The present invention relates to electrosurgical and/or thermal surgical instruments. More specifically, the present invention relates to a system and method of controlling the delivery of power from an energy source to the instrument.
It is becoming more common to use electrosurgical and/or thermal devices during surgery because such devices may provide benefits over traditional medical devices. For example, electrosurgical and/or thermal devices may allow a surgeon to make precise incisions with limited blood loss. Because of their advantages, electrosurgical and/or thermal devices may be used in dermatological, gynecological, cardiac, plastic, ocular, spine, ENT, maxillofacial, orthopedic, urological, neurological and general surgical procedures as well as certain dental procedures, just to name a few.
Surgery generally involves cutting, repairing and/or removing tissue or other materials. Electrosurgical and/or thermal instruments may be used to perform each of these procedures by using the electrosurgical and/or thermal instrument to heat the tissue or other material to a desired temperature. Tissue may react differently, however, at different temperatures. If the temperature of the electrosurgical and/or thermal instrument is not properly controlled, then undesired results may occur which may lead to an adverse outcome for the patient.
Furthermore, a surgeon may be required to use an electrosurgical and/or thermal instrument for a prolonged period of time during a given procedure. During this time the instrument may be intermittently moved in and out of contact with a portion of the patient's body. This can lead to problems both with heat management within the device itself as well as heat management of the heated surgical tip of the instrument. When the instrument is not in contact with a portion of the patient's tissue, body fluid, etc., e.g. it is held in the air above the patient's body, it may be important to limit the power delivered to the instrument to minimize transfer of heat to areas of the instrument where heat is unwanted or even detrimental. For example, if heat transfer to a portion of the electro surgical and/or thermal instrument which is gripped by the surgeon is not properly controlled, the device may become too hot and the surgeon may not be able to handle the instrument for the time necessary to complete the procedure.
Additionally, if the active portion of the electrosurgical and/or thermal instrument, such as a thermal element, is overheated or exposed to excessive thermal stress, the thermal element may be damaged.
Thus there is a need for improved system and method of controlling the delivery of power from an energy source to an electrosurgical and/or thermal surgical instrument to prevent overheating of the instrument and/or the heated surgical tip.
It is an object of the present invention to provide an improved electrosurgical and/or thermal surgical instrument.
According to one aspect of the invention, the instrument may include software and hardware to manage power delivery from an energy source to the instrument.
According to another aspect of the invention, controlling power delivery to the electrosurgical instrument may include using an algorithm which varies the power delivery to an active element of the instrument, thus varying the operational characteristics of the instrument according to the environment of the active element (e.g. whether the active element is being used for tissue treatment or being held in the air). The algorithm may be managed at a fixed power index between about 5 W and 125 W and may be used to deliver a desired power to the electrosurgical and/or thermal surgical instrument in a consistent manner, prevent the active element of the instrument from exceeding the Curie point, and/or prevent overheating of the instrument when the active element is in the air. The control algorithm may allow a surgeon to use the optimal temperature for a desired tissue effect, and also allow the surgeon to select surgical tips having different configurations while providing the desired control when using these different surgical tips.
According to another aspect of the invention, controlling power delivery to the electrosurgical instrument may include using a single or cascaded proportional-integral-derivative controller (“PID”) for forward power or net power, PID tip current limiting control, standing wave ratio (“SWR”) threshold limiting, and/or Load/Air detection.
According to another aspect of the invention, the thermal surgical instrument may include a handpiece responsible for current sensing, temperature sensing, impedance sensing, etc.
According to another aspect of the invention, current data, temperature data, impedance data, etc. which is sensed by the handpiece, or other parts of the thermal surgical instrument, may be sent to a control console which includes a microcontroller, microprocessor, or the like.
According to another aspect of the invention, current data, temperature data, impedance data, etc. may be sent to a control console on a substantially continuous basis. For example, the data may be sent to the control console at intervals of about 10 milliseconds.
According to another aspect of the invention, the surgical instrument may include a thermal element. The thermal element may include, for example, a conductor having a ferromagnetic material plated thereon, a solid ferromagnetic heating element, a ferromagnetic sleeve disposed on an insulated conductor such that heating of the ferromagnetic sleeve is substantially purely inductive, etc.
According to another aspect of the invention, the thermal element of the thermal surgical instrument may be removably received by a handpiece so that various thermal element may be used with the handpiece.
According to another aspect of the invention, a surgical instrument may include information necessary to manage the power output of the thermal element, which may differ according to the shape, dimension, or configuration of the thermal element (e.g., blade, loop, snare, forceps, shears, minimally invasive surgery instruments, probes, catheters etc.). For example, the information may be stored in a single storage device (such as an EEPROM, flash device, lasered ROM or fram, etc.) located in the handpiece, or multiple storage devices located at various locations on a surgical instrument system of the present invention.
According to another aspect of the invention, a surgical instrument may include the following information necessary to manage the power output of the thermal element, such as: current limit; allowable power settings; SWR limit by power level; serial number; calibration constants; tip identification; timing constants (e.g. cool down); etc.
According to another aspect of the invention, the thermal surgical instrument system may include software. The software may use information received from the thermal surgical instrument to implement a variable stage state machine. For example, the software may receive information from a handpiece, tip, and/or power meter of the thermal surgical instrument to implement a 5-stage state machine. The stages of the state machine may include RF On (e.g. RF power has just been enabled), Air (the thermal element of the surgical instrument is in air), Pre-Load (the thermal element is suspected to be in tissue), Transition (the thermal element is suspected to be transitioning from tissue to air), and Load (the tip is confirmed to be in tissue).
According to still another aspect of the invention, controlling power delivery to the thermal surgical instrument may include a power profile control algorithm which includes a group of start/end duration segments to intermittently increase the power delivered to the tip of an electrosurgical instrument. Thus, when it is desired to use the instrument to treat tissue with a tip operated at lower temperatures, for example when coagulating tissue, the power control algorithm may intermittently increase the power delivered to the tip so as to substantially prevent to tip from sticking to the tissue being treated.
According to yet another aspect of the invention, a thermal surgical instrument of the present invention may have one or more controls for selectively managing power delivery to a surgical tip according to a fixed power index or a repeatedly executed power profile.
These and other aspects of the present invention are realized in a thermally adjustable surgical instrument as shown and described in the following figures and related description.
Various embodiments of the present invention are shown and described in reference to the numbered drawings wherein:
It will be appreciated that the drawings are illustrative and not limiting of the scope of the invention which is defined by the appended claims. The embodiments shown accomplish various aspects and objects of the invention. It is appreciated that it is not possible to clearly show each element and aspect of the invention in a single figure, and as such, multiple figures are presented to separately illustrate the various details of the invention in greater clarity. Similarly, not every embodiment need accomplish all advantages of the present invention.
The invention and accompanying drawings will now be discussed in reference to the numerals provided therein so as to enable one skilled in the art to practice the present invention. The drawings and descriptions are exemplary of various aspects of the invention and are not intended to narrow the scope of the appended claims.
As used herein, the term “ferromagnetic,” “ferromagnet,” and “ferromagnetism” refers to substances such as iron, nickel, cobalt, etc. and various alloys that exhibit high magnetic permeability, a characteristic saturation point, and magnetic hysteresis.
Turning now to
It will be appreciated that the thermal surgical instrument 10 may use heat to incise tissue without the use of a sharp edge such as with a conventional scalpel. While the embodiments of the present invention could be made with a relatively sharp edge so as to form a cutting blade, such is not necessary as the heated coating discussed herein will separate tissue without the need for a cutting blade or sharp edge. However, for convenience, the term cutting is used when discussing separating tissue.
According to one aspect of the invention, the thermal surgical instrument system 10 may include one or more control mechanisms, such as one or more foot pedals 20 to control output energy produced by a power supply 30. The energy from the power supply 30 may be sent via radio frequency (RF) or oscillating electrical energy along a cable 40 to a body 50, such as a handpiece, having a thermal element 60, such as a ferromagnetic material 65 associated with a conductor 66. As shown in
The RF energy may travel along the conductor's 66 surface in a manner known as the “skin effect”. Skin effect is the tendency of an alternating electric current to become distributed within a conductor 66 such that the current density is highest near the surface of the conductor 66, and decreases with greater depths in the conductor 66. The electric current flows mainly at the “skin” of the conductor 66, between the outer surface and a level called the skin depth. The skin effect causes the effective resistance of the conductor 66 to increase at higher frequencies where the skin depth is smaller, thus reducing the effective cross-section of the conductor 66. The skin effect is due to eddy currents induced by the changing magnetic field resulting from the alternating current. The skin depth is a function of the electrical resistivity, the magnetic permeability of the material conducting the current, and the frequency of the applied alternating RF current. For example, at 60 Hz in copper, the skin depth is about 8.5 mm. At high frequencies the skin depth becomes much smaller.
Over 98% of the current will flow within a layer 4 times the skin depth from the surface and virtually all of the current is within the first 5 skin depths. This behavior is distinct from that of direct current which usually will be distributed evenly over the cross-section of the conductor 66. The skin depth of a conductor 66 may be expressed by the following equations:
δ=√{square root over (2ρ)}/ωμ=1/√πfμσ
Where:
δ=skin depth (or penetration depth)
ρ=resistivity of the conductor
ω=angular frequency of current
μ=absolute magnetic permeability of conductor
σ=conductivity of the conductor
f=frequency
The current density in the conductor 66 may be expressed by the following equation:
I=Jse−d/δ
Where
Js=the current at the surface of the conductor
δ=skin depth (or penetration depth
d=depth from the surface of the conductor
The flow of current through the conductor 66 may also create a magnetic field which may act on the ferromagnetic material 65 having an open loop B-H curve (also known as an open hysteresis loop), resulting in hysteresis losses and resultant thermal energy. For example, electrodeposited films, such as a nickel-iron coating like PERMALLOY™, may form an array of randomly aligned microcrystals, resulting in randomly aligned domains, which together may have an open loop hysteresis curve when a high frequency current is passed through the conductor 66.
As the domains realign with each oscillation of the current, the ferromagnetic material 65 will heat due to hysteresis losses in the ferromagnetic material 65. Heating of the ferromagnetic portion 65 due to hysteresis loss ceases above its Curie point because the material loses its magnetic properties as explained in more detail below. Additionally, because the relative permeability of the ferromagnetic portion 65 changes in response to temperature, the associated skin depth also changes, and therefore the amount of current conduction through the skin layer undergoes a transition near the Curie point. Thus, heating of the ferromagnetic portion 65 due to resistive heating may also be reduced as it approaches the Curie point.
As mentioned above, the ferromagnetic material 65 may have a Curie temperature. A Curie temperature is the temperature at which the material becomes paramagnetic, such that the magnetic properties of the coating are lost. When the material becomes paramagnetic, the ferromagnetic heating may be significantly reduced or even cease. Theoretically, this should cause the temperature of the ferromagnetic material 65 to stabilize around the Curie temperature if sufficient power is provided to reach the Curie temperature. However, it has been found that the temperature of the ferromagnetic material 65 may exceed its calculated Curie temperature under certain operational conditions. It has been observed that if sufficient power has been applied, the tip temperature can continue to rise due to resistive heating in the overall conductor and the tip can potentially exceed the Curie temperature. When this occurs, an increase in current is observed while operating at a constant power level. It is believed that this may be due, at least in part to an increase in the skin depth and a resulting drop in impedance above the Curie temperature. The increase may also be due to the resistance of the ferromagnetic coating dropping which in turn raises the current level for a fixed power level. The increased current may then cause more resistive heating in the non-ferromagnetic portion of the conductor. Thus, it may be preferable to use an underlying conductor having high electrical conductivity.
Therefore, passage of alternating electrical energy through the conductor's 66 surface may cause Joule heating (also known as ohmic heating or resistive heating) along the thermal element 60. As the alternating electrical energy passes into the ferromagnetic region the current may jump to the ferromagnetic material 65 disposed on the conductor. Thus, a significant portion of the thermal energy created in the ferromagnetic material 65 may be due to Joule heating. Also, the RF energy may be converted into thermal energy in the ferromagnetic region due to hysteresis losses in the ferromagnetic material 65.
A thermal element 60 may be constructed so that the ferromagnetic material 65 has a thickness corresponding to approximately 5 skin depths such that substantially all of the alternating electrical energy flowing through the conductor 66 jumps to the ferromagnetic coating 65. As skin depth is a function of the frequency of the alternating electrical energy passing through the conductor 66 and/or ferromagnetic material 65, the thickness of the ferromagnetic material 65 needed to achieve approximately 5 skin depths may vary depending on the frequency of the alternating electrical energy being delivered to the conductor 66. For example, by delivering a high frequency alternating electrical energy to the conductor 66 a thin layer of ferromagnetic material 65 is sufficient to provide for substantially all of the alternating electrical current to jump to the ferromagnetic material 65. According to one aspect of the invention, a thermal element 60 may be constructed of a 0.5 mm diameter conductor wire having a 10 μm layer of PERMALLOY™ disposed thereon, such that delivering an alternating electrical current having a frequency of 40.68 MHz to the conductor wire will cause substantially all of the alternating electrical current to jump to the PERMALLOY™ layer.
The RF conductor from the signal source up to and including the tip may form a resonant circuit at a specific frequency (also known as a tuned circuit). Thus, when alternating electrical current is delivered to the conductor 66 the standing wave ratio (“SWR”) of the circuit will be approximately 1 at room temperature. As the thermal element 60 heats up, the impedance of the thermal element 60 changes, thereby changing the overall circuit impedance. Monitoring the impedance of the circuit, either directly as shown in
One advantage achieved by the ferromagnetic heating is that the ferromagnetic material 65 can be heated to a cutting temperature rapidly. In some instances the ferromagnetic material 65 can be heated in a small fraction of a second (e.g. as short as 100 ms). Additionally, because of the relatively low mass of the ferromagnetic material 65, the small thermal mass of the conductor 66, and the localization of the heating to a small region due to construction of the body 50, the material may also cool extremely rapidly (e.g. in some instances in approximately one half of a second). This provides a surgeon with a precise thermal instrument while reducing accidental tissue damage caused by touching tissue when the thermal instrument is not activated.
It will be appreciated that the time period required to heat and cool the thermal element 60 will depend, in part, on the relative dimensions of the conductor 66 and the ferromagnetic coating 65 and the heat capacity of the structure of the surgical instrument. For example, the above exemplary time periods for heating and cooling of the thermal element 60 may be achieved with a tungsten conductor having a diameter of about 0.375 mm and a ferromagnetic coating of a Nickel Iron alloy (such as NIRON™ available from Enthone, Inc. of West Haven, Conn.) about the tungsten conductor about 0.010 mm thick and two centimeters long.
One advantage of the present invention is that a sharp edge may not be needed. When power is not being supplied to the surgical instrument, the instrument will not inadvertently cut tissue of the patient or of the surgeon if it is dropped or mishandled. If power is not being supplied to the conductor 66 and ferromagnetic material 65, the “cutting” portion of the instrument may be touched without risk of injury. This is in contrast to a sharpened cutting blade which may injure the patient or the surgeon if mishandled.
It should be understood that the surgical instrument 10 may include indicia of the power being applied and may even include a mechanism for controlling the power. Thus, for example, a series of displays 52 could be used to indicate power level or the body 50, such as a handpiece could include a switch, rotary dial, sets of buttons, touchpad or slide 54 that communicate with the power source 30 to regulate power and thereby affect the temperature at the ferromagnetic material 65 to having varying effects on tissue. The controls also may be included in the power supply 30, for example control dials 32 or the like, or even be included in a separate control instrument, such as a remote control. Other additions may also be placed on the handpiece 50, power supply 30, remote control, etc. in various locations.
The adjustability of the temperature of the ferromagnetic material 65 may provide the surgeon with precise control over the tissue effects that may be achieved through use of the surgical instrument 10. Tissue effects such as cutting, hemostasis, tissue welding, tissue vaporization and tissue carbonization occur at different temperatures. By including a user control to adjust the power output, the surgeon (or other physician, etc.) can adjust the power delivered to the ferromagnetic material 65 and consequently control the tissue effects to achieve a desired result.
Additionally, power delivery to the thermal body 50 may be controlled by varying the amplitude, frequency or duty cycle of the alternating current waveform, or alteration of the circuit to effect the standing wave driving the ferromagnetic coated conductor, which may be achieved by input received by a foot pedal 20 the controls on the power supply 30 or handpiece 50, etc.
Furthermore, as describe in more detail below, the surgical instrument 10 may be comprised of a handpiece 50 which can removably receive a thermal element 60. For example, various removably attachable surgical tips 58 may have a different thermal elements 60 (e.g. differing in size, shape, etc.) associated therewith. Thus, thermal elements 60 of various configurations may be used with the handpiece 50.
Turning now to
The one or more sensing circuits may be used to monitor various behavior characteristics of the thermal element 60 when in use, such as how much current is delivered to the thermal element 60, the impedance of the circuit, etc., or a combination of behavior characteristics of the thermal element 60. For example, the peak-detection device 100 may determine the current which is delivered to the tip 60 by measuring the voltage drop across a resistor 104 (e.g., circuit-board trace in the tip or a corresponding resistor in the handpiece or power supply), which may be directly in-line with the current flowing to the tip. The voltage drop is directly proportional to the current in the branch of the circuit by Ohm's Law (V=IR). The higher the voltage, the more current there is flowing through the branch. The voltage across the resistor 104 may be passed back through a peak-detection circuit to track the peaks of the signal, such as the peaks of a 40.68 MHz signal, within its operational range.
Moreover, the sensing circuitry may detect the impedance of the thermal element 60, thus providing feedback as to the temperature of the thermal element (See e.g.
Sensing various properties of the thermal element 60 may be necessary because of the nature of the high permeability (high-mu) of the ferromagnetic material 65 on the tip 60. It is currently believed that, during normal operation, the majority of the current flow through the ferromagnetic material 65 may be attributed to the skin effect. When too much current flows through the ferromagnetic material 65, the Curie temperature may be reached and the permeability of the ferromagnetic material 65 may drop off dramatically. Consequently, the current begins to flow more significantly through the conductor 66 reducing the resistance in the thermal element 60. As the resistance is decreased at a constant power level, the current will increase and the voltage across the sensing resistor 104 will also increase. Thus, it is currently believed that as the Curie temperature is reached or exceeded that the skin depth increases, contributing to a decrease in the resistance of the heated tip 60. It has been observed that an increase in current occurs as the Curie temperature is exceeded at a constant power level.
Turning now to
Other properties of the material used for the conductor 66 may be important. These properties may include the resistivity of the material, the thermal and electrical conductivity of the material, the material's heat capacity, the material's coefficient of thermal expansion, the annealing temperature of the material, and the ability to plate a second material to the material comprising the conductor 66.
In choosing a material to use as the conductor 66, it may be important that such material have the greatest amount of resistance to bending while having low resistivity to minimize heating of the conductor 66 due to resistance heating. Additionally, it may also be important that the material have a low heat capacity so that heat is not stored in the conductor 66 thus allowing the surgical tip to cool rapidly when not being used. This may help limit or prevent collateral damage to structures adjacent the surgical site.
Additionally, it is desirable that the conductor 66 be comprised of material having a sufficiently high annealing temperature. At times, the surgical tip may be operated at temperatures, for example, between about 400 degrees Celsius and 500 degrees Celsius. Thus, to avoid alterations in the properties of the conductor 66, the annealing temperature of the material used as the conductor should be sufficiently higher than the expected operating ranges of the surgical tip.
Furthermore, it may be desirable that the support 70 be comprised of a material having a coefficient of thermal expansion value that is close to the coefficient of thermal expansion of the ferromagnetic material 65, such as a ferromagnetic coating 78, to facilitate plating of the ferromagnetic coating 78 to the conductor 66 in some configurations.
It has been observed, however, that some materials having adequate resistance to bending (Young's modulus) during normal operation of the surgical tip may have a coefficient of thermal expansion that is too low for adequate plating integrity. Thus, one or more intervening layers 74 having an intermediate coefficient of thermal expansion may be plated on the conductor 66 and then the ferromagnetic layer or coating 78 plated on the one or more intervening layers 74 to provide for a transition to accommodate the difference between the coefficients of thermal expansion of the support 70 and the ferromagnetic material 65.
Another important factor regarding the material used for the conductor 66 may be its ability to conduct electricity. There are multiple materials which provide adequate support, but which are not sufficiently conductive. Thus a conductor 66 may be comprised of multiple layers of different material so as to minimize any undesirable property or properties of the conductor 66.
For example, the conductor 66 may have a one or more conductive intervening layers 74 disposed thereon, such as copper, silver, etc. or other conductive material. The intervening layer 74 allows the energy to pass without significant resistive heating, thus allowing the tip to cool down more rapidly. (It will be appreciated that the cross-sectional view of
The conductor 66 of
The ferromagnetic coating 78 may be exposed or may be covered with an exterior coating 80 made from a biocompatible material to ensure that there is no reaction between the ferromagnetic coating 78 and the patient tissues. The exterior coating 80 may also act as a lubricant between the surgical tip and tissue which is being treated by reducing the attachment of biologic tissues to the surgical tip. For example, the exterior coating 80 may be titanium nitride (or one of its variants), TEFLON or a host of other biocompatible materials.
The exterior layer 80 may also act as an oxygen barrier to prevent oxidation of the layer of ferromagnetic material 65, any intervening layer 74, and/or the support 70. For example, it has been observed that oxidation of the support 70 may cause the support 70 to become brittle making the support 70 more susceptible to damage. It will be appreciated that the exterior layer 80 may be disposed on the conductor 66 so as to substantially cover the ferromagnetic material and the entire conductor 66. Alternatively, the exterior layer may be disposed on the conductor 66 so as to cover the ferromagnetic coating 78 and only a portion of the conductor 66.
According to one aspect of the invention, a thermal element 60 may comprise a conductor having an intermediate layer having a cross-sectional thickness corresponding to about 2-5 skin depths and a ferromagnetic layer having a cross-section thickness also corresponding to about 2-5 skin depths. For example, a thermal element 60, such as the one shown in
It will be appreciated that thermal elements of the present invention may include a ferromagnetic layer having a cross-section thickness corresponding to greater than 5 skin depths. Controlling the temperature of the thermal element may reduce the range of temperatures that the thermal element is subject to as compared to the more extreme thermal cycling that the thermal element would experience if temperature was not limited. Because controlling the temperature of the thermal element reduces such extreme thermal cycling, a thermal element used according to principles of the present invention may have better structural integrity. Thus, in addition to thin layers of ferromagnetic material 65 plated on the conductor, ferromagnetic sleeves and solid ferromagnetic heating elements may be used.
The thermal element 60 (or tips) may be coupled to a base, shroud, etc. 58 (
It will be appreciated that various thermal elements 60 may be constructed such that different thermal elements have a different size, shape, etc. for use in a particular surgical procedure, and/or are configure to be used in association with a particular surgical device.
For example,
Also, thermal elements 60 of the present invention may be disposed on, or embedded in, a surface of a surgical instrument, rather than in a standalone configuration. For example, thermal elements 60 may be constructed for use with a sealing and cutting instrument 15 as shown in
Furthermore, each class of thermal elements 60 (e.g. 2 mm dissecting loop (
Tip configuration parameters or constants may include the following:
One or more of the foregoing parameters may be used by a power control system to deliver a desired power to the instrument in a consistent manner, prevent the thermal element 60 of the surgical instrument from exceeding the Curie point, and/or prevent overheating of the thermal surgical instrument or heating of the instrument at locations other than the desired location. The power control system may include software having a power control algorithm module and/or hardware which may be used independently or in conjunction to control power delivery to the instrument.
Consistent power delivery may be achieved with the use of a control loop feedback mechanism. The feedback mechanism may include one or more proportional-integral-derivative controllers (PID controller). For example,
While
For example,
Furthermore, preventing the tip from exceeding the Curie point may also be accomplished using the cascaded PID control of
Additionally, heating of the tip 60 (
As mentioned above, a state machine may be designed to minimize the amount of power delivered to a thermal element 60 when it is in air and still provide the desired power to heat the ferromagnetic material 65 when in tissue. The particular challenge that this may present is the proper response of the instrument when physically moving between, for example, air and tissue. To overcome this challenge, the software may, for example, use the SWR as a trigger for determining the state of the tip (e.g. a high SWR indicates air, and a low SWR indicates a load).
According to one aspect of the invention, the surgical environment of the thermal element 60 may be determined by, for example, periodically sending a pulse of increase power to the thermal element and monitoring the affects, if any, on the behavior characteristics of the thermal element 60 (e.g. change in impedance, SWR, etc.). For example, if the thermal element 60 is well coupled to tissue then the temperature of the thermal element 60 will rise modestly (i.e. relatively low rate of change in current, impedance, SWR, etc.). If, however, the thermal element 60 is poorly coupled (i.e. the thermal element is in air), then the rate of change in the current, impedance, SWR, etc., will be high indicating that the thermal element is rapidly heating. If a high rate of change in the current, impedance, SWR, etc. is detected, then the power control system may drastically limit the amount of power delivered to the thermal element 60 to prevent overheating of the thermal element 60 and/or overheating at other locations which may be in thermal communication with the thermal element 60, such as the body or handpiece 50.
Limiting the amount of power delivered to the thermal element 60 to prevent overheating may also be important because the thermal element may be damaged when subjected to large temperature differential and/or extreme thermal cycling. For example, subjecting a thermal element to a large temperature differential can cause materials making up the thermal element to fracture, especially when heating the thermal element in air then contacting it with much cooler tissues or liquids. Thus, by limiting power delivery to the thermal element 60 and thereby limiting the temperature that the thermal element reaches, it may be less fragile when transitioning between, for example, air and liquid.
Referring now to
When RF is first turned on, such as by a button press, foot pedal activation, etc, this may be referred to as the RF On state 210. Entry into RF On state 210 may set the control power target to the desired output level. Also, during the RF On state 210, the peak values for SWR and tip current may be monitored. The goal of this state may be to determine an initial condition for the tip 60 power. Some surgeons may activate the tip 60 in the air, and then touch tissue, while others may touch tissue, and then activate the tip 60. Thus, the RF On state 210 may allow the tip 60 to be fully powered in the event it is in contact with tissue when turned on or prevent the tip 60 from overheating if the tip is in the air by, for example, either current limiting the output power and/or only allowing the tip 60 to remain in the RF On state 210 for a short period of time.
From the RF On state 210, the tip 60 may enter either the Air state 220 or the Load state 250 depending on certain measured parameters. For example, the tip 60 may enter the Air state 220 when the peak SWR or tip current is too high for the target power setting. Alternatively if the peak SWR is in range for the target power after, for example, 125 counts (e.g. 500 ms) then the tip may enter the Load state 250. It will be appreciated that any particular duration a tip remains in a particular state described herein is being provided for illustrative purposes only. Thus, for example, according to one aspect of the invention the tip 60 may enter the Load state 250 from the Air state 210 if the peak SWR is in range from 250 counts, instead of 125 counts.
More specifically, the Air state 220 may be entered when indications point to the tip 60 not being in a load, e.g. not being in contact with a sufficient heat sink such as tissue. On entry into Air state 220, power may be set to low (as specified by a given tip's 60 parameters—e.g. 10 W for a 2 mm dissecting loop and a 4 mm resecting loop) to minimize tip heating. Exit from the Air state 220 may be via one of two primary methods, detection of a low SWR or a rapid decrease in reflected power (which may also be related to SWR, but be a more dynamic indicator of change). To ensure that the Air state 220 is not exited prematurely (e.g. a sharp decline in the reflected power may also occur when decreasing the output power), the software may first wait until the slope of the reflected power has stabilized. Once stable, the SWR and slope of the reflected power may be monitored for exit conditions (described in more detail below).
To prevent the tip 60 from becoming stalled in the Air state 220 (or at a low power level) the state may automatically be periodically change from the Air state 220 to the Pre-Load state 230. For example, if the tip 60 is in the Air state 220 for more than one second, the state may be changed to the Pre-Load state 230 (describe in more detail below) to more actively test the tip's 60 status. Changing the tip 60 to the Pre-Load state 230 should not significantly increase net power (e.g. with the power set to 60 W and the tip 60 operating in air only, this active test method delivers an aggregate power of approximately 18.75 W).
Exit conditions from the Air state 220 to the Pre-Load state 230 may include a slope of the reflected power which is stable for, for example, 5 counts (e.g. 20 ms); SWR which is less than the limit at low power; reflected power decreasing quickly (e.g. slope<−200); or about a one second time lapse.
The Pre-Load state 230 may be described as the stabilization state, and may be entered as a pre-condition to the Load state 250. On entry into the Pre-Load state 230, power may be set to the target value and the SWR monitored. The total duration in the Pre-Load state 230 may be between about 31 and 62 counts. For the first 31 counts (approximately 125 ms), the system may be allowed to stabilize with no regard to SWR limiting, allowing brief transitions outside of the allowable range while the power control stabilizes. For the remaining 31 counts, the SWR may be monitored for validity. Thus, even if the tip 60 is in air, it will have operated at the target power for only about 125 ms (as well as being current limited).
Additionally, rather than switch to the Air state 220 when the SWR is exceeded, the algorithm may make the assumption that the Pre-Load state 230 was entered with the intent of going to the Load state 250, and moves to the Transition state 240 instead.
From the Pre-Load state 230, the tip 60 may enter either the Load state 250 or the Transition state 240, depending on certain measured parameters. For example, the tip 60 may enter the Load state 250 when the SWR is within range for about 62 counts (approximately 250 ms). Alternatively, if the SWR exceeds the limit for the target power setting after about 31 counts, then the tip may enter the Transition state 240.
Referring more particularly to the Transition state 240, the Transition state 240 may be entered either from the Pre-Load state 230 or the Load state 250, and be used as an interim step to determine the current state of the tip 60, e.g. still in load, or back in air. On entry to the Transition state 240, the power may be set to the lowest level (e.g. 5 W) for the greater of 5 counts, or until the SWR drops below the target power SWR limit.
Therefore, the Transition state 240 may significantly decrease the power delivered to the tip 60 then, similar to the change to the Pre-Load state 230 from air, actively check the actively check the current state of the tip 60. If the SWR continues to exceed the limit for five successive attempts, it may be assumed that the tip 60 is in air, and the state may be changed accordingly, otherwise, the previous state (either Pre-Load 230 or Load 250) may be reset. Alternatively, the attempt counter may reset when more than one second has been spent in the Load state 250, as the power control algorithm may assume power stability at this point.
From the Transition state 240, the tip 60 may enter the Pre-Load 230 or the Air state 220, depending on certain measured parameters. For example, the tip 60 may enter Pre-Load state 230 when the tip 60 is in the Transition state 240 for at least 5 counts (20 ms) and SWR drops below the limit for the target power. The tip 60 may alternatively enter the Air state 220 if there are, for example, 5 consecutive attempts in the Transition state 240 without at least one second in the Load state 250.
The tip 60 may enter the Load state 250 from the Pre-Load state 230 when power is deemed stable and operating within the SWR limit, or re-entered from the Transition state when a determination is being made as to the current air/load status of the tip 60. The tip 60 may remain in the Load state 250, for example, until such time as the SWR increases past the limit for the target power level. More particularly, exit from the Load state 250 may occur when SWR exceeds the limit for the target power setting for 5 consecutive counts (approximately 20 ms).
The control algorithm is used to operate the power supply so as to maintain the tip 60 within a desired operation range in the particular state that the tip is currently in (e.g. in free air, in tissue, etc.). Thus, for a particular tip, the configuration parameters will determine operational characteristics such as temperature or power limits as well as operational or control parameters such as tuning impedance or reactance and the SWR constant. As discussed, the tip itself may have data stored therein on a storage device such as an EEPROM and provide that information to the power supply when the tip is connected to the surgical handpiece. Alternatively, the tip 60 may include an identification element such as a resistor whose value is different for different tip configurations and identifies the particular tip configuration. Thus, the power supply can sense the value of the resistor and determine from a table which tip configuration corresponds to that unique resistance value. The power supply itself can have the operational parameters of the different types of tips stored therein and use the identification element to determine which operational parameters should be used with the tip which has been connected to the surgical handpiece. It will be appreciated that the configuration parameters may be stored in alternate locations such as a computer or device which is separate from the power supply.
Turning now to
According to one aspect of the invention, a thermal surgical instrument may be selectively controlled such that a user may operate the instrument in a mode where power delivery to a surgical tip is managed according to a fixed power index or a mode where power delivery to a surgical tip is managed according to a repeatedly executed power profile. For example power delivery management may be selectively controlled by activating the foot pedals 20 shown in
Turning now to
Turning now to
Turning now to
There is thus disclosed an improved electrosurgical and/or thermal surgical instrument and system to control the delivery of power from an energy source to the surgical instrument. It will be appreciated that numerous changes may be made to the present invention without departing from the scope of the claims.
This application is a continuation of application Ser. No. 14/081,936, filed Nov. 15, 2013 (now U.S. Pat. No. 9,549,774), which is a division of application Ser. No. 13/706,481, filed Dec. 6, 2012 (now U.S. Pat. No. 8,617,151), which claims the benefit of Provisional Application No. 61/567,603, filed Dec. 6, 2011 and Provisional Application No. 61/669,671, filed Jul. 10, 2012, and is a continuation-in-part of application Ser. No. 12/647,371, filed Dec. 24, 2009 (now U.S. Pat. No. 8,523,852), which claims the benefit of Provisional Application No. 61/170,203, filed Apr. 17, 2009, and Provisional Application No. 61/170,220, filed Apr. 17, 2009, and Provisional Application No. 61/170,207, filed Apr. 17, 2009, the disclosures of which are incorporated by reference in their entireties herein.
Number | Name | Date | Kind |
---|---|---|---|
300155 | Starr | Jun 1884 | A |
770368 | Heath | Sep 1904 | A |
1104053 | Lea | Jul 1914 | A |
1280052 | Lidberg | Sep 1918 | A |
1335987 | Reid et al. | Apr 1920 | A |
1366231 | Winter et al. | Jan 1921 | A |
1401104 | Kruesheld et al. | Dec 1921 | A |
1794296 | Hyams | Feb 1931 | A |
2027854 | Breth et al. | Jan 1936 | A |
2050904 | Trice | Aug 1936 | A |
2120598 | Beuoy | Jun 1938 | A |
2250602 | Pierce | Jul 1941 | A |
2278633 | Bagnall | Apr 1942 | A |
2375154 | Volterra | May 1945 | A |
2412977 | Eskin | Dec 1946 | A |
2501499 | Crowley | Mar 1950 | A |
2670425 | Stone | Feb 1954 | A |
2735797 | Schjeldahl | Feb 1956 | A |
2782290 | Lannan et al. | Feb 1957 | A |
2831242 | Kieffer et al. | Apr 1958 | A |
2846560 | Jacoby et al. | Aug 1958 | A |
2863036 | Mitchell et al. | Dec 1958 | A |
2947345 | Schjeldahl | Aug 1960 | A |
2960592 | Pierce | Nov 1960 | A |
3084242 | Vogler et al. | Apr 1963 | A |
3213259 | Bennett et al. | Oct 1965 | A |
3350544 | Lennox | Oct 1967 | A |
3352011 | Alexander et al. | Nov 1967 | A |
3400252 | Hayakawa et al. | Sep 1968 | A |
3404202 | Carlson et al. | Oct 1968 | A |
3413442 | Buiting et al. | Nov 1968 | A |
3414705 | Marcoux | Dec 1968 | A |
3434476 | Shaw et al. | Mar 1969 | A |
3501619 | Buiting et al. | Mar 1970 | A |
3515837 | Ando | Jun 1970 | A |
3520043 | Darling | Jul 1970 | A |
3556953 | Schulz | Jan 1971 | A |
3768482 | Shaw | Oct 1973 | A |
3825004 | Durden, III | Jul 1974 | A |
3826263 | Cage et al. | Jul 1974 | A |
3834392 | Lampman et al. | Sep 1974 | A |
3978312 | Barton et al. | Aug 1976 | A |
RE29088 | Shaw | Dec 1976 | E |
4089336 | Cage et al. | May 1978 | A |
4091813 | Shaw et al. | May 1978 | A |
RE30190 | Shaw | Jan 1980 | E |
4185632 | Shaw | Jan 1980 | A |
4196734 | Harris | Apr 1980 | A |
4198957 | Cage et al. | Apr 1980 | A |
4206759 | Shaw | Jun 1980 | A |
4207896 | Shaw | Jun 1980 | A |
4209017 | Shaw | Jun 1980 | A |
4256945 | Carter et al. | Mar 1981 | A |
4359052 | Staub | Nov 1982 | A |
4364390 | Shaw | Dec 1982 | A |
4371861 | Abdelrahman et al. | Feb 1983 | A |
4374517 | Hagiwara | Feb 1983 | A |
RE31723 | Shaw | Nov 1984 | E |
4481057 | Beard | Nov 1984 | A |
4485810 | Beard | Dec 1984 | A |
4492231 | Auth | Jan 1985 | A |
4493320 | Treat | Jan 1985 | A |
4523084 | Tamura et al. | Jun 1985 | A |
4549073 | Tamura et al. | Oct 1985 | A |
4600018 | James et al. | Jul 1986 | A |
4622966 | Beard | Nov 1986 | A |
4658819 | Harris et al. | Apr 1987 | A |
4658820 | Klicek | Apr 1987 | A |
4701587 | Carter et al. | Oct 1987 | A |
4752673 | Krumme | Jun 1988 | A |
4807620 | Strul et al. | Feb 1989 | A |
4839501 | Cowell | Jun 1989 | A |
4848337 | Shaw et al. | Jul 1989 | A |
4860745 | Farin et al. | Aug 1989 | A |
4877944 | Cowell et al. | Oct 1989 | A |
4914267 | Derbyshire | Apr 1990 | A |
4915100 | Green | Apr 1990 | A |
4927413 | Hess | May 1990 | A |
4938761 | Ensslin | Jul 1990 | A |
5003991 | Takayama et al. | Apr 1991 | A |
5026387 | Thomas | Jun 1991 | A |
5047025 | Taylor et al. | Sep 1991 | A |
5053595 | Derbyshire | Oct 1991 | A |
5057106 | Kasevich et al. | Oct 1991 | A |
5071419 | Rydell et al. | Dec 1991 | A |
5087256 | Taylor et al. | Feb 1992 | A |
5087804 | McGaffigan | Feb 1992 | A |
5098429 | Sterzer | Mar 1992 | A |
5107095 | Derbyshire | Apr 1992 | A |
5182427 | McGaffigan | Jan 1993 | A |
5189271 | Derbyshire | Feb 1993 | A |
5197649 | Bessler et al. | Mar 1993 | A |
5203782 | Gudov et al. | Apr 1993 | A |
5209725 | Roth | May 1993 | A |
5211646 | Alperovich et al. | May 1993 | A |
5217460 | Knoepfler | Jun 1993 | A |
5300068 | Rosar et al. | Apr 1994 | A |
5300750 | Carter, Jr. et al. | Apr 1994 | A |
5308311 | Eggers et al. | May 1994 | A |
5318564 | Eggers | Jun 1994 | A |
5364392 | Warner et al. | Nov 1994 | A |
5370645 | Klicek et al. | Dec 1994 | A |
5370675 | Edwards et al. | Dec 1994 | A |
5376094 | Kline | Dec 1994 | A |
5382247 | Cimino et al. | Jan 1995 | A |
5400267 | Denen | Mar 1995 | A |
5411508 | Bessler et al. | May 1995 | A |
5423808 | Edwards et al. | Jun 1995 | A |
5425731 | Daniel | Jun 1995 | A |
5445635 | Denen | Aug 1995 | A |
5472443 | Cordis et al. | Dec 1995 | A |
5475203 | McGaffigan | Dec 1995 | A |
5480397 | Eggers et al. | Jan 1996 | A |
5480398 | Eggers | Jan 1996 | A |
5496312 | Klicek | Mar 1996 | A |
5496314 | Eggers | Mar 1996 | A |
5507743 | Edwards et al. | Apr 1996 | A |
5540679 | Fram et al. | Jul 1996 | A |
5540681 | Strul et al. | Jul 1996 | A |
5542916 | Hirsch et al. | Aug 1996 | A |
5571153 | Wallstén | Nov 1996 | A |
5573533 | Strul | Nov 1996 | A |
5593406 | Eggers et al. | Jan 1997 | A |
5595565 | Treat et al. | Jan 1997 | A |
5611798 | Eggers | Mar 1997 | A |
5628771 | Mizukawa et al. | May 1997 | A |
5674219 | Monson et al. | Oct 1997 | A |
5707369 | Vaitekunas et al. | Jan 1998 | A |
5707402 | Heim | Jan 1998 | A |
5807392 | Eggers | Sep 1998 | A |
5807393 | Williamson, IV et al. | Sep 1998 | A |
5827269 | Saadat | Oct 1998 | A |
5836874 | Swanson et al. | Nov 1998 | A |
5836943 | Miller, III | Nov 1998 | A |
5843019 | Eggers et al. | Dec 1998 | A |
5855061 | Malis et al. | Jan 1999 | A |
5911719 | Eggers | Jun 1999 | A |
5951546 | Lorentzen | Sep 1999 | A |
5964759 | Yamanashi et al. | Oct 1999 | A |
6004316 | Laufer | Dec 1999 | A |
6006755 | Edwards | Dec 1999 | A |
6015415 | Avellanet | Jan 2000 | A |
6035238 | Ingle et al. | Mar 2000 | A |
6038017 | Pinsukanjana et al. | Mar 2000 | A |
6039733 | Buysse et al. | Mar 2000 | A |
6066138 | Sheffer et al. | May 2000 | A |
6161048 | Sluijter et al. | Dec 2000 | A |
6190382 | Ormsby et al. | Feb 2001 | B1 |
6210403 | Klicek | Apr 2001 | B1 |
6228084 | Kirwan, Jr. | May 2001 | B1 |
6241723 | Heim et al. | Jun 2001 | B1 |
6287305 | Heim et al. | Sep 2001 | B1 |
6290697 | Tu et al. | Sep 2001 | B1 |
6350262 | Ashley | Feb 2002 | B1 |
6358273 | Strul et al. | Mar 2002 | B1 |
6454781 | Witt et al. | Sep 2002 | B1 |
6533781 | Heim et al. | Mar 2003 | B2 |
6602252 | Mollenauer | Aug 2003 | B2 |
6604003 | Fredricks et al. | Aug 2003 | B2 |
6626901 | Treat et al. | Sep 2003 | B1 |
6632182 | Treat | Oct 2003 | B1 |
6692489 | Heim et al. | Feb 2004 | B1 |
6723094 | Desinger | Apr 2004 | B1 |
6726683 | Shaw | Apr 2004 | B1 |
6821273 | Mollenauer | Nov 2004 | B2 |
6860880 | Treat et al. | Mar 2005 | B2 |
6908463 | Treat et al. | Jun 2005 | B2 |
6911026 | Hall et al. | Jun 2005 | B1 |
6912911 | Oh et al. | Jul 2005 | B2 |
6980862 | Fredricks et al. | Dec 2005 | B2 |
6980865 | Wang et al. | Dec 2005 | B1 |
7011656 | McGaffigan et al. | Mar 2006 | B2 |
7025065 | McGaffigan et al. | Apr 2006 | B2 |
7083613 | Treat | Aug 2006 | B2 |
7112201 | Truckai et al. | Sep 2006 | B2 |
7122030 | Flores et al. | Oct 2006 | B2 |
7164968 | Treat et al. | Jan 2007 | B2 |
7175621 | Heim et al. | Feb 2007 | B2 |
7211079 | Treat | May 2007 | B2 |
7211080 | Treat et al. | May 2007 | B2 |
7235073 | Levine et al. | Jun 2007 | B2 |
7300452 | Gleich | Nov 2007 | B2 |
7317275 | Treat | Jan 2008 | B2 |
7326202 | McGaffigan | Feb 2008 | B2 |
7329255 | McGaffigan | Feb 2008 | B2 |
7377919 | Heim et al. | May 2008 | B2 |
7396356 | Mollenauer | Jul 2008 | B2 |
7435249 | Buysse et al. | Oct 2008 | B2 |
7473250 | Makin et al. | Jan 2009 | B2 |
7473253 | Dycus et al. | Jan 2009 | B2 |
7494492 | Da Silva et al. | Feb 2009 | B2 |
7528663 | Naletov et al. | May 2009 | B2 |
7533719 | Hinson et al. | May 2009 | B2 |
7540324 | de Rouffignac et al. | Jun 2009 | B2 |
7549470 | Vinegar et al. | Jun 2009 | B2 |
7553309 | Buysse et al. | Jun 2009 | B2 |
7556095 | Vinegar | Jul 2009 | B2 |
7556096 | Vinegar et al. | Jul 2009 | B2 |
7559367 | Vinegar et al. | Jul 2009 | B2 |
7559368 | Vinegar et al. | Jul 2009 | B2 |
7562706 | Li et al. | Jul 2009 | B2 |
7562707 | Miller | Jul 2009 | B2 |
7578815 | Howell | Aug 2009 | B2 |
7581589 | Roes et al. | Sep 2009 | B2 |
7584789 | Mo et al. | Sep 2009 | B2 |
7588565 | Marchitto et al. | Sep 2009 | B2 |
7588566 | Treat et al. | Sep 2009 | B2 |
7591310 | Minderhoud et al. | Sep 2009 | B2 |
7597147 | Vitek et al. | Oct 2009 | B2 |
7604052 | Roes et al. | Oct 2009 | B2 |
7610962 | Fowler | Nov 2009 | B2 |
7613523 | Eggers et al. | Nov 2009 | B2 |
7631689 | Vinegar et al. | Dec 2009 | B2 |
7631690 | Vinegar et al. | Dec 2009 | B2 |
7632295 | Flores et al. | Dec 2009 | B2 |
7635023 | Goldberg et al. | Dec 2009 | B2 |
7635024 | Karanikas et al. | Dec 2009 | B2 |
7635025 | Vinegar et al. | Dec 2009 | B2 |
7678105 | McGreevy et al. | Mar 2010 | B2 |
7686804 | Johnson et al. | Mar 2010 | B2 |
7699842 | Buysse et al. | Apr 2010 | B2 |
7702397 | Fredricks et al. | Apr 2010 | B2 |
7776035 | Rick et al. | Aug 2010 | B2 |
7828798 | Buysse et al. | Nov 2010 | B2 |
7871406 | Nields et al. | Jan 2011 | B2 |
7879033 | Sartor et al. | Feb 2011 | B2 |
7887535 | Lands et al. | Feb 2011 | B2 |
7922713 | Geisel | Apr 2011 | B2 |
7931649 | Couture et al. | Apr 2011 | B2 |
7938779 | Sakurai et al. | May 2011 | B2 |
7951149 | Carlton | May 2011 | B2 |
7951150 | Johnson et al. | May 2011 | B2 |
7959633 | Sartor et al. | Jun 2011 | B2 |
7963965 | Buysse et al. | Jun 2011 | B2 |
7972334 | McGreevy et al. | Jul 2011 | B2 |
7972335 | McGreevy et al. | Jul 2011 | B2 |
7981113 | Truckai et al. | Jul 2011 | B2 |
8062290 | Buysse et al. | Nov 2011 | B2 |
8100896 | Podhajsky | Jan 2012 | B2 |
8100908 | McGaffigan et al. | Jan 2012 | B2 |
8104956 | Blaha | Jan 2012 | B2 |
8105323 | Buysse et al. | Jan 2012 | B2 |
8211105 | Buysse et al. | Jul 2012 | B2 |
8241284 | Dycus et al. | Aug 2012 | B2 |
8287528 | Wham et al. | Oct 2012 | B2 |
8377052 | Manwaring et al. | Feb 2013 | B2 |
8377057 | Rick et al. | Feb 2013 | B2 |
8398626 | Buysse et al. | Mar 2013 | B2 |
8480666 | Buysse et al. | Jul 2013 | B2 |
8523852 | Manwaring et al. | Sep 2013 | B2 |
8568402 | Buysse et al. | Oct 2013 | B2 |
8591506 | Wham et al. | Nov 2013 | B2 |
8617151 | Denis et al. | Dec 2013 | B2 |
8667674 | Buysse | Mar 2014 | B2 |
8672938 | Buysse et al. | Mar 2014 | B2 |
9549774 | Denis et al. | Jan 2017 | B2 |
20010014804 | Goble et al. | Aug 2001 | A1 |
20020019627 | Maguire et al. | Feb 2002 | A1 |
20020019644 | Hastings et al. | Feb 2002 | A1 |
20020026188 | Balbierz et al. | Feb 2002 | A1 |
20020029037 | Kim | Mar 2002 | A1 |
20020029062 | Satake | Mar 2002 | A1 |
20020068931 | Wong et al. | Jun 2002 | A1 |
20020087156 | Maguire et al. | Jul 2002 | A1 |
20020120261 | Morris | Aug 2002 | A1 |
20020133148 | Daniel et al. | Sep 2002 | A1 |
20020165529 | Danek | Nov 2002 | A1 |
20020173787 | Buysse et al. | Nov 2002 | A1 |
20030004507 | Francischelli et al. | Jan 2003 | A1 |
20030055417 | Truckai et al. | Mar 2003 | A1 |
20030055424 | Ciarrocca | Mar 2003 | A1 |
20030060818 | Kannenberg et al. | Mar 2003 | A1 |
20030073987 | Sakurai et al. | Apr 2003 | A1 |
20030073989 | Hoey et al. | Apr 2003 | A1 |
20030109871 | Johnson et al. | Jun 2003 | A1 |
20030139741 | Goble et al. | Jul 2003 | A1 |
20030144660 | Mollenauer | Jul 2003 | A1 |
20030171747 | Kanehira et al. | Sep 2003 | A1 |
20030176873 | Chernenko et al. | Sep 2003 | A1 |
20030195499 | Prakash et al. | Oct 2003 | A1 |
20030199755 | Halperin et al. | Oct 2003 | A1 |
20040006335 | Garrison | Jan 2004 | A1 |
20040030330 | Brassell et al. | Feb 2004 | A1 |
20040034349 | Kirwan, Jr. et al. | Feb 2004 | A1 |
20040049185 | Latterell et al. | Mar 2004 | A1 |
20040059345 | Nakao et al. | Mar 2004 | A1 |
20040073256 | Marchitto et al. | Apr 2004 | A1 |
20040167506 | Chen | Aug 2004 | A1 |
20040176756 | McGaffigan | Sep 2004 | A1 |
20040187875 | He et al. | Sep 2004 | A1 |
20040243120 | Orszulak et al. | Dec 2004 | A1 |
20050021016 | Malecki et al. | Jan 2005 | A1 |
20050033338 | Ferree | Feb 2005 | A1 |
20050072827 | Mollenauer | Apr 2005 | A1 |
20050107776 | McGaffigan et al. | May 2005 | A1 |
20050113824 | Sartor et al. | May 2005 | A1 |
20050197661 | Carrison et al. | Sep 2005 | A1 |
20050245919 | van der Welde | Nov 2005 | A1 |
20050273111 | Ferree et al. | Dec 2005 | A1 |
20050283067 | Sobe | Dec 2005 | A1 |
20050283149 | Thorne et al. | Dec 2005 | A1 |
20050288659 | Kimura et al. | Dec 2005 | A1 |
20060095096 | DeBenedictis | May 2006 | A1 |
20060127706 | Goebel et al. | Jun 2006 | A1 |
20060142824 | Zikorus et al. | Jun 2006 | A1 |
20060161149 | Privitera et al. | Jul 2006 | A1 |
20060167450 | Johnson et al. | Jul 2006 | A1 |
20060212030 | McGaffigan | Sep 2006 | A1 |
20060212031 | McGaffigan et al. | Sep 2006 | A1 |
20060217700 | Garito et al. | Sep 2006 | A1 |
20060217706 | Lau et al. | Sep 2006 | A1 |
20060241587 | Heim et al. | Oct 2006 | A1 |
20060241588 | Heim et al. | Oct 2006 | A1 |
20060241589 | Heim et al. | Oct 2006 | A1 |
20060271037 | Maroney et al. | Nov 2006 | A1 |
20070005054 | Heim et al. | Jan 2007 | A1 |
20070005055 | Heim et al. | Jan 2007 | A1 |
20070005056 | Heim et al. | Jan 2007 | A1 |
20070005057 | Heim et al. | Jan 2007 | A1 |
20070005058 | Heim et al. | Jan 2007 | A1 |
20070005059 | Heim et al. | Jan 2007 | A1 |
20070005060 | Heim et al. | Jan 2007 | A1 |
20070016181 | van der Weide et al. | Jan 2007 | A1 |
20070016272 | Thompson et al. | Jan 2007 | A1 |
20070060920 | Weitzner | Mar 2007 | A1 |
20070073282 | McGaffigan et al. | Mar 2007 | A1 |
20070100336 | McFarlin et al. | May 2007 | A1 |
20070100405 | Thompson et al. | May 2007 | A1 |
20070106294 | Nesbitt | May 2007 | A1 |
20070127897 | John et al. | Jun 2007 | A1 |
20070131428 | Willem Cornelis den Boestert et al. | Jun 2007 | A1 |
20070173811 | Couture et al. | Jul 2007 | A1 |
20070208339 | Arts et al. | Sep 2007 | A1 |
20070239151 | Atalar et al. | Oct 2007 | A1 |
20070270924 | McCann et al. | Nov 2007 | A1 |
20080017380 | Vinegar et al. | Jan 2008 | A1 |
20080033419 | Nields et al. | Feb 2008 | A1 |
20080035346 | Nair et al. | Feb 2008 | A1 |
20080035347 | Brady et al. | Feb 2008 | A1 |
20080035705 | Menotti | Feb 2008 | A1 |
20080038144 | Maziasz et al. | Feb 2008 | A1 |
20080077129 | Van Wyk et al. | Mar 2008 | A1 |
20080119841 | Geisel | May 2008 | A1 |
20080128134 | Mudunuri et al. | Jun 2008 | A1 |
20080135253 | Vinegar et al. | Jun 2008 | A1 |
20080135254 | Vinegar et al. | Jun 2008 | A1 |
20080142216 | Vinegar et al. | Jun 2008 | A1 |
20080142217 | Pieterson et al. | Jun 2008 | A1 |
20080161800 | Wang et al. | Jul 2008 | A1 |
20080173444 | Stone et al. | Jul 2008 | A1 |
20080174115 | Lambirth | Jul 2008 | A1 |
20080185147 | Vinegar et al. | Aug 2008 | A1 |
20080187989 | McGreevy et al. | Aug 2008 | A1 |
20080217003 | Kuhlman et al. | Sep 2008 | A1 |
20080217016 | Stegemeier et al. | Sep 2008 | A1 |
20080228135 | Snoderly | Sep 2008 | A1 |
20080236831 | Hsu | Oct 2008 | A1 |
20080255642 | Zarins et al. | Oct 2008 | A1 |
20080277113 | Stegemeier et al. | Nov 2008 | A1 |
20080281310 | Dunning et al. | Nov 2008 | A1 |
20080281315 | Gines | Nov 2008 | A1 |
20080319438 | DeCarlo | Dec 2008 | A1 |
20090014180 | Stegemeier et al. | Jan 2009 | A1 |
20090014181 | Vinegar et al. | Jan 2009 | A1 |
20090093811 | Koblish et al. | Apr 2009 | A1 |
20090112200 | Eggers | Apr 2009 | A1 |
20090118729 | Auth et al. | May 2009 | A1 |
20090118730 | Mollenauer | May 2009 | A1 |
20090198224 | McGaffigan | Aug 2009 | A1 |
20090248002 | Takashino et al. | Oct 2009 | A1 |
20090292347 | Asmus et al. | Nov 2009 | A1 |
20090306644 | Mayse et al. | Dec 2009 | A1 |
20090312753 | Shadduck | Dec 2009 | A1 |
20100004650 | Ormsby et al. | Jan 2010 | A1 |
20100082022 | Haley et al. | Apr 2010 | A1 |
20100152725 | Pearson et al. | Jun 2010 | A1 |
20100198216 | Palanker | Aug 2010 | A1 |
20100228244 | Hancock et al. | Sep 2010 | A1 |
20100268205 | Manwaring et al. | Oct 2010 | A1 |
20100268206 | Manwaring et al. | Oct 2010 | A1 |
20100268207 | Manwaring et al. | Oct 2010 | A1 |
20100268208 | Manwaring et al. | Oct 2010 | A1 |
20100268209 | Manwaring et al. | Oct 2010 | A1 |
20100268210 | Manwaring et al. | Oct 2010 | A1 |
20100268211 | Manwaring et al. | Oct 2010 | A1 |
20100268212 | Manwaring et al. | Oct 2010 | A1 |
20100268213 | Manwaring et al. | Oct 2010 | A1 |
20100268214 | Manwaring et al. | Oct 2010 | A1 |
20100268215 | Manwaring et al. | Oct 2010 | A1 |
20100268216 | Manwaring et al. | Oct 2010 | A1 |
20100268218 | Ormsby et al. | Oct 2010 | A1 |
20110004204 | Dodde et al. | Jan 2011 | A1 |
20110054456 | Thompson et al. | Mar 2011 | A1 |
20110092971 | Sartor et al. | Apr 2011 | A1 |
20110152857 | Ingle | Jun 2011 | A1 |
20120059367 | Buysse et al. | Mar 2012 | A1 |
20120071712 | Manwaring et al. | Mar 2012 | A1 |
20120130256 | Buysse et al. | May 2012 | A1 |
20120150170 | Buysse et al. | Jun 2012 | A1 |
20120226270 | Manwaring et al. | Sep 2012 | A1 |
20120259323 | Manwaring et al. | Oct 2012 | A1 |
20120296326 | Manwaring et al. | Nov 2012 | A1 |
20120303026 | Dycus et al. | Nov 2012 | A1 |
20120330295 | Manwaring et al. | Dec 2012 | A1 |
20130006240 | McNally et al. | Jan 2013 | A1 |
20130012934 | Manwaring et al. | Jan 2013 | A1 |
20130023866 | Stringham et al. | Jan 2013 | A1 |
20130041367 | Wham et al. | Feb 2013 | A1 |
20140058381 | Wham et al. | Feb 2014 | A1 |
20140058384 | Buysse et al. | Feb 2014 | A1 |
20140058385 | Wham et al. | Feb 2014 | A1 |
20140100559 | Wham et al. | Apr 2014 | A1 |
20140180266 | Buysse et al. | Jun 2014 | A1 |
Number | Date | Country |
---|---|---|
0 033 958 | May 1983 | EP |
0 130 671 | Jan 1985 | EP |
2 070 486 | Jun 2009 | EP |
2 036 512 | Feb 2016 | EP |
1 546 624 | May 1979 | GB |
2 022 974 | Dec 1979 | GB |
3-51179 | Aug 1991 | JP |
2558584 | Sep 1996 | JP |
10-277050 | Oct 1998 | JP |
2 072 118 | Jan 1997 | RU |
8200746 | Mar 1982 | WO |
9217121 | Oct 1992 | WO |
9321839 | Nov 1993 | WO |
9408524 | Apr 1994 | WO |
9626677 | Sep 1996 | WO |
9937227 | Jul 1999 | WO |
0106943 | Feb 2001 | WO |
2004014217 | Feb 2004 | WO |
2004076146 | Sep 2004 | WO |
2006017517 | Feb 2006 | WO |
2006029649 | Mar 2006 | WO |
2007080578 | Jul 2007 | WO |
2008060668 | May 2008 | WO |
Entry |
---|
Visioli, Antonio. Practical PID Control. London: Springer-Verlag, 2006. pp. 1-18. Print. (Year: 2006). |
Center for Research in Scientific Computation, A Domain Wall Theory for Ferroelectric Hysteresis, Jan. 1999. |
Denis et al., “Thermal Surgical Tool,” U.S. Appl. No. 61/567,603, filed Dec. 6, 2011, 33 pages. |
Denis et al., “System and Method of Controlling Power Delivery to an Electrosurgical Instrument,” U.S. Appl. No. 61/669,671, filed Jul. 10, 2012, 59 pages. |
European Search Report, dated Nov. 28, 2014, for European Application No. 12865504.0-1652, 9 pages. |
High Temp Metals, Inc., “High Temp Metals,” NI2001201 Technical Data, URL=http://www.hightempmetals.com/techdatafnitempNi200data.php, Jul. 13, 2012. |
International Preliminary Report on Patentability, dated Apr. 1, 2014, for International Application No. PCT/US2012/055229, 9 pages. |
International Preliminary Report on Patentability, dated Jun. 10, 2014, for International Application No. PCT/US2012/068027, 7 pages. |
International Preliminary Report on Patentability, dated May 9, 2013, for International Application No. PCT/US2011/050417, 8 pages. |
International Preliminary Report on Patentability, dated Nov. 19, 2013, for International Application No. PCT/US2012/038005, 7 pages. |
International Preliminary Report on Patentability, dated Oct. 8, 2013, for International Application No. PCT/US2012/032565, 5 pages. |
International Preliminary Report on Patentability, dated Oct. 8, 2013, for International Application No. PCT/US2012/032656, 7 pages. |
International Preliminary Report on Patentability, dated Oct. 8, 2013, for International Application No. PCT/US2012/032659, 9 pages. |
International Preliminary Report on Patentability, dated Oct. 8, 2013, for International Application No. PCT/US2012/032661, 8 pages. |
International Preliminary Report on Patentability, dated Oct. 13, 2011, for International Application No. PCT/US2010/031114, 7 pages. |
International Search Report and Written Opinion, dated Apr. 12, 2012, for International Application No. PCT/US2011/050417, 12 pages. |
International Search Report and Written Opinion, dated Aug. 19, 2013, for International Application No. PCT/US2012/032661, 10 pages. |
International Search Report and Written Opinion, dated Feb. 1, 2013, for International Application No. PCT/US2012/055229, 11 pages. |
International Search Report and Written Opinion, dated Feb. 15, 2013, for International Application No. PCT/US2012/068027, 8 pages. |
International Search Report and Written Opinion, dated Jan. 21, 2011, for International Application No. PCT/US2010/031114, 12 pages. |
International Search Report and Written Opinion, dated Nov. 23, 2012, for International Application No. PCT/US2012/032659, 12 pages. |
International Search Report and Written Opinion, dated Nov. 23, 2012, for International Application No. PCT/US2012/038005, 9 pages. |
International Search Report and Written Opinion, dated Oct. 23, 2012, for International Application No. PCT/US2012/032656, 13 pages. |
International Search Report and Written Opinion, dated Sep. 27, 2012, for International Application No. PCT/US2012/032565, 7 pages. |
Japanese Office Action, for Japanese Application No. 2012-506188. (English Translation). |
Manwaring et al., “Adjustable Ferromagnetic Coated Conductor Thermal Surgical Tool,” U.S. Appl. No. 61/170,203, filed Apr. 17, 2009, 36 pages. |
Manwaring et al., “Thermally Adjustable Surgical or Therapeutic Tool and Method of Use,” U.S. Appl. No. 61/170,220, filed Apr. 17, 2009, 41 pages. |
Manwaring et al., “Surgical Multi-Mode Tool With Ferromagnetic Coated Conductor for Adjustable Thermal Energy Delivery,” U.S. Appl. No. 61/170,207, filed Apr. 17, 2009, 43 pages. |
Metcal Soldering Iron Catalog, 2006. |
URSI EMTS 2004, Electromagnetic Probes for Living Tissue Cauterization, pp. 489-491. |
Visioli, Practice PID Control, Springer-Verlag, London, United Kingdom, 2006, pp. 1-18. |
European Supplementary Search Report, dated Jan. 30, 2015, for European Application No. 12 76 7458, 3 pages. |
Extended European Search Report, dated Nov. 10, 2016, for European Application No. 10765134.1-1659, 8 pages. |
Number | Date | Country | |
---|---|---|---|
20170196617 A1 | Jul 2017 | US |
Number | Date | Country | |
---|---|---|---|
61170203 | Apr 2009 | US | |
61170220 | Apr 2009 | US | |
61170207 | Apr 2009 | US | |
61567603 | Dec 2011 | US | |
61669671 | Jul 2012 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 13706481 | Dec 2012 | US |
Child | 14081936 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 14081936 | Nov 2013 | US |
Child | 15383535 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 12647371 | Dec 2009 | US |
Child | 13706481 | US |