METHOD FOR MEASURING BLOOD PRESSURE AND APPARATUS FOR AUTOMATED BLOOD PRESSURE MEASURING

Abstract: A method of non-invasive blood pressure measuring is conducted in the so-called stat mode, wherein several subsequent measurement cycles occur. A next subsequent blood pressure measuring cycle starts at a time being a function of a cycle specific time interval of a preceding measuring cycle. An apparatus comprises means for retarding start of a next cycle, said retarding means comprise time incrementing means for storing a cycle specific time interval of a preceding measuring cycle. Said retarding means allow a start of a next subsequent cycle as a function of said time interval of the preceding cycle.

Description: The present invention relates to a method for measuring blood pressure, comprising the steps of applying a blood pressure cuff about a subject's limb containing an artery; inflating said cuff to a pressure p max above the systolic pressure p sys , thereby occluding said artery, reducing cuff pressure from p max to at least a pressure p min below the diastolic pressure p dia , thereby permitting an increasing flow through the progressively less occluded artery, detecting of effects at the cuff caused by said increasing flow through that progressively less occluded artery, processing said detected effects in processing means and displaying said processed effects as subject's actual blood pressure values, and conducting a next subsequent blood pressure measuring cycle after the end of a death-time interval Δt dea , said death time interval starting at a time t dz after cuff pressure reaching p min . The invention further relates to an apparatus for automated blood pressure measuring, in particular for cyclic measuring, comprising an inflatable and deflatable pressure cuff, said cuff being applicable about a subject's limb containing an artery, means for inflating said cuff to a pressure p max above the systolic pressure p sys , thereby occluding said artery, means for reducing cuff pressure from p max to at least a pressure p min below the diastolic pressure p dia , thereby permitting an increasing flow through the progressively less occluded artery, means for detecting of effects at the cuff caused by said increasing flow through the progressively less occluded artery, processing means for processing said detected effects and for displaying said processed effects as subject's actual blood pressure values, said processing means further comprising means for retarding the start of a next subsequent measuring cycle until a death-time interval Δt dea has ended. Such so-called "non-invasive" blood pressure measuring methods and apparatus are well-known in the art and known as sphygmomanometers. A similar method and a similar apparatus is known from EP-A2-0 207 807. During such non-invasive sphygmanometric measurements, an inflatable cuff is suitably located around a limb of a subject, for example a human, and is inflated up to a predetermined pressure p max above the systolic pressure p sys , thereby occluding an artery. The limb may be an arm, in particular the upper arm, a foot, or a finger of subject. Thereupon, cuff pressure is reduced, thereby permitting an increasing flow through the progressively less occluded artery. The effects at the cuff may be detected by the auscultative method, thereby detecting the so-called "Korotkoff noise" caused by the artery during deflating of cuff. A further well-known method is the so-called "oscillometric method", for example as described within EP-A2-0 208 520. The oscillometric method of measuring blood pressure is one of the most popular methods in commercially available systems. This method relies on measuring changes in arterial counterpressure, such as imposed by the inflatable cuff which is controllably relaxed or inflated. The cuff pressure is reduced in predetermined increments, and at each pressure level fluctuations are monitored. The resulting signals typically consist of the DC voltage with small superimposed variational component caused by arterial blood pressure pulsations. After suitable filtering to reject the DC component and to provide amplification, peak pulse amplitudes above a given base line are measured and stored. As deflating of cuff continues, the peak amplitudes will normally increase from a lower level to a relative maximum, and thereafter will decrease. The lowest cuff pressure at which the oscillation has a maximum value is representative of mean arterial pressure. Systolic and diastolic pressures can be derived as a predetermined fraction of mean arterial pressure, or by more sophisticated methods of direct processing of the oscillatory complexes. In some applications, several subsequent measurement cycles are necessary and become essential aspect of human and veterinary treatment. Such subsequent measurements are preferably conducted in emergency rooms, intensive and critical care units, and in the operating theatre. One problem on conducting subsequent measurement cycles is the dimension of the pause or death-time between two subsequent cycles. Death-time is understood as an interval starting from a time at which the deflated cuff has reached a minimum pressure, for example 666 Pa (5 mmHg), at which minimum pressure the cuff is deflated approximately totally, and ending at the start time t next of the next subsequent cycle. The known methods and the known apparatus for conducting said measurements in a cyclic manner, so-called "stat-mode", use a constant predetermined death-time interval. If the death-time interval is chosen long, this may be agreeable to the patient. Long death-time intervals, however, do not allow a lot of measurement cycles within a predetermined time interval. For example, the effects of a drug, applicated to the patient during a surgical operation need to be supervised by blood measurement cycles with 20 or 30 seconds. If using a very short death-time interval, it may be very disagreeable for the patient. Furthermore, if a overall time of a measurement cycle is very long, for example based on artifacts during measurement caused by movements of the patient, a short death-time interval is not convenient because of possible blood backwash reflecting to the heart of the patient. Time-consuming measurement cycles are necessary, if patient's systole and diastole are far apart. Nevertheless, all known methods and apparatus for automated non-invasive blood pressure measurements use constantly preselected death-time intervals between two subsequent measurement cycles. It is, therefore, object of the present invention to provide a method and an apparatus for measuring blood pressure as initially indicated using death-time intervals being convenient to the individual subject to be measured. This object is achieved by a method, comprising the step of starting said next subsequent blood pressure measuring cycle at a time t next next being a function of a cycle specific time interval Δt pre of the preceding measuring cycle. This object is further achieved by an apparatus with means for retarding start of next cycle, said means comprising time-incrementing means for storing a cycle specific time interval Δt pre of a preceding measuring cycle, said retarding means allow a start of a next subsequent cycle as a function of said time interval Δt pre . According to the invention, each death-time interval is adapted to the individual subject to be measured and is adapted to the preceding measuring cycle during a cyclic measurement, in particular in stat-mode measurements. The cycle specific time interval Δt pre may be the overall time for conducting said preceding measuring cycle. In particular, the death-time interval may be a fraction of the overall time interval. As a result, a short time interval Δt pre leads to a short death-time interval, and on the contrary, a long time interval Δt pre leads to a long death-time interval. Further, if the cycle specific time interval Δt pre varies during several measurement cycles, for example in response to drugs applied to patient, the death-time interval is automatically adapted cycle by cycle to the varying preceding measuring cycle. The apparatus according to the invention automatically stores time increments of a preceding cycle and allows a start of a next subsequent cycle after a death-time interval being a function of said time increments. So, according to the invention, both a death-time interval adaption to the individual subject to me measured and an automatic adaption to varying measurement cycle intervals is achieved. As a result, blood pressure measuring is more agreeable to subject. According to another aspect of the invention, the time interval t pre starts at a time t₁ after reaching a threshold cuff pressure p thr during inflating said cuff, and ends at a time t₂ after reaching the said threshold pressure p thr again during the cuff pressure reducing step of said cycle. This has the advantage that the time interval Δt pre depends on the varying cuff pressures during measuring cycle, said varying cuff pressures are essential factors to which the measuring cycle time depends. The time interval t pre corresponds to this time the cuff pressure being above a threshold cuff pressure. The death-time interval may be, for example, elected as identical with the time interval Δt pre . According to another aspect of the invention, the said threshold pressure Δt pre corresponds to the mean blood pressure p mea of the subject to be measured. This has the advantage that the threshold pressure is adapted to a particular blood pressure value being representative to the actual condition of the subject to be measured. As a result, a subsequent next cycle depends on both an absolute time interval of the preceding cycle and to the blood pressure measured during said preceding cycle. According to another aspect of the invention, the threshold cuff pressure p thr varies within p thrmin ≦ p thr ≦ p thrmax . This has the advantage, that, in particular if the threshold cuff pressure p thr corresponds to the mean pressure p mea of the subject to be measured, p thr cannot exceed minimum and maximum limits. This assures that if an extremely shift of the mean blood pressure p mea occurs, the corresponding death-time interval neither becomes too short nor unnecessary long. According to another aspect of the invention, for measuring the blood pressure of a human, the threshold cuff pressure p thr is limited to p thrmin = 6,6 kPa(50 mmHg) ≦ p thr ≦ p thrmax = 13,33 kPa(100 mm Hg). This has the advantage that the threshold pressure varies within an area being typical for human mean blood pressure values. For the first measuring cycle, a preselected threshold cuff pressure is used, since within said first cycle the mean blood pressure value is not yet known. According to another aspect of the invention, a further cycle is started if a second time interval Δt preII = Δt pre following to first time interval Δt pre has ended. This has the advantage that a very simple method is achieved, and a simple equipment of an apparatus according to the invention is possible. A first counter is provided, said first counter starting incrementing after reaching at a time t₁ the threshold cuff pressure p thr during inflating cuff. Said first counter starts decrementing after reaching at a time t₂ the said threshold pressure p thr again during the cuff pressure reducing step of the said cycle. So, a subsequent next measuring cycle is started if first counter is zero. According to another aspect of the invention, said second cycle is started if both said second time interval Δt preII and a minimum death-time interval Δt min have ended. In some cases, if t pre is a very short interval, it may occur that after end of the second time interval Δt preII the cuff pressure has not yet reached p min . A deflation of cuff pressure down to p min , however, is wanted in view of convenience for subject to be measured. For example, it is more agreeable to patient if the cuff is deflated nearly totally or at least to p min before inflating the cuff again. The minimum death-time interval Δt min may be very short and possibly zero, in particular if the second time interval Δt preII has end several seconds before start point time t dz of the death-time interval Δt min . According to another aspect of the invention, said second cycle is started if a maximum death-time interval Δt max has ended, but said second time interval Δt preII has not yet ended. This has the advantage that in cases of very large second time intervals Δt preII , and wherein the start time t dz of the death-time interval is in a earlier phase of the said second time interval Δt preII , the death-time interval is not unnecessary long. If waiting in these cases, until a second time interval Δt preII has gone, a death-time interval of 10 or 15 seconds may occur. This time is unnecessary long and results in a reduced number of measuring cycle units per time unit. For example, a maximum death-time interval of 6 seconds is sufficient for human blood pressure measurements. Within an apparatus according to the invention, this feature is achieved by the fact that the said first counter is connected to a second counter incrementing a preselected maximum death-time interval, said second counter starts incrementing after cuff pressure has reached p min . So, a start of the next subsequent cycle can occur if first counter has reached zero and meanwhile second counter has incremented to a minimum death-time interval, but the latest if the second counter has incremented to said maximum death-time interval. Some embodiments of the present invention will not be described with reference to the accompanying drawings in which Figure 1 shows a graph having plotted a cuff pressure via time, demonstrating a first embodiment according to the invention, Figure 2 shows a similar graph as Figure 1, demonstrating a second embodiment according to the invention, Figure 3 shows a graph similar to that of Figures 1 and 2 demonstrating a third embodiment according to the invention, and Figure 4 is a flow chart representing the operation of an apparatus according to one embodiment of the invention. Referring now to Figure 1, the graph shown is representative to a cuff pressure/time graph of an non-invasive blood pressure measurement. A blood pressure cuff is applied about a subject's artery and inflated above the systolic level p sys up to p max , thus fully occluding the artery for a full heart cycle. The cuff pressure is thereafter reduced step by step to permit an increasing flow through the progressively less occluded artery. For example, in accordance with conventional oscillometric techniques, pressure oscillations in the artery are sensed by changes in the counterpressure of the cuff, and in turn by a transducer. A measure of the peak amplitudes of the successively encountered oscillatory complexes (not shown in this graph) are stored in a memory. Also retained is the cuff pressure obtained for each complex peak. As the measurement cycle progresses, the peak amplitude of the blood pressure complexes generally become monotonically larger to a maximum and then become monotonically smaller as the cuff pressure continues toward deflation. The peak amplitude of the cuff pressure oscillation complexes and the corresponding occluding cuff pressure values are retained in a computer memory of a processing means. The inflating of cuff up to p max occurs within 2 to 4 seconds, depending on cuff size and arrangement of cuff, e.g. about subject's upper arm or finger. If cuff pressure reaches a threshold cuff pressure value p thr at time t₁, a counter or timer is started, incrementing time up to time t₂. The time t₂ corresponds to the point, the cuff pressure reaches again the threshold value p thr during the stepwise deflation of cuff. At time t₂, a second time interval Δt preII = Δt pre is started. If using said counter incrementing from time t₁ = 0 to time t₂, said counter starts decrementing at time t₂ down to zero. During second time interval Δt preII , the cuff is deflated down to p min at time t dz . The pressure p min is in the present embodiment 0,66 kPa (5 mmHg). At time t dz , a death-time interval Δt dea is started, said death-time interval Δt dea ends at time t next , said time t next is identical with the end of second time interval Δt preII . At time t next , a next subsequent measuring cycle is initialled by inflating cuff up to pressure p max . Thereafter, a further stepwise deflating of cuff occurs as above described. The cuff works in the stat mode and, therefore, a array of subsequently following cycles are conducted. The pressure threshold value p thr corresponds to the mean blood pressure p mea of the subject to be measured. Since, during the first measuring cycle, the mean pressure value is not known, an incrementing of counter starts if cuff pressure reaches minimum threshold pressure value p thrmin . Therefore, the start point of the incrementing of first counter at time t 1f is somewhat earlier than start time t₁. The deviation, however, is very small because of the great gradient of cuff pressure within the inflating step. The area of possible threshold pressure values p thr being the base for the start of time interval Δt pre are limited by maximum and minimum threshold values p thrmax and p thrmin , resp., with p min = 6,6 kPa (50 mmHg) and p max = 13,33 kPa (100 mmHg). As a result, the death-time interval Δt dea is both a function of the mean pressure value, if p thr = p mea and of the time between two subsequent incremental deflating steps within one individual measuring cycle. Referring now to Figure 2, showing a graph similar to that of Figure 1 but illustrating a situation wherein in second time interval Δt preII ends before cuff pressure during deflating steps has reached p min . This situation may arise if, for example, the mean pressure value is very high and the time interval Δt pre very short. A start of a new cuff inflating step at time t end , e.g. after interval Δt preII may result in many measurement cycles per time unit. However, based on the fact that the cuff pressure cannot reach p min , the subject to be measured always has the feeling of an inflated compressed cuff around its limb. This compressed situation or feeling is very disagreeable, in particular within stat mode, and may result in blood accumulation within the at least partial occluded artery. Therefore, the cuff pressure is allowed to be reduced at least to p min . Within the in Figure 2 illustrated embodiment of the invention, a minimum death-time interval Δt min is provided, for example 2 seconds. It is possible to reduce the death-time interval Δt min to zero, in particular if the graph branch between time t end end time t dz is very flat and approximates to p min . In these cases, a next measuring cycle can be started immediately after cuff pressure reaches p min . Referring now to Figure 3, a situation is illustrated wherein the time interval Δt pre is so long that said second time interval Δt preII ends after a long interval after cuff pressure has reached p min . If starting a next subsequent measuring cycle only after end of second time interval Δt preII , an unnecessary long death-time interval will result. Therefore, a maximum death-time interval Δt max , for example 6 seconds, is provided. A next subsequent measuring cycle is started at time t next after maximum death-time interval Δt max has gone, also if second time interval Δt preII has not yet ended. The principles underlying the operation of the apparatus of the present invention are best described with reference to the flow chart in Figure 4 to which attention should now be directed. To this end, proceeding from a start block 10 a step 12 detects the actual cuff pressure. Test 14 determines whether the pressure value is equal or above to a predetermined threshold pressure p thr . If p thr is not yet reached, test 12 determines actual cuff pressure again ("NO" branch of test 14). However, if actual cuff pressure has reached p thr , block 16 starts incrementing counter 1 ("YES" branch of test 14). Subsequently, step 18 determines the actual cuff pressure. Test 20 determines whether actual cuff pressure has decreased down to p thr again. If threshold pressure p thr is not yet reached, step 18 further conducts pressure measurements ("NO" branch of test 20). However, if actual pressure p has reached threshold pressure p thr , block 22 stops incrementing counter 1 and starts decrementing counter 1 ("YES" branch of test 20). Step 24 determines actual cuff pressure and test 26 determines whether actual cuff pressure has reached p min . If p min is not reached, step 24 determines actual pressure again ("NO" branch of test 26). However, if p min is already reached test 28 determines whether counter 1 = zero ("YES" branch of test 26). If counter 1 is not yet zero, test 30 determines whether maximum death-time interval Δt max has gone ("NO" branch of test 28). If maximum death-time interval has gone, a new inflating of cuff is started by start 10 ("YES" branch of test 30). This situation is illustrated within Figure 3. However, if test 30 determines Δt max has not gone, test 28 determines whether counter 1 is zero ("NO" branch of test 30). However, if test 28 determines counter 1 = zero, test 32 determines whether minimum death-time interval Δt min has gone. If minimum death-time interval has ended, start 10 initiates a next subsequent cuff inflating step ("YES" branch of test 32). This situation is illustrated within Figure 1. However, if test 32 determines t min is not gone, a step 34 conducts time measurements until test 32 indicates that Δt min has gone. This situation is illustrated within Figure 2. The time measurement of test 32 may occur in connection with a second counter. Said second counter starts incrementing if actual cuff pressure value has reached p min . Step 34 determines whether second counter has incremented up to Δt min . Said second counter also can be used for determining whether Δt max has ended.

Claims: A method for measuring blood pressure, comprising the steps of applying a blood pressure cuff about a subject's limb containing an artery; inflating said cuff to a pressure p max about the systolic pressure p sys , thereby occluding said artery; reducing cuff pressure from p max to at least a pressure p min below the diastolic pressure p dia , thereby permitting an increasing flow through the progressively less occluded artery; detecting of effects at the cuff caused by said increasing flow through said progressively less occluded artery; processing said detected effects in processing means and displaying said processed effects as subject's actual blood pressure values, and conducting a next subsequent blood pressure measuring cycle after the end of a death-time interval Δt dea , said death-time interval starts at a time t dz after cuff pressure reaching p min , characterized by starting said next subsequent blood pressure measuring cycle at a time t next being a function of a cycle specific time interval Δt pre of the preceding measuring cycle. A method according to claim 1, characterized in that the time interval Δt pre starts at a time t₁ after reaching a threshold cuff pressure p thr during inflating said cuff, and ends at a time t₂ after reaching the said threshold pressure p thr again during the cuff pressure reducing the step of said cycle. A method according to claim 2, characterized in that the said threshold pressure p thr corresponds to the mean blood pressure p mea . A method according to claim 2 or 3, characterized in that the said threshold cuff pressure p thr is limited as p thrmin ≦ p thr ≦ p thrmax . A method according to claim 4, characterized in that for measuring the blood pressure of a human, p thr is p thrmin = 6,66 kPa(50 mmHg) ≦ p thr ≦ p thrmax = 13,33 kPa(100 mmHg). A method according to any of the preceding claims, characterized in that a next subsequent cycle is started if a second time interval Δt preII = Δt pre following to the first time interval Δt pre has ended. A method according to claim 6, characterized in that said second cycle is started if both, said second time period Δt preII and a minimum death-time interval Δt min have ended. A method according to claim 6 or 7, characterized in that said second cycle is started if a maximum death-time interval Δt max has ended, but said second time interval t preII has not yet ended. An apparatus for automated blood pressure measuring, in particular for cyclic measuring in the so-called stat mode, comprising an inflatable and deflatable pressure cuff, said cuff being applicable about a subject's limb containing an artery; means for inflating said cuff to a pressure p max above the systolic pressure p sys , thereby occluding said artery; means for reducing cuff pressure from p max to at least a pressure p min below the diastolic pressure p dia , thereby permitting an increasing flow through the progressively less occluded artery; means for detecting of effects at the cuff caused by said increasing flow through said progressively less occluded artery; a processing means for processing said detected effects and for displaying said processed effects as subject's actual blood pressure values, said processing means further comprise means for retarding start of a next measuring cycle until a death-time interval Δt dea has ended, characterized in that said means for retarding start of the next cycle comprise time incrementing means for storing a cycle specific time interval Δt pre of a preceding measuring cycle, and that said retarding means allow a start of a next subsequent cycle as a function of said time interval Δt pre . Apparatus according to claim 9, characterized in that said retarding means comprise a first counter, said first counter starts incrementing after reaching at a time t₁ a threshold cuff pressure p thr during inflating cuff, and said first counter starts decrementing after reaching at a time t₂ the said threshold pressure p thr again during the cuff pressure reducing step of said cycle, and said subsequent next measuring cycle is started if first counter is zero. Apparatus according to claim 10, characterized in that said first counter is connected to a second counter, said second counter increments a preselected death-time interval, said second counter starts incrementing after cuff pressure has reached p min , and a start of said next subsequent cycle occurs if first counter has reached zero and meanwhile second counter has incremented to a minimum death-time interval Δt min , but the latest if second counter has incremented to a preselected maximum death-time interval Δt max .

Inventors: FRANKENREITER, MICHAEL
Applicants: HEWLETT-PACKARD GMBH
Application year: 1988
Main classification: A61B5
IPC codes: A61B5