The present invention relates generally to the field of ophthalmic surgery and, more particularly, to a method of controlling surgical parameters of a phacoemulsification system.
The human eye functions to provide vision by transmitting light through a clear outer portion called the cornea, and focusing the image by way of the lens onto the retina. The quality of the focused image depends on many factors including the size and shape of the eye, and the transparency of the cornea and lens. When age or disease causes the lens to become less transparent, vision deteriorates because of the diminished light which can be transmitted to the retina. This deficiency is medically known as a cataract. An accepted treatment for cataracts is to surgically remove the cataract and replace the lens with an artificial intraocular lens (IOL). In the United States, the majority of cataractous lenses are removed using a surgical technique called phacoemulsification. During this procedure, a thin cutting tip is inserted into the diseased lens and vibrated ultrasonically. The vibrating cutting tip liquefies or emulsifies the lens so that the lens may be aspirated out of the eye. The diseased lens, once removed, is replaced by an IOL.
A typical ultrasonic surgical device suitable for an ophthalmic procedure includes an ultrasonically driven handpiece, an attached cutting tip, an irrigating sleeve and an electronic control console. The handpiece assembly is attached to the control console by an electric cable or connector and flexible tubings. A surgeon controls the amount of ultrasound power that is delivered to the cutting tip of the handpiece and applied to tissue at any given time by pressing a foot pedal to request power up to the maximum amount of power set on the console. Flexible tubings supply irrigation fluid to and draw aspiration fluid from the eye through the handpiece assembly.
The operative part of the handpiece is a centrally located, hollow resonating bar or horn that is attached to a set of piezoelectric crystals. The crystals are controlled by the console and supply ultrasonic vibrations that drive both the horn and the attached cutting tip during phacoemulsification. The crystal/horn assembly is suspended within the hollow body or shell of the handpiece by flexible mountings. The handpiece body terminates in a reduced diameter portion or nosecone at the body's distal end. The nosecone is externally threaded to accept the irrigation sleeve. Likewise, the horn bore is internally threaded at its distal end to receive the external threads of the cutting tip. The irrigation sleeve also has an internally threaded bore that is screwed onto the external threads of the nosecone. The cutting tip is adjusted so that the tip projects only a predetermined amount past the open end of the irrigating sleeve.
In use, the ends of the cutting tip and the irrigating sleeve are inserted into a small incision of predetermined width in the cornea, sclera, or other location. One known cutting tip is ultrasonically vibrated along its longitudinal axis within the irrigating sleeve by the crystal-driven ultrasonic horn, thereby emulsifying the selected tissue in situ. The hollow bore of the cutting tip communicates with the bore in the horn that in turn communicates with the aspiration line from the handpiece to the console. Other suitable cutting tips include piezoelectric elements that produce both longitudinal and torsional oscillations. One example of such a cutting tip is described in U.S. Pat. No. 6,402,769 (Boukhny), the contents of which are incorporated herein by reference.
A reduced pressure or vacuum source in the console draws or aspirates the emulsified tissue from the eye through the open end of the cutting tip, the cutting tip and horn bores and the aspiration line, and into a collection device. The aspiration of emulsified tissue is aided by a saline solution or other irrigant that is injected into the surgical site through the small annular gap between the inside surface of the irrigating sleeve and the cutting tip.
One known surgical technique is to make the incision into the anterior chamber of the eye as small as possible in order to reduce the risk of induced astigmatism. These small incisions result in very tight wounds that squeeze the irrigating sleeve tightly against the vibrating tip. Friction between the irrigating sleeve and the vibrating tip generates heat. The risk of the tip overheating and burning tissue is reduced by the cooling effect of the aspirated fluid flowing inside the tip.
When the tip becomes occluded or clogged with emulsified tissue, the aspiration flow can be reduced or eliminated, allowing the tip to heat up, thereby reducing cooling and resulting in temperature increase, which may burn the tissue at the incision. In addition, during occlusion, a larger vacuum can build up in the aspiration tubing so that when the occlusion eventually breaks, a larger amount of fluid can be quickly suctioned from the eye, possibly resulting in the globe collapsing or other damage to the eye.
Known devices have used sensors that detect large rises in aspiration vacuum, and detect occlusions based a particular pre-determined aspiration vacuum level. Based on this sensed occlusion, power to the handpiece may be reduced and/or irrigation and aspiration flows can be increased. See U.S. Pat. Nos. 5,591,127, 5,700,240 and 5,766,146 (Barwick, Jr., et al.), the entire contents of which are incorporated herein by reference. These devices, however, use a fixed aspiration vacuum level to trigger a response from the system. This fixed level is a threshold value based upon a fixed percentage of the selected upper vacuum limit. The use and effectiveness of such systems, however, are limited since they do not respond until that preset aspiration vacuum level is reached. U.S. Pat. No. 6,179,808 to Boukhny, et. al., the entire contents of which are incorporated herein by reference, describes a system that reduces signal amplitude and/or duty cycle when the temperature exceeds a predetermined limit, as calculated based on the measured or estimated irrigation flow.
Known occlusion sensing systems can thus be improved since, in reality, aspiration vacuum levels can vary over a short period of time during different stages of occlusion. Setting this preset vacuum limit too low results in the system changing its operating parameters prematurely, and holding on to those parameters after the occlusion has cleared. Setting the limit too high can result in the system changing its setting too close to the actual occurrence of the occlusion, and changing its setting back to normal prior to the clearance of the occlusion. In addition, cutting efficiency is maximized when the cutting tip is occluded, so increasing power when an occluded condition is detected maximizes cutting efficiency, but increases the risk of overheating the tissue surrounding the tip.
Further, throughout the surgery, there are times when the tip is pressing against the lens in order to emulsify lens tissue, and there are times when the tip is not in contact with the lens. Ultrasound energy, however, remains on until the surgeon releases the foot pedal, even during times when the lens material is aspirated, the surgeon pulls the tip away from the lens, or the lens moves away from the tip. The efficiency of the surgery decreases, and the wasted energy can cause unnecessary heating of the tip, which may increase the likelihood of an undesirable burn to the tissue at the incision.
Therefore, a need continues to exist for an occlusion detection system that more accurately detects the occurrence and clearance of an occlusion in a surgical aspiration system. This information can be used by the control system to adjust power accordingly, e.g., increasing power during an occlusion in order to improve the cutting efficiency of the ultrasound tip and/or reducing power when the relative temperature reaches a predetermined threshold in order to prevent excessive heating. Cutting efficiency may be further increased by adding a load detection system that detects when the tip is no longer in contact with lens material and adjusts power automatically.
According to one embodiment, a method of controlling a surgical system includes establishing a threshold power level, monitoring a load on the cutting tip of an ultrasound handpiece based on the voltage and current drawn by the handpiece during a non-zero sense power interval that is between cutting power intervals. The power drawn by the handpiece is compared to the threshold power level and is adjusted as necessary, for example, if the power drawn by the handpiece exceeds the threshold power level by adjusting an amplitude or stroke of the output of the ultrasound handpiece.
In an alternative embodiment, a method of controlling a surgical system includes establishing a threshold power level and monitoring a load on the cutting tip of an ultrasound handpiece based on the voltage and current drawn by the handpiece during a non-zero sense power interval that is between cutting power intervals. The power drawn by the handpiece is compared to the threshold power level, and adjusted as necessary. Further, a threshold temperature is established, and the irrigation pressure in the line running to the handpiece is monitored. A rate of flow of irrigation fluid is calculated and the heat absorption capacity of the irrigation fluid flow is determined. The heat absorption capacity and power supplied to the handpiece are compared or analyzed to determine a temperature of an eye, which is compared to the threshold temperature. The power delivered to the cutting tip of the handpiece is adjusted as necessary.
According to another embodiment, a method of controlling a surgical system includes establishing a threshold power level and monitoring a load on the cutting tip of the ultrasound handpiece based on the voltage and current drawn by the handpiece during a non-zero sense power interval that is between cutting power intervals. The power drawn by the handpiece is compared to the threshold power level and adjusted if the power drawn by the handpiece exceeds the threshold power level. Power can be adjusted by changing the amplitude or stroke of the ultrasound handpiece. In addition, a rate of change of an operating parameter of the surgical system is determined, and a stage of occlusion is determined based on the rate of change. The power delivered to the cutting tip of the handpiece is adjusted as necessary based on the determined stage of occlusion.
In various embodiments, the load monitoring is performed during a sense interval or pulse at a power level that is less than the power level of cutting pulses and by monitoring voltage and current. Voltage and current can be monitored during a substantially constant portion of a pulse or interval or during a decay of a sense interval or pulse. The sense pulse or interval can have a fixed or variable duration. Sense pulses or intervals can immediately precede or follow cutting pulses, or can be pulses or intervals that are separate from cutting pulses. Load monitoring can also be performed by during a decay of a non-zero sense power interval. Some degree of cutting may occur, since a sense interval is at a relatively low power level.
Power can be adjusted by adjusting a stroke of the cutting pulse or interval following a non-zero sense interval. In various embodiments, power adjustments may be made by adjusting a duty cycle of the output of the ultrasound handpiece. A sensitivity adjustment can be used to adjust the amount of power that is delivered to the cutting tip.
Power adjustments can also be related to comparisons of calculating flow rates of irrigation fluid and determining a heat absorption capacity to determine a temperature of an eye, which is compared to a threshold temperature to determine whether power should be adjusted.
Referring now to the drawings, in which like reference numbers represent corresponding parts throughout and in which:
This specification describes embodiments of a method for controlling a surgical system for use in, for example, phacoemulsification surgery. Embodiments provide a surgical system that is able to detect stages of a surgical event, such as an occlusion, e.g., the onset of an occlusion, a pre-occlusion condition, a full occlusion, and when an occlusion breaks, by detecting changes in the pressure levels of an aspiration system, an irrigation system, or a combination thereof. By monitoring how the aspiration vacuum or irrigation pressure levels vary, the onset and break up of an occlusion can be accurately detected. Once an occlusion is detected, the surgical system can be programmed to increase the power available to the handpiece, either by increasing the stroke of the tip or by increasing the duty cycle of the pulsed ultrasound power.
To help avoid overheating of the tip, the surgical system monitors the irrigation flow rate and reduces the power to the handpiece automatically if an overheating situation is predicted. Alternatively, or in addition, the amount of power drawn by the handpiece can be monitored, which indicates the cutting load on the tip. This information can be used to automatically adjust the power or stroke (displacement) of the tip to compensate for load variations on the tip. In the following description, reference is made to the accompanying drawings, which show by way of illustration, but not limitation, specific embodiments that can be utilized.
Embodiments can be implemented on commercially available surgical systems or consoles through appropriate hardware and software controls. One suitable system 100 is generally illustrated in
Various ultrasonic handpieces 112 and cutting tips can be utilized including, but not limited to, handpieces and tips described in U.S. Pat. Nos. 3,589,363; 4,223,676; 4,246,902; 4,493,694; 4,515,583; 4,589,415; 4,609,368; 4,869,715; 4,922,902; 4,989,583; 5,154,694 and 5,359,996, the entire contents of which are incorporated herein by reference. Exemplary handpieces are shown in
Referring again to
In use, irrigation pressure sensor 122 is connected to the handpiece 112 and the infusion fluid source 126 through irrigation lines 130, 132 and 134. The irrigation pressure sensor 122 measures the pressure of irrigation fluid from the source 126 to the handpiece 112 and supplies this information to the CPU 116 through the cable 136. The irrigation fluid pressure data may be used by the CPU 116 to control the operating parameters of the console 114 using software commands. For example, the CPU 116 may, through a cable 140, vary the output of the power supply 120 being sent to the handpiece 112 and the tip 113 though a power cable 142. The CPU 116 may also use data supplied by the irrigation pressure sensor 122 to vary the operation of the pump 118 through a cable 144. The pump 118 aspirates fluid from the handpiece 112 through a line 146 and into a collection container 128 through line 148. The CPU 116 may also use data supplied by the irrigation pressure sensor 122 and the applied output of power supply 120 to provide audible tones to the user. Additional details concerning such surgical systems can be found in U.S. Pat. No. 6,179,808 (Boukhny, et al.) and U.S. Pat. No. 6,261,283 (Morgan, et al.), the entire contents of which are incorporated herein by reference.
In one embodiment, the control console 114 can control the amount of power that is delivered to the handpiece 112 based on the stage of an occlusion event. More particularly, power adjustments are made based on changes of an aspiration vacuum level, an irrigation pressure level, or both aspiration vacuum and irrigation pressure levels. The change can be, for example, a rate of change of the increase or decrease of aspiration vacuum and/or irrigation pressure.
Adjustments to the amount of power delivered to a handpiece can be made as shown in
More specifically, it has been determined that aspiration vacuum and irrigation pressure levels follow a detectable pattern before, during and after an occlusion. This pattern can be used to identify a stage of an occlusion and adjust the power delivered to the handpiece 112 accordingly.
As shown in
As shown in
Following the occlusion onset event 500, the occlusion develops or matures into a pre-occlusion event or condition 510. As shown in
The pre-occlusion condition 510 matures into a full occlusion 520. A full occlusion is characterized by the maximum limit 630. Further, the irrigation pressure is steady 635.
Following the full occlusion 520, the occlusion breaks 530. An occlusion break event 530 is characterized by a rapid decrease of both the aspiration vacuum 640 and the irrigation pressure 645. As shown in
Following the occlusion break 520 is an occlusion recovery stage 530. A recovery stage 530 is characterized by a continued slowing of the rate of decrease of the aspiration vacuum 650 and irrigation pressure 655, eventually reaching a substantially constant level. In other words, the rates of decline of the vacuum and irrigation pressures gradually increase from a negative value to approximately 0.
Based on the surgical systems tested, the patterns of vacuum and irrigation pressures shown in
For example, the linear correlation between two sequences xi and yi is a measurement of how close one sequence can be transformed into the other via a linear transformation:
yi=axi+b
Where: a=linear correlation coefficient, b=offset.
Given two sequences, the linear correlation R is calculated as follows:
Where: N—correlation length (i.e. number of points in the sequences)
The linear correlation coefficient is calculated as follows:
A method according to one embodiment involves calculating the linear correlation between a sample sequence of aspiration vacuum and/or irrigation pressure sensor readings collected during use of the surgical system and the predefined pattern representing the occlusion events in question. The calculated correlation value reflects the similarity between the sample sequence and the predefined pattern, with the highest possible value of 1.0 representing an absolute match. The range of values indicating a sufficient correlation is preferably between 0.80 and 0.99.
Once a match or acceptable correlation is established, the certainty of the some surgical events, such as pre-occlusion and occlusion recovery is high, and the surgical parameters of the system can be adjusted as necessary.
For events such as occlusion onset and occlusion break, the pattern match should be qualified based on the rate of the change of the test values. The rate of change of vacuum and irrigation pressures can be evaluated using linear correlation coefficient, which reflects the slope ratio of the test sequence and the predefined pattern, and can thus be used to evaluate whether the sample sequence has a sufficient rate of change for a particular event.
In one embodiment, the rate of change is a direct calculation of the derivative (ΔValue/ΔTime), or the change in a value over a certain time. The criteria for a sufficient rate can be established empirically for a given system at different settings (e.g. different aspiration pump rates).
For cases that require qualification on both pattern match and the rate of change, the occlusion event is considered to be detected when both conditions are satisfied. Once the occlusion event is detected the surgical parameters of the system can be adjusted. The described method can be applied to detecting all events in an occlusion sequence (occlusion onset, pre-occlusion, occlusion, occlusion break, and recovery). By detecting patterns of aspiration vacuum and/or irrigation pressure levels, the timing of when power should be adjusted can be accurately determined. Thus, embodiments are more accurate than known systems that rely on a threshold or pre-determined aspiration vacuum levels to identify a full occlusion.
In a further embodiment, the matching of patterns can be accomplished using convolution rather than correlation. Accordingly, persons of ordinary skill in the art will appreciate that the correlation, derivative, and convolution techniques discussed herein are merely illustrative examples, and are not intended to be limiting.
In a further embodiment, the amount of power delivered to the handpiece can be regulated to prevent overheating of the tip 113, which can lead to damage to the eye tissue. This embodiment is referred to as Thermal Watch™ and is generally illustrated in
In step 700, a threshold temperature is established. In step 710, a pressure of a source of an irrigation fluid 126, such as saline, is monitored. In step 720, a calculation or determination is made of the flow rate of irrigation fluid from the irrigation fluid source 126 being monitored. A capacity of the flow of irrigation fluid to absorb heat, or the heat absorption capacity of the irrigation fluid, is determined in step 730. In step 740, the determined heat absorption capacity and the power supplied to the handpiece 112 are compared or analyzed. Based on this comparison or analysis, a temperature of the eye or other tissue is determined in step 750.
For example, an approximate temperature of the eye can be determined by performing a temperature calculation at discrete time steps where the estimated temperature at the current time is found by multiplying the previous temperature estimation by a cooling coefficient (which is <1) then adding the power delivered during the time interval times a power coefficient and subtracting the flow during the time interval times a flow coefficient.
In step 760, the estimated eye temperature and the threshold temperature are compared. The amount of power delivered to the cutting tip 113 of the ultrasound handpiece 112 is adjusted, as necessary, in step 770, based on whether the estimated temperature exceeds the threshold or exceeds the threshold by a predetermined amount. For example, the power delivered to the handpiece may be reduced by reducing amplitude of the ultrasound signal and/or decreasing duty cycle of the ultrasound signal, if the estimated temperature exceeds the threshold, whereas the power may be maintained or increased if the estimated temperature is below the threshold.
If Thermal Watch™ is enabled, then in step 810, a threshold value, set by the surgeon, is noted or read by the system. The threshold value may be unitless and be in any number of steps from “Off” to “Maximum”.
In step 815, the system monitors the pressure of the irrigation fluid (the “IPS Reading”) and/or the height of the irrigation fluid source bottle 126 in step 820. These irrigation fluid pressure parameters, indicate the rate of flow of irrigation fluid, i.e., the quantity of irrigation fluid over a certain time, in step 825. Knowing the rate of irrigation fluid flow, the heat quenching capacity for that rate of irrigation fluid flow can be approximated (step 830). The flow function in time F(t) can approximated a linear function of pressure drop across the fluidics line: F(t)=R(P0−P(t)), where P0 is the irrigation source pressure (e.g. irrigation bottle height), P(t) is irrigation pressure sensor reading, and R is fluidic line resistance between the pressure source and the irrigation pressure sensor. The resistance R is established empirically for a given fluidic (i.e. consumable) configuration. The above approximation yields accurate results for a steady state flow conditions. To improve estimation accuracy for transient response an exponentially decaying correction can by added to the equation above as follows:
where δ is the transient coefficient, and τ0 is the time constant of the approximated fluidic line. Both values can be established empirically for a given fluidic (i.e. consumable configuration). Sample values established for the Alcon INFINITI® system consumable are: δ=0.3, τ0=1.3 seconds. The equation above can easily converted into a discrete form allowing practical implementation of the method.
The amount of heat that is generated by the ultrasonic cutting tip 113 of the handpiece 112 (i.e., the Ultrasonic or “US Power Level”) is also monitored in step 835. The approximation of the heat quenching capacity for the irrigation fluid flow is then compared to the amount of heat that is generated by the ultrasonic cutting tip 113 to determine an approximate temperature of the eye in step 840. A determination is made whether the temperature of the eye is higher than a preset threshold value or is within a certain margin of the threshold in step 845. For example, the margin may be three degrees Fahrenheit (3° F.) within (e.g. below) the threshold, as shown in
If the temperature of the eye is not within the margin (e.g. 3° F.) or does not exceed the threshold, then linear ultrasound control functions can be used (step 850). However, if the temperature of the eye is within the margin or exceeds the threshold, then the system utilizes an algorithm to compute an appropriate duty cycle in step 855. The control algorithm may be, for example, a standard linear control algorithm such as a PI (proportional-integral) or PID (proportional-integral-derivative) control algorithm. The control algorithm may also be a non-linear control algorithm, such as a bang-bang controller with or without hysteresis. Persons skilled in the art will appreciate that various algorithms can be used in different applications.
For example, in step 860, a determination is initially made whether the system currently operates in a continuous mode. In continuous mode, a continuous supply of power is applied to the handpiece without interruption. If the system is in continuous mode then in step 865, the system switches the mode of operation from continuous to pulsed ultrasonic power. If the system is not in continuous mode, then a determination is made in step 870 whether the system is operating in burst or pulse mode.
Referring to
The off time 910 between fixed width pulses 900 is controlled by the surgeon's input via, for example, depression of the foot pedal. In other words, in Burst mode, each pulse 900 has a fixed “on” time, and a variable “off” time. The “off” time is varied by adjusting the position of the foot pedal or foot switch.
For example,
Referring again to
Referring to
Alternatively, if the system is operating in continuous mode (860), and the temperature of the eye is above the threshold, then the power can be switched off until the eye temperature drops below the threshold. Further, if the system is operating in a burst or pulse mode and temperature of the eye is above the threshold, power can be turned off for a remainder of a pulse, and the next power pulse can be delayed, if necessary, until the eye temperature drops below the threshold. Finally, the power level (stroke length) can be reduced to help prevent injury to the eye rather than manipulation of the pulse duty cycle.
Persons skilled in the art will appreciate that the Thermal Watch feature can be used with different types of pulses, e.g., continuous, pulsed, burst, and pulses having different patterns, such as pulses described later in this specification and shown in
Similar power adjustments can be made when an occlusion event is detected. For example, in one embodiment, the power delivered to the tip 113 can be increased by increasing the “On” time or by decreasing the power “Off” time in the ultrasound duty cycle so as to increase the cutting efficiency of handpiece 112. The temperature of eye can be monitored using the Thermal Watch™ feature to decrease the power “On” time, or increase the power “Off” time prior to tip 113 becoming overheated. Accordingly, embodiments provide a manner of effectively increasing power when necessary (e.g., when an occlusion event occurs), but effectively monitoring and reducing the power, as necessary, in order to prevent overheating of the tip 113 and burning or damaging eye tissue.
An alternative embodiment is directed to a load detection system and method, generally referred to as “Power on Demand,” can limit or overrule the amount of power that is requested by a surgeon if it is determined that too much power is being requested in order to prevent damage to eye tissue. The system can detect when the cutting tip 113 is no longer in contact with lens tissue or is in contact with different sections of a lens tissue with varying hardness, and automatically adjusts the amount of power delivered to the handpiece.
As previously discussed, one or more piezoelectric crystals in the handpiece 112 are driven by power that is provided by a power supply. The crystals vibrate, which in turn causes a needle in the handpiece to vibrate and emit ultrasound energy. The surgeon positions the needle so that the ultrasound energy is delivered to an eye tissue, such as a lens to, for example, break up cataracts. A separate aspiration system is used to remove tissue fragments. A surgeon may request that a certain amount of power be delivered to the tip 113, by, for example, depressing a foot switch or other switch activator. During the surgical procedure, the system applies a low level of voltage to the crystals causing them to emit a small amount of ultrasound energy. The voltage across the crystals and the current through the crystals under this condition are then measured. The voltage and current values are used to calculate a power value that is drawn by the handpiece. The ultrasound handpiece 112 tends to draw more power in order to maintain a given stroke (amplitude) when the tip 113 is in contact with harder tissue or material (such as a cataractuous lens). This increase in power based on contact with material encountered by the tip in a typical cataract surgery has been found to be measurable at lower power settings. In a modified pulsed mode, a small amount of power is applied to the tip 112 between the higher power pulses used to cut the tissue. In other words, a small amount of power is applied during low power periods.
For example, as shown in
In the illustrated embodiment, the duration of the cutting interval 1100 and sense interval 1110 are approximately the same. Voltage and current measurements are performed during the sense intervals in order to correlate an amount of power that is drawn by the handpiece 112 during the sense interval, with a load 1130 at the tip 113. Some degree of cutting may also occur since a small amount of power is still applied to the tip, however, cutting primarily occurs during the higher power cutting interval. Thus, although this specification refers to a “sense” interval, both sensing and cutting may occur during this interval.
The amount of power drawn by a handpiece 112 is determined during the sense interval 1110 is then used to adjust the power of the next or subsequent cutting interval 1100. The power is adjusted proportionately based on the detected power and the surgeon's request. In other words, if a higher load is detected at the tip, a higher in portion (possibly all) of the power requested by a surgeon will be delivered on the next cutting interval. Likewise, if a lower load is detected, a smaller portion (possibly none) of the power requested by the surgeon will be delivered during the next cutting interval 1110.
For example, the power detected during sense interval 1110a is used to proportionately adjust the power level of the next cutting interval 1100b. Similarly, the power detected during sense interval 1110b is used to proportionately adjust the next cutting interval 1100c. Thus, the cutting power 1100 is continuously adjusted to compensate for different loads 1130 on the ultrasonic tip 113 of the handpiece 112.
As shown in
Due to the variation in ultrasound handpieces and cutting tips, the load 1130 sensing feature should be calibrated at the beginning of each surgery. For example, calibration can be performed during a “tune cycle” during which the handpiece tip 113 is placed in a test chamber filled with irrigation fluid. At this time, ultrasound power is applied to the tip 113 at the sensing power setting. The amount of power drawn by the handpiece 112 under this baseline condition is saved in the control system memory as a threshold or a “no-load” condition. If necessary, as surgery progresses, the control system 114 may use automatic threshold adjustment to adjust this threshold value based on loads 1130 that are measured during the surgery.
The load sensing feature also allows the surgeon to control the sensitivity of the adjustments made by the control system 114. More specifically, a sensitivity adjustment is a linear or coefficient adjustment that sets the gain of the power reductions made when less than full load is sensed. Once the threshold and sensitivity are set, the power to the handpiece 112 may be adjusted based on an algorithm.
The power drawn by the cutting tip 113 is monitored in step 1210. A power supply 120 is coupled to the handpiece 112 and delivers power to the tip 113 via a power line 1302. A power control system 1300 is connected to the inputs and outputs of the power supply 120 via connectors 1303-1305. The connectors 1304 and 1305 are coupled to the output of the power supply 120, and the connector 1303 is coupled to the input of the power supply 120.
The power control system 1300 shown includes feedbacks 1310 and 1311 for voltage and current. The feedback components 1310 and 1311 are coupled to the connectors 1304 and 1305. Voltage and current measurements obtained during sense intervals 1110 vary based on the stresses placed on the piezoelectric crystals in the handpiece 112. If the needle or tip 113 encounters tissue that is more resistant to cutting (a high load), the magnitudes of the voltage and/or the current may increase, whereas if the needle or tip 113 encounters tissue that is more easily cut (a lower load), the magnitudes of the voltage and/or current may decrease. The voltage and current values obtained by the feedbacks 1310 and 1311 during each sense interval 1110 are provided to respective Root Mean Square (“RMS”) converters 1320 and 1321.
The RMS converters 1320 and 1321 determine an average voltage magnitude and an average current magnitude over a defined period of time. These RMS values are provided to Analog to Digital (“A/D”) converters 1330 and 1331, which provide digital signals representing the respective measured analog voltage and current to a microprocessor 1340.
The microprocessor 1340 can be the same microprocessor 116 as discussed above or a separate microprocessor or controller. The digital voltage and current values are provided by the A/D converters 1330 and 1331 to the microprocessor 1340. Software in the microprocessor 1340 calculates 1350 the “Sense” power 1352 detected during a sense interval 1110 as Power (“P”)=Voltage (“V”)×Current (“I”) based on the values provided by the A/D converters 1330 and 1331. Thus, the calculation involves a linear calculation without the necessity to account for non-linear attributes, such as phase and resonance. The sense power 1352 is then compared to the threshold or baseline power 1355.
The calculated sense power 1352 exceeds the threshold or base power 1355 when power is needed by the handpiece 112 to cut tissue, i.e., when the handpiece 112 is applied to something other than the base material or liquid, such as saline. The comparison of sense power 1352 and the threshold power 1355 is used to determine how the power to be delivered to the handpiece 112 should be adjusted, if at all, during the next cutting interval in step 1240 based on the characteristics of the tissue encountered by the tip 113 of the handpiece 112. This comparison is multiplied by a scaling coefficient 1356 that is stored in the handpiece or in the software that relates the amount by which the sense power 1352 exceeds the threshold power 1355 to the fraction of full loading detected 1357. The scaling coefficient 1356 can, for example, be empirically determined based on prior operation of the system.
In addition to this threshold comparison and percent load calculation, a sensitivity adjustment or coefficient 1360 is set by the surgeon to indicate what fraction of the power requested by the surgeon should be delivered to the tip during the next cutting interval based on an amount by which the sense power 1352 exceeds the threshold power 1355. The sensitivity coefficient 1360 ranges from 0-0.1 or is otherwise generally represented as a % value, e.g., 20%, 50% or 85%. These values may be represented to the surgeon as off, low, medium, high or some other scale or indication. In step 1250, values obtained by the (sense voltage−threshold)×scaling factor calculation are multiplied by the sensitivity coefficient 1360. A greater quantity of the requested power 1370 (e.g., as indicated by the level of a footswitch 1375) is delivered to the handpiece 112 with higher sensitivity coefficients than with lower sensitivity coefficients. For example, if the surgeon requests “X” amount of power 1370 via the foot pedal 1375, then some, all, or none of that “X” power 1370 may be delivered to the handpiece 112 depending on the sensitivity coefficient 1360.
Thus, the power 1380 that is actually delivered to the handpiece 112 may be less than or the same as the amount of power requested 1370 by a surgeon by depression of the foot pedal 1375. Accordingly, the embodiments use linear relationships and calculations, threshold determinations and linear calculations based on sensitivity coefficients in order to adjust the amount of power 1380 that is delivered to a handpiece 112.
Referring to
Referring to
The time required for a sense pulse or interval to decay to a certain level can be correlated to a load at the tip. This can be done using, for example, a lookup table that cross-references the rate of decay and a load at the tip. This decay and load information can then be used to adjust the power level of the next cutting pulse or interval if necessary. For example, referring to reference Point C in
According to a further embodiment, cutting and sense pulses can be at different frequencies. For example, cutting pulses can be applied at a particular frequency, and a sense pulses can be applied at one of the harmonics of the cutting pulse frequency. For example, cutting pulses may be applied at about 40 kHz, and sense pulses can be applied at one of the harmonics, such as 80 kHz or 120 kHz.
Persons skilled in the art will appreciate that the FIGS. 11 and 14-23 are provided as exemplary sense and cutting interval patterns and are not intended to be limiting since sense and cutting intervals can be adjusted as necessary for different systems and applications. Further, persons skilled in the art will appreciate that both sensing and some degree of cutting may occur during a lower power sense interval since sensing occurs at a non-zero level, and some cutting occurs, although the amount of cutting is small compared to cutting that occurs during a higher power cutting interval. Persons skilled in the art will also appreciate that the Thermal Watch feature can be used with these different pulse patterns since the Thermal Watch considers the amount of power delivered and is not dependent on a particular pulse pattern.
Referring to
Although references have been made in the foregoing description to various embodiments, persons of ordinary skill in the art will recognize that insubstantial modifications, alterations, and substitutions can be made to the described embodiments without departing from the scope of embodiments. For example, persons of ordinary skill in the art will recognize that various capabilities and embodiments can be operated individually or in combination. For example, in an alternative embodiment, the embodiments directed to determining changes in aspiration vacuum and/or irrigation pressure can be combined with the “Thermal Watch” embodiments shown in
This application is a division of U.S. patent application Ser. No. 12/577,521, filed Oct. 12, 2009, now U.S. Pat. No. 8,257,307, issued Sep. 4, 2012, which is a division of U.S. patent application Ser. No. 11/068,301, filed Feb. 28, 2005, now U.S. Pat. No. 7,625,388 issued Dec. 1, 2009, which claims priority to U.S. Provisional Application Ser. No. 60/587,693, filed Jul. 14, 2004, and which is a continuation-in-part of U.S. patent application Ser. No. 10/818,314, filed Apr. 5, 2004, now U.S. Pat. No. 7,297,137, issued Nov. 20, 2007, which claims priority to U.S. Provisional Application Ser. No. 60/555,240, filed Mar. 22, 2004.
Number | Name | Date | Kind |
---|---|---|---|
3526219 | Balamuth | Sep 1970 | A |
3589363 | Banko et al. | Jun 1971 | A |
3601126 | Estes et al. | Aug 1971 | A |
3693613 | Kelman | Sep 1972 | A |
3812855 | Banko | May 1974 | A |
3812858 | Oringer | May 1974 | A |
3857387 | Shock | Dec 1974 | A |
3902495 | Weiss et al. | Sep 1975 | A |
3930505 | Wallach | Jan 1976 | A |
3942519 | Shock | Mar 1976 | A |
3952732 | Shock | Apr 1976 | A |
3956826 | Perdreaux, Jr. | May 1976 | A |
3964487 | Judson | Jun 1976 | A |
3990452 | Murry et al. | Nov 1976 | A |
4024467 | Andrews et al. | May 1977 | A |
4024866 | Wallach | May 1977 | A |
4114623 | Meinke et al. | Sep 1978 | A |
4126137 | Archibald | Nov 1978 | A |
4156187 | Murry et al. | May 1979 | A |
4168707 | Douvas et al. | Sep 1979 | A |
4184510 | Murry et al. | Jan 1980 | A |
4223676 | Wuchinich | Sep 1980 | A |
4246902 | Martinez | Jan 1981 | A |
4248232 | Engelbrecht et al. | Feb 1981 | A |
4406284 | Banko | Sep 1983 | A |
4417578 | Banko | Nov 1983 | A |
4493694 | Wuchinich | Jan 1985 | A |
4496342 | Banko | Jan 1985 | A |
4504264 | Kelman | Mar 1985 | A |
4508532 | Drews et al. | Apr 1985 | A |
4515583 | Sorich | May 1985 | A |
4589415 | Haaga | May 1986 | A |
4590935 | Ranalli | May 1986 | A |
4609368 | Dotson, Jr. | Sep 1986 | A |
4651280 | Chang et al. | Mar 1987 | A |
4658819 | Harris et al. | Apr 1987 | A |
4705500 | Reimels et al. | Nov 1987 | A |
4712544 | Ensslin | Dec 1987 | A |
4739759 | Rexroth et al. | Apr 1988 | A |
4750488 | Wuchinich et al. | Jun 1988 | A |
4770654 | Rogers et al. | Sep 1988 | A |
4793346 | Mindich | Dec 1988 | A |
4827911 | Broadwin et al. | May 1989 | A |
4869715 | Sherburne | Sep 1989 | A |
4922902 | Wuchinich et al. | May 1990 | A |
4961424 | Kubota et al. | Oct 1990 | A |
4969885 | Farin | Nov 1990 | A |
4989583 | Hood | Feb 1991 | A |
4989588 | Kubota et al. | Feb 1991 | A |
5026387 | Thomas | Jun 1991 | A |
5116343 | Ames et al. | May 1992 | A |
5139509 | Fischer et al. | Aug 1992 | A |
5151085 | Sakurai et al. | Sep 1992 | A |
5154694 | Kelman | Oct 1992 | A |
5154696 | Shearing | Oct 1992 | A |
5160317 | Costin | Nov 1992 | A |
5180363 | Idemoto et al. | Jan 1993 | A |
5188102 | Idemoto et al. | Feb 1993 | A |
5188589 | Wypych et al. | Feb 1993 | A |
5205817 | Idemoto et al. | Apr 1993 | A |
5222959 | Anis | Jun 1993 | A |
5242385 | Strukel | Sep 1993 | A |
5279547 | Costin | Jan 1994 | A |
5304115 | Pflueger et al. | Apr 1994 | A |
5331951 | Kepley | Jul 1994 | A |
5342293 | Zanger | Aug 1994 | A |
5359996 | Hood | Nov 1994 | A |
5431664 | Ureche et al. | Jul 1995 | A |
5520633 | Costin | May 1996 | A |
5569188 | Mackool | Oct 1996 | A |
5591127 | Barwich, Jr. et al. | Jan 1997 | A |
5676649 | Boukhny et al. | Oct 1997 | A |
5700240 | Barwick, Jr. et al. | Dec 1997 | A |
5722945 | Anis et al. | Mar 1998 | A |
5733256 | Costin | Mar 1998 | A |
5766146 | Barwick, Jr. | Jun 1998 | A |
5808396 | Boukhny | Sep 1998 | A |
5865790 | Bair | Feb 1999 | A |
5938677 | Boukhny et al. | Aug 1999 | A |
6027515 | Cimino | Feb 2000 | A |
6028387 | Boukhny | Feb 2000 | A |
6077285 | Boukhny | Jun 2000 | A |
6083193 | Kadziauskas et al. | Jul 2000 | A |
6175180 | Angelini et al. | Jan 2001 | B1 |
6179805 | Sussman et al. | Jan 2001 | B1 |
6179808 | Boukhny et al. | Jan 2001 | B1 |
6193683 | Ludin et al. | Feb 2001 | B1 |
6241700 | Leukanech | Jun 2001 | B1 |
6261283 | Morgan et al. | Jul 2001 | B1 |
6261297 | Kadziauskas et al. | Jul 2001 | B1 |
6283974 | Alexander | Sep 2001 | B1 |
6315755 | Sussman | Nov 2001 | B1 |
6394974 | Kadziauskas et al. | May 2002 | B1 |
6402769 | Boukhny | Jun 2002 | B1 |
6491661 | Boukhny et al. | Dec 2002 | B1 |
6629948 | Rockley | Oct 2003 | B2 |
6679899 | Wiener et al. | Jan 2004 | B2 |
6699212 | Kadziauskas | Mar 2004 | B1 |
6780165 | Kadziauskas | Aug 2004 | B2 |
7077820 | Kadziauskas et al. | Jul 2006 | B1 |
7229455 | Sakurai et al. | Jun 2007 | B2 |
7297137 | Gordon et al. | Nov 2007 | B2 |
7374552 | Wuchinich | May 2008 | B2 |
7485106 | Kadziauskas et al. | Feb 2009 | B2 |
7645255 | Gordon et al. | Jan 2010 | B2 |
7758538 | Boukhny et al. | Jul 2010 | B2 |
20010001123 | Madan et al. | May 2001 | A1 |
20010011176 | Boukhny | Aug 2001 | A1 |
20030045887 | Sakurai et al. | Mar 2003 | A1 |
20040092800 | Mackool | May 2004 | A1 |
20040092922 | Kadziauskas et al. | May 2004 | A1 |
20060041200 | Dotter et al. | Feb 2006 | A1 |
20060079788 | Anderson et al. | Apr 2006 | A1 |
Number | Date | Country |
---|---|---|
0359217 | Mar 1990 | EP |
1729658 | Dec 2006 | EP |
1765190 | Mar 2007 | EP |
8705793 | Oct 1987 | WO |
9207622 | May 1992 | WO |
9520374 | Aug 1995 | WO |
9918901 | Apr 1999 | WO |
9945868 | Sep 1999 | WO |
0124744 | Apr 2001 | WO |
0141672 | Jun 2001 | WO |
0197728 | Dec 2001 | WO |
0217833 | Mar 2002 | WO |
02056806 | Jul 2002 | WO |
03043550 | May 2003 | WO |
2004080505 | Sep 2004 | WO |
Entry |
---|
Jiromaru Tsujino, “Ultrasonic Motor Using a One-Dimensional Logitudinal-Torsional Vibration Converter with Diagonal Slits,” Smart Mater, Struct. 7 (1998) pp. 345-351. |
Shuyu, Lin “Sandwiched Piezoelectric Ultrasonic Transducers of Longitudinal-Torsional Compound Vibrational Modes.” IEEE Transactions of Ultrasonics, Ferroelectrics and Frequency Control, Nov. 1997, pp. 1189-1197. |
Number | Date | Country | |
---|---|---|---|
20120296264 A1 | Nov 2012 | US |
Number | Date | Country | |
---|---|---|---|
60587693 | Jul 2004 | US | |
60555240 | Mar 2004 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 12577521 | Oct 2009 | US |
Child | 13565875 | US | |
Parent | 11068301 | Feb 2005 | US |
Child | 12577521 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 10818314 | Apr 2004 | US |
Child | 11068301 | US |