Vacuum sense control for phaco pulse shaping

Information

  • Patent Grant
  • 9226849
  • Patent Number
    9,226,849
  • Date Filed
    Thursday, January 3, 2013
    11 years ago
  • Date Issued
    Tuesday, January 5, 2016
    8 years ago
Abstract
A method and apparatus for precisely controlling particle movement relative to a phacoemulsification needle tip is provided. The design monitors actual vacuum present and calculates a pulse shape amplitude waveform proportional to the amount of measured vacuum. An increase in vacuum indicates that the handpiece/needle is becoming occluded by a large particle. The present design determines whether additional power is required to bump or move a large particle away from the needle tip. The present design may employ a control loop that senses and continuously monitors vacuum. The design may dynamically vary the amount of ultrasonic energy delivered to the surgical area in response to the observed actual vacuum, and can actively vary the amount of power delivered to the surgical area based on the size of the particle and the resultant vacuum realized.
Description
BACKGROUND OF THE INVENTION

1. Field of the Invention


The present invention relates generally to the field of surgical tissue removal, and more specifically to ultrasonic power delivery during surgical tissue removal procedures such as phacoemulsification.


2. Description of the Related Art


Phacoemulsification surgery has been successfully employed in the treatment of certain ocular problems, such as cataracts. Phacoemulsification surgery utilizes a small conical incision to insert the tip of at least one phacoemulsification handheld surgical implement, or handpiece. The handpiece includes a needle that is ultrasonically driven once placed within an incision to emulsify the eye lens, or break the cataract into small pieces. The broken cataract pieces may subsequently be removed using the same handpiece or another handpiece in a controlled manner. The surgeon may then insert lens implants in the eye through the incision. The incision is allowed to heal, and the results for the patient are typically significantly improved eyesight.


As may be appreciated, the flow of fluid to and from a patient through a fluid infusion or extraction system and power control of the phacoemulsification handpiece is critical to the procedure performed. Different medically recognized techniques have been utilized for the lens removal portion of the surgery. Among these, one popular technique is a simultaneous combination of phacoemulsification, irrigation and aspiration using a single handpiece. This method includes making the incision, inserting the handheld surgical implement to emulsify the cataract or eye lens. Simultaneously with this emulsification, the handpiece provides a fluid for irrigation of the emulsified lens and a vacuum for aspiration of the emulsified lens and inserted fluids.


Pulse delivery has developed from a simple on/off arrangement through what is known as a burst delivery or pulse delivery, using fixed off periods or fixed duty cycles, to a specific pulse delivery such as the Whitestar pulse delivery method of Advanced Medical Optics Corporation of Santa Ana, Calif. Such designs provide the surgeon with different functionality useful in different phacoemulsification procedures, such as breaking the lens or removing the lens.


Previous systems have employed either an optimum phase angle to affect constant energy transfer into the tissue or apply a modulated voltage amplitude shaping pulse to control the phacoemulsification handpiece. These procedures can produce a significant amount of heat in the affected area. Care must be taken to avoid overheating of eye tissue during phacoemulsification while still performing the desired cutting or removal procedures. The risk of damaging the affected area via application of heat can be a considerable negative side effect.


Conditions may arise during ocular surgeries that reduce the cutting effectiveness of current pulse shaping designs. In particular, one undesirable effect exhibited by these systems is that small particles at the phaco tip can be knocked off from the tip at an undesirable time. The phaco tip must be sufficiently occluded by, or in contact with, the particle in order to effectively remove such particles. In order to circumvent or manage this effect, surgeons typically reduce the voltage amplitude shaping pulse to keep small particles from being knocked off at the tip. This method of reducing the voltage amplitude can materially limit cutting effectiveness. In general, blockage of the phaco tip dramatically reduces cutting effectiveness, as does any overall reduction in voltage amplitude applied.


Typical available systems may employ what is known as an occluded mode, wherein an occlusion or blockage of the phaco tip, such as by a piece of lens, is addressed in some manner. The typical way of addressing occlusion has been to cease operation until the tip is no longer occluded, i.e. simply releasing the pressure applied to the tip. This enables the operator/surgeon to manually move the tip and allow the occlusion to disengage from the instrument. such an implementation simply monitors the pressure of vacuum on the tip, and when it exceeds a certain amount, the vacuum is released or no longer applied.


Increased efficiency in this environment is desirable, such that any devices or procedures that can lessen heat applied to the affected area or simplify the work of the operator surgeon is beneficial. Patient recovery time can be enhanced when desirable performance is provided, such as reduced heat to the affected region.


Based on the foregoing, it would be advantageous to provide a system that employs a wave pulse shaping mechanism that enables successful surgeries without delivering excessive heat to the surgical site, and allows operators to operate the phacoemulsification system effectively under both occluded and non-occluded conditions. It would also be beneficial to overcome the aforementioned drawbacks present in previously known ultrasonic tissue removal systems.


SUMMARY OF THE INVENTION

According to one aspect of the present design, there is provided a method of delivering ultrasonic energy during a surgical procedure, such as a phacoemulsification procedure. The method comprises applying at least one pulse, and typically multiple pulses, each having a pulse shape. The pulse shape comprises a predetermined pulse shape portion and either an increased energy portion comprising an increase in energy proportional to an increase in sensed aspiration vacuum pressure or a decreased energy portion comprising a decrease in energy proportional to a decrease in sensed aspiration vacuum pressure.


According to a second aspect of the present design, there is provided an apparatus comprising a device configured to encounter vacuum pressure at the surgical area, a vacuum sensor configured to monitor vacuum pressure encountered by the device, and a computer configured to compute an ultrasonic pulse profile for delivery to a needle configured to vibrate based on the ultrasonic pulse profile received, the ultrasonic pulse profile based on monitored vacuum pressure received from the vacuum sensor. The ultrasonic pulse profile comprises a baseline ultrasonic pulse region and an altered ultrasonic pulse region, the altered ultrasonic pulse region comprising a pulse portion altered based on monitored vacuum pressure.


These and other advantages of the present invention will become apparent to those skilled in the art from the following detailed description of the invention and the accompanying drawings.





DESCRIPTION OF THE DRAWINGS

The present invention is illustrated by way of example, and not by way of limitation, in the figures of the accompanying drawings in which:



FIG. 1 is a functional block diagram of a phacoemulsification system in accordance with the present invention;



FIG. 2 is a flowchart illustrating the operation of a phacoemulsification system with variable ultrasonic power levels;



FIG. 3 illustrates a standard phacoemulsification ultrasonic wave shape, actual vacuum on aspiration line, and a calculated pulse shape amplitude waveform;



FIG. 4 illustrates a calculated pulse shape amplitude waveform superimposed on a standard phacoemulsification ultrasonic wave shape to produce a pulse shape amplitude wave shape;



FIGS. 5A-F show alternate examples of wave shapes according to the present design; and



FIG. 6 shows an exemplary wave shape according to another embodiment of the present design.





DETAILED DESCRIPTION OF THE INVENTION

The following description and the drawings illustrate specific embodiments to enable those skilled in the art to practice the system and method described. Other embodiments may incorporate structural, logical, process and other changes. Examples merely typify possible variations. Individual components and functions are generally optional unless explicitly required, and the sequence of operations may vary. Portions and features of some embodiments may be included in or substituted for those of others.


Currently available phacoemulsification systems include a variable speed peristaltic pump, a vacuum sensor, an adjustable source of ultrasonic power, and a programmable microprocessor with operator-selected presets for controlling aspiration rate, vacuum and ultrasonic power levels. A phacoemulsification handpiece is interconnected with a control console by an electric cable for powering and controlling the piezoelectric transducer. Tubing provides irrigation fluid to the eye and enables withdrawal of aspiration fluid from an eye through the handpiece. The hollow needle of the handpiece may typically be driven or excited along its longitudinal axis by the piezoelectric effect in crystals created by an AC voltage applied thereto. The motion of the driven crystal is amplified by a mechanically resonant system within the handpiece such that the motion of the needle connected thereto is directly dependent upon the frequency at which the crystal is driven, with a maximum motion occurring at a resonant frequency. The resonant frequency is dependent in part upon the mass of the needle interconnected therewith, which is typically vibrated by the crystal.


One similar system and design is illustrated in U.S. patent application Ser. No. 10/387,335, entitled “Modulated Pulsed Ultrasonic Power Delivery System and Method,” inventors Kenneth E, Kadziauskas et al., filed Mar. 12, 2003, the entirety of which is incorporated herein by reference.


Power control of the phacoemulsification handpiece is highly critical to successful phacoemulsification surgery. Certain previous systems address the requirements of power control for a phacoemulsification handpiece based on the phase angle between the voltage applied to a handpiece piezoelectric transducer and the current drawn by the piezoelectric transducer and/or the amplitude of power pulses provided to the handpiece. The typical arrangement is tuned for the particular handpiece, and power is applied in a continuous fashion or series of solid bursts subject to the control of the surgeon/operator. In certain circumstances, the surgeon/operator may wish to apply these power bursts for a duration of time, cease application of power, then reapply at this or another power setting. The frequency and duration of the burst is typically controllable, as is the length of the stream of bursts applied to the affected area. The time period where power is not applied enables cavitation in the affected area, and broken lens sections may be removed using aspiration provided by the handpiece or an aspiration apparatus. The on/off application of power facilitates breaking the cataract into pieces and relatively efficient removal thereof.


The present design provides a system and method for precisely controlling the movement of the phacoemulsification needle tip using a pulse shape controlled, or partially based on, sensed vacuum pressure. Controlling particle movement at the needle tip may enable better destruction (i.e. emulsification) of large and small particles. The present vacuum based design determines whether additional energy is required to bump or move a large particle away from the needle tip. The system may determine less energy is needed to enable a smaller particle to be drawn to the needle tip. The present design can include a control loop to sense and continuously monitor actual vacuum at the needle tip, and the design may vary the amount of ultrasonic power delivered to the surgical area in response to the observed actual needle tip vacuum. Moreover, the present design may actively vary the amount of ultrasonic power delivered based on the size of the particle, directly proportional to measured vacuum.



FIG. 1 illustrates a phacoemulsification system in block diagram form. The system has a control unit 105, indicated by the dashed lines in FIG. 1 that includes a source of pulsed ultrasonic power 107, a microprocessor computer 109 that provides control outputs to ultrasonic power level controller 111, and a vacuum source 115. A vacuum sensor 113 may continuously monitor and report the actual value of vacuum observed on line 110 and may provide these values for input to computer 109 representing the vacuum level, or actual vacuum level, received on the input side of vacuum source 115. Vacuum source 115 represents a vacuum source typically included within control unit or phacoemulsification device 105, generating a vacuum and attached to the line 110 and interfacing with computer 109 to provide actual vacuum pressure readings dynamically and receive signals to, for example, increase or decrease vacuum applied. Vacuum source may be provided separately from control unit 105.


The block representation of the handpiece 104 includes a needle and electrical means, typically a piezoelectric crystal, for ultrasonically vibrating the needle. The control unit 105 supplies power on line 102 to a phacoemulsification handpiece/needle 104. An irrigation fluid source is fluidly coupled to handpiece/needle 104 (not shown in FIG. 1). The irrigation fluid at 116 and ultrasonic power at 117 are applied by handpiece/needle 104 to a patient's eye, or affected area or region, indicated diagrammatically by block 106. Alternatively, the irrigation source may be routed to the eye 106 through a separate pathway independent of the handpiece. The eye 106 is aspirated by the using vacuum source 115 through line/handpiece needle 108 and line 110. Control unit 105 manages the amount of aspiration provided. A switch 112 disposed on the handpiece 104 may be utilized to enable a surgeon/operator to select an amplitude of electrical pulses to the handpiece via the computer 109, power level controller 111 and ultrasonic power source 107 as discussed herein. Any suitable input device such as for example, a foot pedal (not shown) may be utilized in lieu of the switch 112.


The control unit 105 may include a manual user interface 120 to allow the surgeon/operator to preset various system parameters. User defined system parameters may include, but are not limited to, selecting pulse shape amplitude mode, setting maximum vacuum, minimum pulse shape amplitude, and maximum pulse shape amplitude. In addition, the computer 109 may provide operator-lettable limits for aspiration rates, vacuum levels and ultrasonic power levels. The surgeon/operator may select the pulse shape amplitude (PSA) mode during any phase of an operational procedure via the manual user interface 120 console. Selection of PSA mode may direct the microprocessor computer 109 to continuously monitor the resultant vacuum at line/handpiece needle 108 by measuring the pressure on line 110 via vacuum sensor 113. The computer 109 may respond to a surgeon selected preset maximum vacuum level and preset minimum and maximum PSA values using signals from the vacuum sensor 113. If the received vacuum from vacuum sensor 113 exceeds a maximum vacuum level as set by the surgeon, an occluded condition exists, and the system can halt vacuum pressure in an effort to enable occlusion removal.


Operation of the control unit 105 in response to an occluded-unoccluded condition of handpiece 104 is shown in the flow diagram of FIG. 2. An occluded handpiece/needle 104 condition may arise when a large particle becomes held by vacuum at the handpiece/needle 104 tip. This situation is found to reduce the phacoemulsification cutting efficiency. Furthermore, large particles tend to be more readily emulsified when the particle is moved away from the handpiece/needle 104 tip. Conversely, an unoccluded handpiece/needle 104 may arise when a small particle is not held firmly in position and may fall off the handpiece/needle 104. In this situation, a reduction in ultrasonic power delivered may allow the smaller particle to be moved closer to the needle tip and may improve small particle destruction.


The present design may continuously vary the ultrasonic power delivered to the surgical area in response to particle size as determined by actual vacuum present on the aspiration line 108. Although the present design is described in terms of varying pulse shaping amplitude as a function of vacuum, alternate embodiments of the present design may include varying other system parameters such as phaco power and duty cycle as a function of vacuum, vacuum level, or vacuum pressure. Note that as used herein, the term “vacuum” is intended to mean any type of negative pressure, including a vacuum condition, vacuum level, or vacuum pressure.


As illustrated in FIG. 2, the surgeon/operator may enable PSA mode at point 201. The present design may continuously monitor actual vacuum level at point 202, where actual vacuum level represents the vacuum level present on line/handpiece needle 108 and line vacuum line 110. Microprocessor computer 109 may calculate a desired PSA level at point 203, where desired PSA level is typically a function of actual vacuum level, but may be a fixed value or function. The resulting PSA level obtained from this calculation may indicate to computer 109 a need to change the PSA level. Computer 109 may change the amount of ultrasonic energy delivered by supplying signals to power level controller 111 to generate an PSA wave shape at point 204 to increase, decrease, or maintain the amount of energy delivered. Power level controller 111 may superimpose the PSA wave shape at point 206 with the standard wave shape at point 205 resulting in an increase or decrease in ultrasonic power delivered based on actual vacuum level.


In this manner, the present design may dynamically change the total amount of energy delivered to the surgical area in real-time based on conditions encountered, specifically vacuum pressure received or sensed. The present design may provide a continuous control loop for increasing or decreasing the amount of ultrasonic energy delivered by performing an PSA wave shape function at point 207 based on the combination of the standard wave shape at point 205 modified by the PSA waveform at point 204 in response to measured vacuum. If the surgeon/operator elects to disable the PSA mode at point 201, the phacoemulsification system generates the standard phaco wave shape (e.g. burst, pulsed, etc.) at point 208 and performs the standard phaco wave shape at point 209.


The present design may calculate the pulse shape amplitude based on the following equation:

PSA=MinAmp+[(ActualVac)*(MaxAmp−MinAmp)]/(MaxVac)  (1)

where: MaxAmp=maximum pulse shape amplitude, MinAmp=minimum pulse shape amplitude, ActualVac=actual vacuum, MaxVac=maximum vacuum, and PSA=pulse shape amplitude.


Equation (1) provides valid pulse shape amplitude values for MaxVac values greater than zero, Table 1 provides resultant PSA values calculated based on an example of an implementation of Equation (1) using the following values:

MaxVac=200 mm/hg;
MinAmp=10%; and


MaxAmp=40%, where the percentage value represents percent above unmodified signal amplitude, 10% represents 10 percent above existing or nominal amplitude, or 110% of nominal,









TABLE 1







Example of Calculated PSA Versus Actual Vacuum










ActualVac
PSA














0
10%



10
11.5%  



20
13%



40
16%



60
19%



80
22%



100
25%



150
32.5%  



200
40%










PSA is calculated as a percentage of the nominal wave amplitude generated by the phaco system, FIG. 3 illustrates the relationships between a standard phacoemulsification ultrasonic wave shape, actual vacuum measured on the aspiration line, and a calculated pulse shape amplitude waveform. Graph A in FIG. 3 represents an exemplary burst mode phaco wave shape with a duty cycle of 33%. The ultrasonic power on time is shown at point 301 with fixed amplitude. The ultrasonic power off time is shown at point 302. Although a phaco burst mode wave shape is shown, the present design may be applied to any standard or even non-standard phaco wave shape including a shape generated using pulse mode. Burst mode and pulse mode wave shapes known in the art. Graph B in FIG. 3 represents an example of actual vacuum measured on the aspiration line. In this example, the linear increase in vacuum pressure shown at point 303 may represent a larger particle beginning to occlude the phaco tip opening. Although the example is shown as having a linear increase in vacuum for simplicity, the present design may accommodate any dynamic changes in actual real-time vacuum. This occlusion may cause vacuum to build to a higher level as the phaco tip becomes more completely blocked off. The vacuum level at point 304 represents reaching the MaxVac as preset by the surgeon/operator in this example. This may represent a completely blocked off or occluded phaco needle tip.


The vacuum level at point 305 may represent a decrease in vacuum as the large particle is bumped or moved away from the phaco needle tip. Movement may result in a decrease in observed vacuum present of the aspiration line. The vacuum level at point 306 is representative of a large particle being precisely held away from the tip to ensure the most efficient destruction or emulsification of the large particle. The present design may generate the pulse shape amplitude waveform represented in Graph C in FIG. 3 based on the observed vacuum (Graph B) and the standard phaco wave shape either selected or provided (Graph A).


Based on the PSA equation, the present design may generate the pulse shape amplitude waveform with an ultrasonic on time at point 310 and off time at point 311. This generated PSA waveform amplitude is 10 percent greater than the standard wave shape shown in Graph A in accordance with a measured vacuum of 0 mm/hg. As vacuum pressure increases from 0 mm/hg to 200 mm/hg, the present design may generate the PSA waveforms shown at points 312, 313, 314 and 315. The PSA waveform increases proportionally to actual vacuum until the MaxVac value is reached.


In this example, the present design may generate a PSA waveform with amplitude 40 percent greater than the standard phaco wave shape shown in Graph A. The actual vacuum at point 304 may represent an occluded phaco needle tip. As the phaco power is increased via the PSA waveform augmentation to the standard or nominal waveform, the large particle may begin to move away from the needle and thus cause a drop in vacuum at point 305. As the large particle moves away from the Phaco needle tip, the needle tip may hold the large particle at a distance from the needle tip, enhancing emulsification of the particle. Large particle movement may be controlled or held in the present design by reducing the PSA waveform amplitude at point 316 in accordance with actual vacuum at point 306.


The amplitude of the wave generated may vary, but also the duration of the pulse and the additional amplitude spike may vary depending on circumstances. In general, a fairly short amplitude spike is added to the nominal waveform, where amplitude of the spike is dependent upon the calculation of Equation (1) or some similar vacuum based function.



FIG. 4 illustrates a calculated pulse shape amplitude waveform 401 superimposed on a standard phacoemulsification ultrasonic wave shape 402 in Graph A. The present design may combine or sum these two ultrasonic power signals to produce a modified ultrasonic wave shape for phacoemulsification as shown in Graph B of FIG. 4. This combination may form the pulse shape amplitude wave shape, Graph B represents a PSA wave shape in accordance with the vacuum profile shown in Graph B of FIG. 3. The ultrasonic profile represented at point 403 shows a 10% increase in amplitude generated by the present design for an actual vacuum of 0 mm/hg. The ultrasonic profile represented at point 404 shows a 40% increase in amplitude generated by the present design for an actual vacuum of 200 mm/hg. The ultrasonic profile represented at point 405 shows a 25% increase in amplitude generated by the present design for an actual vacuum of 100 mm/hg.


The ultrasonic power wave shape shown in Graph B of FIG. 4 represents an unoccluded condition at point 403, followed by an occluded condition at point 404 as a large particle is drawn closer and held at the phaco needle tip opening. Movement of the large particle away from the phaco needle tip occurs at point 405 due to the increased phaco power delivered at point 404. This increased power moves or bumps the large particle away from the phaco needle tip. In this automated configuration, the present design may enable the surgeon/operator to use less force to dissipate an occlusion by increasing the ultrasonic power as vacuum increases, thereby allowing the particle to be held firmly in position during emulsification. The present design may indicate to the surgeon the size of the particle by observing actual vacuum. In addition, the control loop mechanism within the present design may enable the surgeon to self-feed said particles at the phaco needle tip. The ability to self-feed large and small particles may eliminate the need for a second surgical instrument to push particles towards the phaco tip, as required by many currently deployed systems.


The present design has been described using an exemplary square wave phacoemulsification burst mode wave shape. As noted, although the description relates to how the present design modifies the amplitude of a standard pulse wave shape, the present design may alternately or additionally modify the width of the PSA waveform. In this arrangement, additional ultrasonic power may be delivered to the surgical area as required.


The illustrations presented in FIGS. 5A-5F illustrate pulses provided with enhanced amplitude that vary in duration, from a small percentage of the overall pulse width to a large percentage of pulse width. FIG. 5A illustrates one embodiment of a PSA wave shape. FIG. 5B illustrates a PSA wave shape with an increase in pulse shape amplitude over that shown in FIG. 5A. FIG. 5C illustrates an exemplary PSA wave shape wherein the width of the PSA waveform has been increased over that shown in FIG. 5A. Similarly, FIG. 5D illustrates an exemplary PSA wave shape wherein the width of the PSA waveform has been increased over that shown in FIG. 5B. FIG. 5E illustrates an exemplary PSA wave shape wherein the width of the PSA waveform has been increase over that shown in FIG. 5C, and FIG. 5F illustrates an exemplary PSA wave shape wherein the width of the PSA waveform has been increase over that shown in FIG. 5D.


The present design may modify amplitude and width of the PSA waveform in order to provide the desired ultrasonic power for efficient phacoemulsification of large and small particles.


The present design is not limited to generating square waves in response to the standard generated phaco wave shape. Other similar waveforms may be employed and depend on the environment encountered, including but not limited to phaco conditions, tip size, operating frequency, fluid conditions, and occlusion conditions. FIG. 6 illustrates an alternate aspect of the invention wherein rounded wave 600, or graduated power delivery curves are applied to the surgical area. In general, the rounded waveform follows the teachings presented herein, wherein pulse applied is based on vacuum pressure received and comprises a PSA enhanced amplitude region and a standard wave region. Other waveforms may be employed but are generally based in some form on vacuum pressure encountered.


A further aspect of the present design may include varying the time and power levels based on actual vacuum to attain transient cavatation as quickly as possible in the surgical environment without generating significant heat in the region. As may be appreciated by those skilled in the art, sufficient power is delivered based on the circumstances presented to induce transient cavatation, typically by delivering an initial higher power surge or burst of energy, followed by a drop off in energy from the initial surge in accordance with the present design.


Thus the present design delivers ultrasonic energy during a surgical procedure, such as a phacoemulsification procedure, and comprises applying at least one pulse and typically multiple pulses each having a pulse shape. The pulse shape comprises a predetermined pulse shape portion and either an increased energy portion comprising an increase in energy proportional to an increase in sensed aspiration vacuum pressure or a decreased energy portion comprising a decrease in energy proportional to a decrease in sensed aspiration vacuum pressure. Alternately, the design monitors actual vacuum pressure level at the surgical region, dynamically calculates a pulse shape amplitude (PSA) level based on monitored actual vacuum pressure level, generates a PSA waveform based on the dynamically calculating, and sums a predetermined wave shape with the PSA waveform to produce a PSA wave shape. The design then delivers the PSA wave shape to a handpiece.


The design may be embodied in an apparatus comprising a device configured to encounter vacuum pressure at the surgical area, a vacuum sensor configured to monitor vacuum pressure encountered by the device, and a computer configured to compute an ultrasonic pulse profile for delivery to a needle configured to vibrate based on the ultrasonic pulse profile received, the ultrasonic pulse profile based on monitored vacuum pressure received from the vacuum sensor. The ultrasonic pulse profile comprises a baseline ultrasonic pulse region and an altered ultrasonic pulse region, the altered ultrasonic pulse region comprising a pulse portion altered based on monitored vacuum pressure.


As may be appreciated by those skilled in the art, the present design may be realized in software executing in microprocessor computer 109, or may be implemented with dedicated microcontrollers or analog circuitry.


The foregoing is not determinative or exclusive or inclusive of all components, interfaces, communications, and operational modes employable within the present design. The design presented herein and the specific aspects illustrated are meant not to be limiting, but may include alternate components while still incorporating the teachings and benefits of the invention, namely a method of generating a pulse shape amplitude in an arrangement that modifies phaco ultrasonic power delivered proportional to actual vacuum present. While the invention has thus been described in connection with specific embodiments thereof, it will be understood that the invention is capable of further modifications. This application is intended to cover any variations, uses or adaptations of the invention following, in general, the principles of the invention, and including such departures from the present disclosure as come within known and customary practice within the art to which the invention pertains.

Claims
  • 1. An apparatus for controlling ultrasonic power delivery to a surgical area, comprising: a device configured to encounter vacuum pressure at the surgical area;a vacuum sensor configured to monitor vacuum pressure encountered by said device; anda computer configured to compute an ultrasonic pulse profile for delivery to a needle configured to vibrate based on the ultrasonic pulse profile received, the ultrasonic pulse profile based on monitored vacuum pressure received from the vacuum sensor, wherein the computer is further configured to compute and apply at least one pulse to the needle, each pulse having an ultrasonic pulse shape formed based on actual sensed vacuum pressure;wherein the formed ultrasonic pulse shape comprises a predetermined ultrasonic pulse shape portion superimposed on an altered ultrasonic pulse shape portion;wherein the altered ultrasonic pulse shape portion is either an increased energy portion comprising an increase in energy proportional to an increase in sensed vacuum pressure or a decreased energy portion comprising a decrease in energy proportional to a decrease in sensed vacuum pressure, and wherein the increased energy portion and decreased energy portion are determined based upon a ratio of actual sensed vacuum pressure to maximum sensed vacuum pressure, taking into account the maximum pulse amplitude and minimum pulse amplitude.
  • 2. The apparatus of claim 1, wherein the device comprises the needle.
  • 3. The apparatus of claim 2, wherein the computer delivers the ultrasonic pulse profile to the needle so that movement of the needle induces transient cavitation within fluid within the surgical area.
  • 4. The apparatus of claim 2, wherein the surgical area is an eye and the apparatus is for controlling ultrasonic power delivery during a phacoemulsification procedure.
  • 5. The apparatus of claim 1, wherein the needle is within a second device.
  • 6. The apparatus of claim 5, wherein the computer delivers the ultrasonic pulse profile to the needle so that movement of the needle induces transient cavitation within fluid within the surgical area.
  • 7. The apparatus of claim 5, wherein the surgical area is an eye and the apparatus is for controlling ultrasonic power delivery during a phacoemulsification procedure.
  • 8. The apparatus of claim 1, wherein the computer delivers the ultrasonic pulse profile to the needle so that movement of the needle induces transient cavitation within fluid within the surgical area.
  • 9. The apparatus of claim 1, wherein the surgical area is an eye and the apparatus is for controlling ultrasonic power delivery during a phacoemulsification procedure.
  • 10. The apparatus of claim 1, wherein the increased energy portion and the decreased energy portion are computed based on actual sensed vacuum pressure multiplied by maximum pulse amplitude minus minimum pulse amplitude and divided by maximum sensed vacuum pressure, added to minimum pulse amplitude.
  • 11. The apparatus of claim 1, wherein the computer is configured so that the applying comprises applying multiple pulses each comprising an individual pulse shape formed based on actual sensed vacuum pressure.
  • 12. The apparatus of claim 1, wherein the vacuum pressure is an aspiration vacuum pressure.
Parent Case Info

This application is a divisional of and claims priority to U.S. application Ser. No. 13/473,959 filed on May 17, 2012, which is a continuation U.S. application Ser. No. 13/196,559 filed on Aug. 2, 2011, now U.S Pat. No. 8,202,287, that issued on Jun. 19, 2012, which is a continuation of U.S. application Ser. No. 12/684,657, filed on Jan. 8, 2010, now U.S. Pat. No. 7,998,156, that issued on Aug. 16, 2011, which is a continuation of U.S. application Ser. No. 11/461,741 filed on Aug. 1, 2006, now U.S. Pat. No. 7,785,336, that issued on Aug. 31, 2010 each of which is hereby incorporated by reference in its entirety.

US Referenced Citations (114)
Number Name Date Kind
2434480 Anderson Jan 1948 A
3857387 Shock Dec 1974 A
3941122 Jones Mar 1976 A
4184510 Murry et al. Jan 1980 A
4343111 Inoue Aug 1982 A
4736130 Puskas Apr 1988 A
4808948 Patel et al. Feb 1989 A
4827911 Broadwin et al. May 1989 A
4952834 Okada Aug 1990 A
4954960 Lo et al. Sep 1990 A
4970656 Lo et al. Nov 1990 A
4983901 Lehmer Jan 1991 A
5001649 Lo et al. Mar 1991 A
5091656 Gahn Feb 1992 A
5209221 Riedlinger May 1993 A
5213569 Davis May 1993 A
5242404 Conley et al. Sep 1993 A
5249121 Baum et al. Sep 1993 A
5268624 Zanger Dec 1993 A
5279547 Costin Jan 1994 A
5318563 Malis et al. Jun 1994 A
5331951 Kepley Jul 1994 A
5342293 Zanger Aug 1994 A
5370602 Kepley Dec 1994 A
5388569 Kepley Feb 1995 A
5403307 Zelman Apr 1995 A
5405614 D'angelo et al. Apr 1995 A
5406503 Williams, Jr. et al. Apr 1995 A
5417246 Perkins et al. May 1995 A
5431664 Ureche et al. Jul 1995 A
5453087 Malinowski Sep 1995 A
5520633 Costin May 1996 A
5534741 Smith Jul 1996 A
5547459 Kaufman et al. Aug 1996 A
5582578 Zhong et al. Dec 1996 A
5591127 Barwick, Jr. et al. Jan 1997 A
5700240 Barwick et al. Dec 1997 A
5733256 Costin Mar 1998 A
5738677 Colvard et al. Apr 1998 A
5766146 Barwick, Jr. Jun 1998 A
5797494 Balling et al. Aug 1998 A
5800365 Zhong et al. Sep 1998 A
5808396 Boukhny Sep 1998 A
5836959 Seibel et al. Nov 1998 A
5852794 Staggs Dec 1998 A
5873885 Weidenbenner Feb 1999 A
5938677 Boukhny et al. Aug 1999 A
5979494 Perkins et al. Nov 1999 A
5984882 Rosenschein et al. Nov 1999 A
5997528 Bisch et al. Dec 1999 A
6010496 Appelbaum et al. Jan 2000 A
6027515 Cimino Feb 2000 A
6083193 Kadziauskas et al. Jul 2000 A
6086598 Appelbaum et al. Jul 2000 A
6117126 Appelbaum et al. Sep 2000 A
6155975 Urich et al. Dec 2000 A
6161545 Chow Dec 2000 A
6175180 Angelini et al. Jan 2001 B1
6193683 Ludin et al. Feb 2001 B1
6203516 Kepley Mar 2001 B1
6251113 Appelbaum et al. Jun 2001 B1
6261297 Kadziauskas et al. Jul 2001 B1
6319220 Bylsma Nov 2001 B1
6391020 Kurtz et al. May 2002 B1
6391042 Cimino May 2002 B1
6394974 Kadziauskas et al. May 2002 B1
6425883 Urich et al. Jul 2002 B1
6428531 Visuri et al. Aug 2002 B1
6443900 Adachi et al. Sep 2002 B2
6452120 Chen Sep 2002 B1
6452123 Chen Sep 2002 B1
6452883 Chan Sep 2002 B2
6487447 Weimann et al. Nov 2002 B1
6506176 Mittelstein et al. Jan 2003 B1
6589204 Sussman et al. Jul 2003 B1
6610052 Furumoto Aug 2003 B2
6629948 Rockley et al. Oct 2003 B2
6699212 Kadziauskas et al. Mar 2004 B1
6726679 Dick et al. Apr 2004 B1
6733491 Kadziauskas et al. May 2004 B2
6780165 Kadziauskas et al. Aug 2004 B2
6808396 Kawaguchi et al. Oct 2004 B2
6884252 Urich et al. Apr 2005 B1
6890332 Truckai et al. May 2005 B2
6896674 Woloszko et al. May 2005 B1
6908472 Wiener et al. Jun 2005 B2
6939317 Zacharias Sep 2005 B2
6962583 Kadziauskas et al. Nov 2005 B2
7077820 Kadziauskas et al. Jul 2006 B1
7169123 Kadziauskas et al. Jan 2007 B2
7193521 Moberg et al. Mar 2007 B2
7316664 Kadziauskas et al. Jan 2008 B2
7485106 Kadziauskas et al. Feb 2009 B2
8202287 Staggs Jun 2012 B2
20010003155 Rockley et al. Jun 2001 A1
20010003295 Langlotz et al. Jun 2001 A1
20010003385 Ise Jun 2001 A1
20020052600 Davison et al. May 2002 A1
20020072741 Sliwa, Jr. et al. Jun 2002 A1
20020082793 Kadziauskas et al. Jun 2002 A1
20040092921 Kadziauskas et al. May 2004 A1
20040092922 Kadziauskas et al. May 2004 A1
20040193182 Yaguchi et al. Sep 2004 A1
20050054971 Steen et al. Mar 2005 A1
20050209560 Boukhny et al. Sep 2005 A1
20050209621 Gordon et al. Sep 2005 A1
20050288665 Woloszko Dec 2005 A1
20060149301 Claus Jul 2006 A1
20060195077 Kadziauskas et al. Aug 2006 A1
20060264809 Hansmann et al. Nov 2006 A1
20070056596 Fanney et al. Mar 2007 A1
20070073214 Dacquay et al. Mar 2007 A1
20070078379 Boukhny et al. Apr 2007 A1
20080146989 Zacharias Jun 2008 A1
Foreign Referenced Citations (23)
Number Date Country
2242328 May 1998 CA
19940712 Mar 2001 DE
270819 Jun 1988 EP
270819 Jan 1989 EP
336620 Oct 1989 EP
336620 Dec 1993 EP
1351631 Oct 2003 EP
1537840 Jun 2005 EP
2204337 Aug 1990 JP
5038343 Feb 1993 JP
6183762 Jul 1994 JP
6189972 Jul 1994 JP
9313496 Dec 1997 JP
2001161740 Jun 2001 JP
2002087836 Mar 2002 JP
2002233534 Aug 2002 JP
9520374 Aug 1995 WO
9808442 Mar 1998 WO
0051508 Sep 2000 WO
0064388 Nov 2000 WO
0113838 Mar 2001 WO
02056806 Jul 2002 WO
2005092023 Oct 2005 WO
Non-Patent Literature Citations (4)
Entry
Devine M.D., et al., “How to Set the Dials,” Phacoemulsification Surgery, 1991, pp. 7-28.
“Ocusystem Operation Manual, May 1995, 79 pages,”.
“Pulsar cuts phaco time, boots efficiency in cataract removal; Ophthalmology Times: Aug. 15, 1986; 1 page, 11 (16), Harcourt Brace Jovanovich, Inc,”.
Taylor W.F.,et al., “Intraoperative Troubleshooting of an Advanced Phacoemulsification System,” The Surgial Technologist, 1985, vol. 17 (2), pp. 11-14.
Related Publications (1)
Number Date Country
20140018724 A1 Jan 2014 US
Divisions (1)
Number Date Country
Parent 13473959 May 2012 US
Child 13733688 US
Continuations (3)
Number Date Country
Parent 13196559 Aug 2011 US
Child 13473959 US
Parent 12684657 Jan 2010 US
Child 13196559 US
Parent 11461741 Aug 2006 US
Child 12684657 US