow, and dQ/dt is positive. dQ/dt is calculated and replaced by its converted (clamped) value.
(iv) The value attributable to the pressure in the mask is decreased by ΔP (ρl/A) dQ/dt, where ρ is the air density, l is the length of tubing, A is the cross sectional area of the tubing, Q is the flow as a function of time, and dQ/dt is the converted (clamped) value of the flow derivative.
Although the invention has been described with reference to particular embodiments, it is to be understood that these embodiments are merely illustrative of the application of the principles of the invention. Numerous modifications may be made therein and other arrangements may be devised without departing from the spirit and scope of the invention.
Number | Date | Country | Kind |
---|---|---|---|
2005905830 | Oct 2005 | AU | national |
This application is a continuation of U.S. application Ser. No. 12/088,033, filed on Mar. 25, 2008, which is a national phase entry under 35 U.S.C. § 371 of International Application No. PCT/AU2006/001552 filed Oct. 19, 2006, published in English, which claims priority from Australian Provisional Patent Application No. 2005905830 filed Oct. 21, 2005, all of which are incorporated herein by reference.
Number | Name | Date | Kind |
---|---|---|---|
4944310 | Sullivan | Jul 1990 | A |
5299567 | Joye et al. | Apr 1994 | A |
5331995 | Nesffall et al. | Jul 1994 | A |
5485834 | Joye et al. | Jan 1996 | A |
5540219 | Mechlenburg et al. | Jul 1996 | A |
5551419 | Froehlich et al. | Sep 1996 | A |
5598838 | Servidio et al. | Feb 1997 | A |
5609576 | Voss et al. | Mar 1997 | A |
5704345 | Berthon-Jones | Jan 1998 | A |
6029665 | Berthon-Jones | Feb 2000 | A |
6131571 | Lampotang et al. | Oct 2000 | A |
6138675 | Berthon-Jones | Oct 2000 | A |
6142952 | Behbehani et al. | Nov 2000 | A |
6257234 | Sun | Jul 2001 | B1 |
6332463 | Farrugia et al. | Dec 2001 | B1 |
6363933 | Berthon-Jones | Apr 2002 | B1 |
6367474 | Berthon-Jones et al. | Apr 2002 | B1 |
6390091 | Banner et al. | May 2002 | B1 |
6390092 | Leenhoven | May 2002 | B1 |
6484719 | Berthon-Jones | Nov 2002 | B1 |
6502572 | Berthon-Jones et al. | Jan 2003 | B1 |
6532957 | Berthon-Jones | Mar 2003 | B2 |
6557553 | Borrello | May 2003 | B1 |
6575163 | Berthon-Jones | Jun 2003 | B1 |
6675797 | Berthon-Jones | Jan 2004 | B1 |
6688307 | Berthon-Jones | Feb 2004 | B2 |
6810876 | Berthon-Jones | Nov 2004 | B2 |
6817361 | Berthon-Jones et al. | Nov 2004 | B2 |
6837242 | Younes | Jan 2005 | B2 |
7128069 | Farrugia et al. | Oct 2006 | B2 |
7367338 | Baecke et al. | May 2008 | B2 |
8152789 | Starkweather | Apr 2012 | B2 |
20050211248 | Lauk et al. | Sep 2005 | A1 |
20050241640 | Baecke et al. | Nov 2005 | A1 |
20060173406 | Hayes | Aug 2006 | A1 |
Number | Date | Country |
---|---|---|
05184677 | Jul 1993 | JP |
2000516491 | Dec 2000 | JP |
2001346880 | Dec 2001 | JP |
2004508105 | Mar 2004 | JP |
2005282498 | Oct 2005 | JP |
2006506137 | Feb 2006 | JP |
2007524446 | Aug 2007 | JP |
2004045670 | Jun 2004 | WO |
2004112680 | Dec 2004 | WO |
2005065757 | Jul 2005 | WO |
Entry |
---|
European Patent Office extended Search Report for Application No. 06804418.9; dated Jul. 6, 2010. |
Supplementary European Search Report for Application No. 06804418.9, dated Jul. 6, 2010. |
Number | Date | Country | |
---|---|---|---|
20170065783 A1 | Mar 2017 | US | |
20170348499 A9 | Dec 2017 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 12088033 | US | |
Child | 15354400 | US |