System and method for return electrode monitoring

Abstract
A system for determining probability of tissue damage is disclosed. The system includes a plurality of return electrodes adhered to a patient and adapted to couple to an electrosurgical generator configured to generate an electrosurgical current. The system also includes a current monitor and a switching component connected in series with each of the plurality of the return electrodes. The current monitor being configured to measure the electrosurgical current passing therethrough. The system further includes a processor coupled to each of the current monitors and the switching components. The processor is configured to determine the balance of a current load among the plurality of the return electrodes and configured to control each of the switching components to adjust the current passing through each of the return electrodes to balance the current load.
Description
BACKGROUND

1. Technical Field


The present disclosure relates generally to a system and method for using a plurality of return electrodes during electrosurgery and, more particularly, to a system and method for balancing the various thermal effects of the plurality of return electrodes by minimizing the probability and ensuring the plurality of return electrodes are properly attached to a patient.


2. Background of Related Art


During electrosurgery, a source or active electrode delivers energy, such as radio frequency (RF) energy, from an electrosurgical generator to a patient and a return electrode or a plurality thereof carry current back to the electrosurgical generator. In monopolar electrosurgery, the source electrode is typically a hand-held instrument placed by the user at the surgical site and the high current density flow at this electrode creates the desired surgical effect of ablating, cutting or coagulating tissue. The patient return electrodes are placed at a remote site from the source electrode and are typically in the form of pads adhesively adhered to the patient.


The return electrodes usually have a large patient contact surface area to minimize heating at that site since the smaller the surface area, the greater the current density and the greater the intensity of the heat. That is, the area of the return electrode that is adhered to the patient is important because it is the current density of the electrical signal that heats the tissue. A larger surface contact area is desirable to reduce heat intensity. Return electrodes are sized based on assumptions of the maximum current seen in surgery and the duty cycle (i.e., the percentage of time the generator is on) during the procedure.


The first types of return electrodes were in the form of large metal plates covered with conductive jelly. Later, adhesive electrodes were developed with a single metal foil covered with conductive jelly or conductive adhesive. However, one problem with these adhesive electrodes was that if a portion peeled from the patient, the contact area of the electrode with the patient decreased, thereby increasing the current density at the adhered portion and, in turn, increasing the heat applied to the tissue. This risked burning the patient in the area under the adhered portion of the return electrode if the tissue was heated beyond the point where circulation of blood could cool the skin.


To address this problem, split return electrodes and hardware circuits, generically called return electrode contact quality monitors (RECQMs), were developed. These split electrodes consist of two separate conductive foils. The hardware circuit uses an AC signal between the two electrode halves to measure the impedance therebetween. This impedance measurement is indicative of how well the return electrode is adhered to the patient since the impedance between the two halves is directly related to the area of patient contact with the return electrode. That is, if the electrode begins to peel from the patient, the impedance increases since the contact area of the electrode decreases. Current RECQMs are designed to sense this change in impedance so that when the percentage increase in impedance exceeds a predetermined value or the measured impedance exceeds a threshold level, the electrosurgical generator is shut down to reduce the chances of burning the patient.


Currently, during electrosurgical procedures involving especially high current, it is common to use multiple return electrodes to ensure adequate surface area to minimize heating at the return electrodes and thereby minimize the risk of damaging tissue. Typical ablation procedures can deliver up to 2.0 Arms for up to 20 minutes either continuously or with periodic current pulses. This extended duration for a high total current value may create a potential for alternate site burns due to return electrode pad heating. Further, the use of multiple return electrodes may also pose an additional potential problem—the increase in temperature under each of the return electrodes is not uniform, e.g., there is a thermal imbalance among the multiple return electrodes. This is caused by the differing impedance values between the active electrode and each of the multiple return electrodes, which varies due to placement and proximity of the active electrode to the return electrode.


Typically, since current is the primary factor in return electrode heating, measurement of the total current output from the electrosurgical generator may be used to infer possible tissue damage. Although the total current output of the electrosurgery generator is approximately equal to the sum of the current through each of the return electrodes, the individual return electrode currents may not be equal due to the differing impedances as described above. This condition may generate an imbalance of current among each of the return electrodes resulting in an imbalance of thermal rise on the return electrodes.


SUMMARY

Systems and methods for ensuring the plurality of return electrodes are properly attached to a patient, balancing thermal effects, and reducing probability of tissue damage during electrosurgical procedures involving a multitude of return electrodes are disclosed. More specifically, the system includes an electrosurgical generator and a plurality of return electrodes as well as a current monitor, a switch, and an impedance sensor electrically connected to each of the return electrodes and the electrosurgical generator. The generator monitors the current passing through each of the return electrodes through the current monitor. The generator determines current load for each return electrode and if the current load exceed a predetermined threshold the return electrode is removed from the circuit via a switch component.


According to one embodiment of the present disclosure, a system for determining probability of tissue damage is disclosed. The system includes a plurality of return electrodes adhered to a patient and adapted to couple an electrosurgical generator configured to generate an electrosurgical current. The system also includes a current monitor and a switching component connected in series with each of the plurality of the return electrodes. The current monitor is configured to measure the electrosurgical current passing therethrough. The system further includes a processor coupled to each of the current monitors and the switching components. The processor is configured to determine the balance of a current load among the plurality of the return electrodes and is further configured to control each of the switching components to adjust the current passing through each of the return electrodes to balance the current load.


According to another embodiment of the present disclosure, a method for determining for determining probability of tissue damage. The method includes the step of providing a plurality of return electrodes adhered to a patient and adapted to couple to an electrosurgical generator configured to generate an electrosurgical current, wherein a current monitor and a switching component are connected in series with each of the plurality of the return electrodes. The method also includes the steps of measuring the electrosurgical current passing through each of a plurality of the return electrodes, determining the balance of a current load among the plurality of the return electrodes and controlling each of the switching components to adjust the current passing through each of the return electrodes to balance the current load.





BRIEF DESCRIPTION OF THE DRAWINGS

The above and other aspects, features and advantages of the present disclosure will become more apparent in light of the following detailed description in conjunction with the accompanying drawings in which:



FIG. 1 is a schematic illustration of a monopolar electrosurgical system;



FIG. 2 is a schematic block diagram of an electrosurgical system for determining adherence of multiple return electrodes to a patient;



FIG. 3 is a flow diagram showing a method for determining adherence of multiple return electrodes to a patient;



FIG. 4 is a schematic block diagram of on electrosurgical system for determining the probability of tissue damage and controlling return current in multiple return electrodes;



FIG. 5 is a flow diagram showing a method for monitoring and controlling return electrode current in multiple return electrodes; and



FIG. 6 is a flow diagram showing a method for determining the probability of tissue damage.





DETAILED DESCRIPTION

Embodiments of the present disclosure are described hereinbelow with reference to the accompanying drawings. In the following description, well-known functions or constructions are not described in detail to avoid obscuring the present disclosure in unnecessary detail.


Systems and methods for determining whether return electrodes are properly attached to a patient, for balancing thermal effects of multiple return electrodes, and for preventing tissue damage when using multiple return electrodes are disclosed.



FIG. 1 is a schematic illustration of a monopolar electrosurgical system 1. The system 1 includes a surgical instrument 11, e.g., an active electrode, for treating tissue at a surgical site. Electrosurgical energy is supplied to the instrument 11 by a generator 10 via a cable 18 allowing the instrument 11 to ablate, cut or coagulate the tissue. The electrosurgical system also includes a plurality of return electrodes 14, 15 and 16 placed under the patient's back, the patient's leg, and the patient's arm, respectively, to return the energy from the patient to the generator 10 via a cable 12. The return electrodes 14, 15 and 16 are preferably in the form of a split pad which is adhesively attached to the patient's skin.


The surface area of the return electrodes 14, 15 and 16 that adheres to the patient is substantially similar since the surface area affects the current density of the signal which, in turn, heats the tissue. The smaller the contact area of the return electrode with the patient's tissue, the greater the current density and concentrated heating of tissue underneath the return electrodes 14, 15 and 16. Conversely, the greater the contact area of the return electrodes 14, 15 and 16, the smaller the current density and the less heating of tissue.



FIG. 2 illustrates a schematic block diagram of the electrosurgical system 1 for determining whether the return electrodes 14, 15 and 16 are properly adhered to the patient's body. The system 1 includes generator 10 for generating electrosurgical energy, an active electrode 11, e.g., an instrument, for delivering the electrosurgical energy to the tissue and a plurality of return electrodes 14, 15 and 16 for receiving the electrosurgical energy and returning the electrosurgical energy to the generator 10. Although the present disclosure describes the electrosurgical system 1 in reference to three return electrodes 14, 15 and 16, those skilled in the relevant art will understand that the principles of the present disclosure may be used with any number of return electrodes. In one embodiment, the system measures impedance between a pair of split pads of the return electrode via an impedance sensor to determine adherence of the return electrode to the patient


The generator 10 includes a microprocessor 26, an adjustable power supply 22, such as a high voltage supply coupled to an RF output stage 24 which generates RF energy for transmission to the instrument 11. The microprocessor 26 includes a plurality of input ports. A first input port in electrical communication with an output current sensor 28 measures the output current (IOUTPUT) being transmitted to the patient through the instrument 11.


The return electrodes 14, 15 and 16 are electrically connected to the generator 10 through the cable 12 and in series to current monitors 43, 53 and 63, which are connected to the microprocessor 26 and report the current passing through the respective return electrodes 14, 15 and 16. When using multiple return electrodes, monitoring the output current by the generator 10 may not be accurate in measuring the current passing through each of the return electrodes 14, 15 and 16. Therefore, the system according to the present disclosure places the current monitors 43, 53 and 63 in series with the corresponding return electrodes 14, 15 and 16 to allow accurate current measurements to measure current passing through each of the return electrodes, IMx, where x is the number of the return electrode.



FIG. 3 shows a method for determining adherence of multiple return electrode pads to a patient. This is accomplished by determining the ratios of the current load on each of the return electrodes 14, 15 and 16. Ideally, the return electrodes 14, 15 and 16 are of the same size and made from the same material. In absence of interference from other variables affecting impedance (e.g., temperature, moisture, etc.), the current load on each return electrode is the same since their impedance is the same. Alternatively, pads of different size or shape can be used with adjustment made to the allowable ratio. Current load is determined by calculating the ratio of the current distribution on each of the return electrodes 14, 15 and 16. For instance, if there are three return electrodes (e.g., the return electrodes 14, 15 and 16) then the ratio of the current load on each of the return electrodes should be 33% (i.e., total current, ITOTAL, divided by the number of return electrodes—current passing through each return electrode IMx is 33% of the total current output). If that ratio changes, it follows that the current load is distributed unevenly. This is caused by differing impedance of each of the return electrodes or tissue between the active electrode and each respective return electrode. Since all of the return electrodes are of the same size and material, the differing impedances are caused by the placements and/or adherence of the return electrodes. Hence, determining the ratios of the current load allows the system to determine whether the return electrodes 14, 15 and 16 are placed properly on the patient and are properly adhered thereto.


The presently disclosed process verifies the ratios at two stages: first, prior to commencement of an electrosurgical procedure, and second, during the procedure. In step 100, an initial check of adherence of the return electrodes 14, 15 and 16 is performed. The return electrodes 14, 15 and 16 are placed on the patient and the generator 10 is activated. The generator 10 outputs a low level interrogation current to calculate the baseline ratio for each of the return electrodes 14, 15 and 16. A low level interrogation current is used since the method initially verifies the placement and adherence of the return electrodes 14, 15 and 16 prior to commencement of electrosurgery. Current is measured by the current monitors 43, 53 and 63 and the measurements are transmitted to the microprocessor 26.


In step 102, the generator 10 determines the percentage of total current ITOTAL passing through each return electrode 14, 15 and 16 and compares the calculated values to the preferred ratio (e.g., 33%). In step 104, the generator 10 determines if the current load ratios of the return electrodes 14, 15 and 16 are equal (i.e., larger or smaller than 33%). The ratios may be considered equal if they fall within a predetermined threshold. For instance, if the ratio denoting that the return electrode is properly adhered to the patient is 33% and the actual ratio (e.g., 31%) is within a predetermined threshold (e.g., 2%), the two ratios are considered equal. This eliminates the probability of insignificant changes in the current load affecting the comparison process.


If the ratios are not equal, then the generator 10 (e.g., microprocessor 26) signals that the placement of the return electrodes 14, 15 and 16 needs to be checked and adjusted if required in step 106. After readjustment, in step 106, the generator 10 outputs low interrogation current again, to verify that the readjustment corrected the problem. The process loops until the ratios of the current load of each of in the return electrodes 14, 15 and 16 are equal or within a predetermined tolerance.


If the ratios of the current load are equal, then the process continues to step 108, wherein a second check of the ratios is performed as RF energy is supplied to the tissue and returned via the return electrodes 14, 15 and 16. The current monitors 43, 53 and 63 measure the current passing through the return electrodes 14, 15 and 16 throughout the procedure and transmit the measurements to the generator 10. In step 110, the generator 10 again determines the percentage of total current ITOTAL passing through each return electrode 14, 15 and 16 and compares the calculated values to the preferred ratio (e.g., 33%).


In step 112, the generator 10 determines if the current load ratios of the return electrodes 14, 15 and 16 has changed from the baseline measurements taken prior to commencement of the electrosurgical procedure by comparing the measured current ratio to the preferred current ratio. If the ratios have changed, the algorithm of the generator 10 assumes that the positioning of the return electrodes 14, 15 and 16 has also changed since the last check of the ratios in step 104. If there is a change, in step 114 the generator 10 adjusts the RF current output or shuts down. The action taken by the generator 10 depends on the degree in the change. A relatively small change in the ratio (e.g., below 5% for a three return electrode system) may require an adjustment in the RF energy output. This may be accomplished using switches (e.g., switches 44, 54 and 64 shown in FIG. 4 and described in more detail below). A large change in the ratio (e.g., 5% or more) may require shutting down the generator 10. If the generator 10 shuts down, then the process proceeds to step 106, which is an optional step, where adjustments to the placement and positioning of the return electrodes 14, 15 and 16 are made.


If the ratios are unchanged as determined in step 112, then the process loops to step 108, where the ratio is continually verified during the electrosurgical procedure. This process ensures that the return electrodes 14, 15 and 16, are properly attached to the patient prior to and during electrosurgery, thereby allowing the RF energy to be efficiently dissipated.



FIG. 4 illustrates a schematic block diagram of the electrosurgical system 1 for determining the probability of tissue damage and controlling the return current in multiple return electrodes 14, 15 and 16. In addition to the components shown in FIG. 2 and described above, the system of FIG. 4 includes switches 44, 54 and 64 and impedance sensors 40, 50 and 60. Further, the generator 10 also includes a current “on” time calculator 30 and a current “off” time calculator 32 electrically connected to the microprocessor 26. In embodiments, the calculators 30 and 32 may be implemented as software applications configured to be executed by the microprocessor 26.


The “on” time calculator 30 determines the amount of the time the current is being supplied to any one of the multiple return electrodes 14, 15 and 16 and transmits this data to the microprocessor 26. Conversely, the “off” time calculator 32 calculates the amount of time that any one of the return electrodes 14, 15 and 16 did not receive any current or the RF output current was turned “off” and sends a signal to the microprocessor 26 via one of its input ports.


The return electrodes 14, 15 and 16 are electrically connected in series to the current monitors 43, 53 and 63 and the switches 44, 54 and 64, respectively. The current monitors 43, 53 and 63 are connected to the microprocessor 26 and report the current passing through the respective return electrodes 14, 15 and 16. The switches 44, 54 and 64 are connected to the time calculators 30 and 32 so that the time calculators 30 and 32 can calculate if the return electrodes 14, 15 and 16 are included in the circuit. In addition, the switches 44, 54 and 64 are connected to a controller 25 which regulates whether the switches 44, 54 and 64 are open or closed.


The return electrodes 14, 15 and 16 include a pair of split pads 41, 42, 51, 52, 61 and 62, respectively, which are electrically connected to impedance sensors 40, 50 and 60. The function of the sensors 40, 50 and 60 will be discussed with reference only to the sensor 40 and its corresponding components. The sensor 40 measures the impedance between the split pads 41, 42 of the return electrode 14 to determine the degree of adherence of the return electrode 14. That is, if a portion of the return electrode 14 becomes detached from the patient, the impedance will increase. The sensor 40 transmits a signal indicative of the measured impedance to an input port of the microprocessor 26. Those skilled in the art will appreciate that the return electrodes 14, 15 and 16 may include multiple pairs of split pads.


In using multiple return electrodes, monitoring the output current output by the generator 10 is an inaccurate measure of the current passing through each of the return electrodes 14, 15 and 16. Therefore, the system according to the present disclosure places the current monitors 43, 53 and 63 and the switches 44, 54 and 64 in series with the corresponding return electrodes 14, 15 and 16. The switches 44, 54 and 64 can be active components, such as transistors of various types, (e.g., field effect transistor, insulated gate bipolar transistor, etc.) or electro-mechanical components (e.g., relays, solenoid switches, etc.).


The return electrodes 14, 15 and 16 are connected to the generator 10 through the cable 12. As will be discussed in more detail below, to obtain current measurements for each of the individual return electrodes 14, 15 and 16, the current monitors 43, 53 and 63 are included in the circuit between the return electrodes 14, 15 and 16 and the cable 12. The switches 44, 54 and 64 are also incorporated into the circuit in the same manner.


Monitoring and controlling of current passing through the return electrodes 14, 15 and 16 for balancing thermal effects will be discussed in conjunction with FIG. 5. In step. 116, the current passing through each of the return electrodes 14, 15 and 16 (IMx, wherein x is the number of the current monitor) is measured using the respective current monitors 43, 53 and 63 and is transmitted to the microprocessor 26.


In step 118, the current passing through all return electrodes 14, 15 and 16, ITOTAL, is calculated by the microprocessor 26 by summation of current monitor values IMx for each of the return electrodes. In step 120, a threshold current value, ITH, is calculated by the microprocessor 26 based on formula (1):

ITH=ITOTAL/n+TOLERANCE.  (1)


In the formula (1), ITOTALis the value calculated in step 118, n is the number of return electrodes and TOLERANCE is a predetermined value representative of the current for any particular return electrode exceeding the average return electrode current value. TOLERANCE can be from about 0 mA to about 100 mA. Further, tolerance can also be a percentage of the average current value from about 0% to about 25%.


Once the microprocessor 26 calculates ITH, the value is transmitted to the comparator 34. In step 122, all of the IMx values are compared to determine the highest return electrode current value Ihigh. The highest IMx(e.g., Ihigh) is then sent to the comparator 34.


In step 124, the comparator 34 determines if the current load is unbalanced, for instance, the current passing through the return electrode 14, is higher than the current passing through other return electrodes 15 and 16. The comparator 34 compares the highest IMx value with ITH to determine if the highest return electrode current value from step 122 exceeds the predetermined allowable current threshold. If the highest return electrode current does not exceed the allowable current threshold, all measured return electrode currents are within the allowable tolerance and the process is repeated from step 116. Conversely, if the highest return electrode current exceeds the allowable current threshold, then it is expected that the return electrode will overheat and possibly damage tissue. In that case, the comparator 34 notifies the controller 25 of the imbalance in the current of the return electrode with the highest measured current the process proceeds to step 126.


In step 126, the “off” time for the return electrode having highest IMx, is calculated by the microprocessor 26 using formula (2):

Toff=(Toffmax−Toffmin)/(ITOTAL−ITH)2*Ihigh2  (2)

In formula (2), Toffmax is the maximum off-time period, which is the longest possible duration of time that a particular return electrode can be disconnected. Toffmin is the minimum allowable period of time during which a particular return electrode can be disconnected. The Toffmax and Toffmin values are preset prior to the start of the procedure either automatically or manually. The “off” time periods may also be adjusted for each individual return electrode.


ITOTAL is the total current calculates in step 118, ITH is the threshold current calculated in step 120, and Ihigh2 is the square of the highest return electrode current value. Thus, the “off” time period is expressed as a function of the difference of the maximum and minimum “off” time periods multiplied by the ratio of the square of the measured current and the square of the difference between the total current and the threshold current.


In step 128, the controller 25 then opens the corresponding switches 44, 54 and 64 for the duration of Toff calculated in step 126. This distributes the current load more evenly through the other return electrodes. This balances the current load and the thermal load across all of the return electrodes 14, 15 and 16.


Switches 44, 54 and 64 may be opened using pulse width modulation, which allows for using predetermined pulses to manipulate specific switches. More specifically, a pulsed electrical control signal (e.g., from the microprocessor 26) is used to toggle the switch 44 depending on the duty cycle of the control signal, such as when the signal is “on,” the switch 44 is open and when the signal is “off” the switch 44 is closed.


Additional improvements to this algorithm include a comparison of total return current (ITOTAL) to the output current (IOUTPUT) measured by the output current sensor 28 to determine if there is any unintended leakage paths. The comparison is made by taking into consideration leakage current which can be from about 0 mA to about 150 mA (e.g., IEC 60601-2-2 maximum leakage standard). If ITOTAL is larger than IOUTPUT by a corresponding leakage current amount then a warning is given to the user or a control signal issued by the microprocessor 26 to adjust the RF energy supply accordingly.


In another embodiment, the redistribution of the current load may be accomplished by adjusting impedance of the circuit. Instead of the switch 44, a device that adjusts impedance of the circuit (e.g., resistor network, variable capacitor, transformer coupled load, transistor in linear region, etc.) including the current monitor 42 and the return electrode 14 may be utilized. If an imbalanced current is detected, then the impedance altering device which would be connected in series with the circuit, may raise the impedance and thereby reduce the current passing therethrough.


The current load determining algorithm may be also configured to measure impedance of the return electrodes 14, 15 and 16 and control the current flowing therethrough as a function of the measured impedance. If the return electrode is improperly adhered, the return electrode is going to have increased relative impedance as compared with other return electrodes. As a result, the current passing through the improperly adhered return electrode will decrease. The current monitors 43, 53 and 63 are used to detect the decrease in current and determine if the return electrode having a lower current also corresponds to having an increased impedance thereby confirming that the particular return electrode is improperly adhered and/or positioned.


In a further embodiment of the present disclosure, a system and method are provided for determining the absolute value of the thermal effect of the return electrodes 14, 15 and 16. The value of the thermal effect is determined by measuring the probability of tissue damage using the impedance values at the return electrodes 14, 15 and 16.


An algorithm in the microprocessor 26, described in more detail below, processes the signals from the output current sensor 28, the current monitors 43, 53 and 63 and the time calculators 30 and 32 in the calculation of the probability of tissue damage. The output port of the microprocessor 26 is in electrical communication with the comparator 34. The calculation of microprocessor 26 is compared to threshold values stored in the comparator 34, and if these values are exceeded, a signal is sent to generate an alarm using an alarm 27 as a warning to the user. If the threshold values are exceeded, the comparator 34 also sends a power adjustment signal to the controller 25 which signals the power supply 22 to either adjust, e.g., reduce the RF output current, shut off the power supply 22, or open any of the switches 44, 54 and 64 to terminate the supply of current, depending on the amount that the threshold is exceeded.


The following description is of the formulas and calculations involved in a method to calculate the probability of tissue damage occurring under the return electrodes 14, the same method can be used for the other return electrodes. As previously stated, if the total current passing through the return electrode 14 is increased or the current duty cycle, defined by the percentage of time the generator 10 is “on” during which the current is applied, is increased, heating under the electrode will also increase.


Tissue damage may result when a heating factor of the tissue underneath the return electrode 14 is higher than acceptable. The heating factor of the tissue is a measure of how much heat is dissipated in the tissue. Formula (3) provides the heating factor (it should be noted that in the formulas described in the disclosure, x represents the number of the associated electrode):

Heating Factor=IMx2 tonx  (3)

where IMx2 equals the square of the current in milliamps passing through a return electrode, e.g., Im14 is the current passing through the return electrode 14, and tonx is the time that current is passing through a return electrode, e.g., ton14 time on for the return electrode 14. The (Im14) is obtained from the corresponding current monitor 43 as discussed in more detail below.


Thus, the heating factor can be defined as the square of a given current passed through the return electrode attached to a patient multiplied by the time the current is applied. As is apparent from the formula, if either the current is increased or the on time is increased, the amount of heat dissipated in the tissue, and thus the chances of tissue damage, are increased.


The foregoing heat factor formula assumes that the area attached to the patient is unchanged. However, as a practical matter, that area can change as a portion of the return electrode can become detached from the patient. The return electrodes 14, 15 and 16 are split to enable the impedance to be measured between two split pads 41 & 42, 51 & 52 and 61 & 62, respectively. The impedance measurement provides an indication of how well the return electrodes 14, 15 and 16 are adhered to the patient since there is a direct relationship between the impedance and the area of patient contact. If the electrode is partially peeled from the patient, the impedance increases. This is because each portion of the electrode pad that touches the patient has a specific resistance. All of these resistances are connected in a parallel circuit, and the resultant equivalent resistance is smaller than any of its individual elements. Therefore, if any of these parallel resistances are removed because of peeling, the equivalent resistance increases slightly.


To accommodate for changed surface contact area of the return electrode, a constant (Khx) is added to the formula where Khx>=1. For example, Kh14=1 when the return electrode 14 is fully adhered, and Khx>1 if the return electrode 14 is not fully adhered. Formula (4) represents the modification:

Heating Factor=Khx IMx2 tonx  (4)


As is apparent from the formula, if the surface contact area of the return electrode 14 decreases, since (Kh14) will be greater than 1, the heating factor will increase. As the surface area decreases, as explained above, the current density increases and the amount of heating for a given output current also increases. It is to be appreciated the range of values of constant K can be determined from empirical data and stored as a database, chart, etc, which can be accessed using the measured impedance value.


Another factor affecting dissipation of heat in the tissue is the time period the RF energy is applied. The patient's body has the ability to remove heat from the area under the return electrode by the blood flow in the capillaries, small arteries and small veins. The more time between the applications of RF energy, the greater the heat removal because the body will have more time to naturally remove the heat. This ability to remove heat over a period of time can be represented by the following formula:

Cooling factor=Kcx toffx

where (Kc14) is a cooling constant for the return electrode 14 dependent on the patient and (toff14) is the time in seconds that current is not passing through the return electrode 14.


The above-described formulas allow the method and system of the present disclosure to measure the current delivered and the time period the current is delivered, as well as calculate and compare the heating and cooling factors to measure the probability of tissue damage as shown in FIG. 6. The method shown in FIG. 6 will be discussed with reference to the return electrode 14 and its corresponding components.


In step 200, the current passing through the return electrode 14 (Im14) is measured by the current monitor 43. In step 202, the current monitor 43 transmits the measurement to the microprocessor 26 which squares the measurement, represented by (Im142) in milliamps. In step 204, the time that the current being applied through the return electrode 14 (ton14) is measured in seconds. The (ton14) for the return electrode 14 is defined as the time during which the generator 10 is activated and the return electrode 14 is in the circuit, e.g., the switch 44 is closed. The (ton14) is calculated by the time calculator 30 based on the readings from the output current sensor 28 and the switch 44. In step 206, the microprocessor 26 multiplies the time on (ton14) by the squared current (Im142), the formula being represented by (Im142)*(ton14) to yield a first value.


In step 208, the impedance sensor 40 measures the impedance at the return electrode 14 which is indicative of the degree of adherence of the return electrode 14 to the patient. In step, 210 the adherence constant (Kh14) is calculated. In step 212, the microprocessor 26 multiplies the adherence constant (Kh14) by (Im142)*(ton14) to calculate the heating factor in step 214. Thus, the heating factor is calculated by the algorithm which multiplies (Kh14) by (Im142)*(ton14) wherein (Kh14) is the adherence constant and K=1 when the return electrode is fully adhered to the patient and K>1 if the electrode is not fully adhered.


The cooling factor is calculated by the measured time the current is not being applied. More specifically, in step 216, the time “off” for the return electrode 14 in seconds of the output current (toff14) is calculated. The (toff14) for the return electrode 14 is defined as time during which the generator 10 is deactivated or when the return electrode 14 is not in the circuit, e.g., the switch 44 is open. The (toff14) is calculated by the time calculator 32 based on the readings from the output current sensor 28 and the switch 44. In step 218, the microprocessor 26 multiplies the time off (toff14) by the cooling constant (Kc14) to calculate the cooling factor as (Kc14)*(toff14) in step 220. The cooling constant (Kc14) takes into account the patient body's natural cooling where the blood flow in the capillaries, small arteries and veins of the patient cools the tissue over time. For example, assuming tissue normally cools at one degree per minute, since there is some variation, the cooling constant could be conservatively selected as ½ degree per minute. Other constants could be selected depending on the tissue cooling time.


In step 222, the cooling factor is subtracted from the heating factor by the microprocessor 26 to determine a difference value representative of the probability of tissue damage. In step 224, the microprocessor 26 sends a signal to the comparator 34 representative of the difference value and the comparator 34 compares the difference value to a first threshold value. If the difference value is less than or equal to the first threshold value, a signal sent to the controller 25 and to the power supply 22 maintains the RF output current in step 226. This indicates that the differential between the cooling factor and heating factor is relatively low, hence there is a low probability of tissue damage and no adjustments to the current passing through the return electrode 14 need to be made.


If the difference value exceeds the first threshold value, in step 228, the difference value is then compared by the comparator 34 to a second threshold predetermined value in step 228. The second threshold value is preset to correspond to the situation where tissue damage is highly likely and the RF current through the tissue needs to be terminated. If the difference value exceeds the second threshold value, this indicates that the heating factor is too high relative to the cooling factor. In step 232, the comparator 34 will transmit a second signal to the controller 25. The controller 25 will process this signal and generate a shut off signal to the power supply 22 to shut off the RF current or to the switch 44 to turn off the current passing only through the return electrode 14. This shut off will allow the body time to dissipate the heat and cool the tissue.


Both threshold values are predetermined based on the probability of tissue damage so the overheating of tissue can be timely detected and the electrosurgical generator adjusted accordingly. If the difference value exceeds the first threshold value, but does not exceed the second threshold value, this means that although the heating factor is relatively high and there is some probability of tissue damage at the present power levels, it is not high enough that a shut down is mandated. Instead, the output level needs to be reduced. In this circumstance, in step 230, the comparator 34 will transmit a third signal to the controller 25 indicative of the high probability of tissue damage. The controller 25, in turn, will transmit a signal to the power supply 22 or to the switch 44 to reduce the output power to thereby reduce the output current by a preset amount.


It is also contemplated that if the difference value falls between the first threshold value and the second threshold value, rather than reducing the power, the duty cycle can be reduced. The duty cycle reduction could also alternately be the first response if the probability of tissue damage exceeds a first threshold followed by a reduction in power if the first threshold is further exceeded.


Thus, the system 1 remains operational, but at reduced current levels, to reduce the heating effect on the tissue. The probability of tissue damage is preferably continuously calculated in this manner throughout the surgical procedure to continuously monitor and control the heating of tissue.


As indicated in FIGS. 2 and 4, if the probability of tissue damage exceeds the first threshold value an alarm signal is sent to the alarm 27 to generate an alarm. The alarm can be in the form of a visual indicator, an audible indicator or both. Additionally, a visual and/or audible alarm can be sounded if the probability of tissue damage exceeds the second threshold value indicating shut off of the power supply.


In an alternate embodiment, the system and method according to the present disclosure include an additional step of determining the size of the return electrode to be utilized, e.g. adult, infant, neonate, and adjusting the heating and cooling constants accordingly. The user could inform the generator of the size being used, or alternatively, the size can be automatically sensed by the generator based on the differences in the return electrode connector.


The system and method according to the present disclosure monitors the current, calculates the probability of tissue damage for each of the multiple return electrodes, and adjusts the current passing through the multiple return electrodes accordingly. Since conventional return electrodes are connected in parallel, it is very difficult to calculate those values using the total current output. The system according to the present disclosure overcomes this difficulty by using individual current monitors and impedance sensors for each of the multiple return electrodes. These devices report the current and the impedance values of each of the return electrode circuits. Using current values as part of the heating factor calculation is believed to increase the accuracy of the probability of a tissue damage determination since current values are believed to actually cause the heating of the tissue. These values allow the electrosurgical system to prevent tissue damage by diverting current or completely turning current off and balancing the thermal effect over multiple return electrodes. This feature, in turn, allows for more energy to be applied during the procedure as a whole as well as increases the length of the surgical procedure.


While several embodiments of the disclosure have been shown in the drawings, it is not intended that the disclosure be limited thereto, as it is intended that the disclosure be as broad in scope as the art will allow and that the specification be read likewise. Therefore, the above description should not be construed as limiting, but merely as exemplifications of preferred embodiments. Those skilled in the art will envision other modifications within the scope and spirit of the claims appended hereto.

Claims
  • 1. A system for determining probability of tissue damage, the system comprising: a plurality of return electrodes adapted to be adhered to a patient and adapted to couple to an electrosurgical generator configured to generate an electrosurgical current;a plurality of current monitors and a plurality of switching components, wherein each current monitor of the plurality of current monitors and each switching component of the plurality of switching components is connected in series with one respective return electrode of the plurality of return electrodes, the plurality of current monitors being configured to measure the electrosurgical current passing therethrough;a processor coupled to each current monitor of the plurality of current monitors and each switching component of the plurality of switching components, the processor configured to determine a current threshold based on an average current load among the plurality of return electrodes and a tolerance value;a comparator configured to perform a comparison of the electrosurgical current passing through at least one of the plurality of return electrodes with the current threshold; anda controller configured to control each switching component of the plurality of switching components to adjust the electrosurgical current passing through each return electrode of the plurality of return electrodes to balance the average current load based on a result of the comparison performed by the comparator.
  • 2. The system according to claim 1, wherein the plurality of switching components are configured to be operated via a pulse width modulated control signal.
  • 3. The system according to claim 1, wherein the plurality of switching components are configured to adjust the electrosurgical current by opening a circuit of the at least one of the plurality of return electrodes.
  • 4. The system according to claim 3, wherein the circuit of the at least one of the plurality of return electrodes is configured to be opened for at least a time-off period.
  • 5. The system according to claim 4, wherein the processor is configured to calculate the time-off period as a function of the electrosurgical current measured by the plurality of current monitors.
  • 6. The system according claim 1, further including a plurality of impedance sensors, wherein each impedance sensor of the plurality of impedance sensors is coupled to one respective return electrode of the plurality of return electrodes.
  • 7. The system according to claim 1, wherein each switching component of the plurality of switching components is selected from the group consisting of a relay and a transistor.
US Referenced Citations (246)
Number Name Date Kind
2536271 Fransen et al. Jan 1951 A
3380445 Frasier Apr 1968 A
3534306 Watrous et al. Oct 1970 A
3543760 Bolduc Dec 1970 A
3642008 Bolduc Feb 1972 A
3683923 Anderson Aug 1972 A
3812861 Peters May 1974 A
3913583 Bross Oct 1975 A
3923063 Andrews et al. Dec 1975 A
3933157 Bjurwill et al. Jan 1976 A
3987796 Gonser Oct 1976 A
4067342 Burton Jan 1978 A
4092985 Kaufman Jun 1978 A
4094320 Newton et al. Jun 1978 A
4102341 Ikuno et al. Jul 1978 A
4114622 Gonser Sep 1978 A
4117846 Williams Oct 1978 A
4121590 Gonser Oct 1978 A
4126137 Archibald Nov 1978 A
4166465 Esty et al. Sep 1979 A
4188927 Harris Feb 1980 A
4200104 Harris Apr 1980 A
4200105 Gonser Apr 1980 A
4213463 Osenkarski Jul 1980 A
4231372 Newton Nov 1980 A
4237887 Gonser Dec 1980 A
4253721 Kaufman Mar 1981 A
4303073 Archibald Dec 1981 A
4304235 Kaufman Dec 1981 A
4331149 Gonser May 1982 A
4343308 Gross Aug 1982 A
4381789 Naser et al. May 1983 A
4384582 Watt May 1983 A
4387714 Geddes et al. Jun 1983 A
4393584 Bare et al. Jul 1983 A
4416276 Newton et al. Nov 1983 A
4416277 Newton et al. Nov 1983 A
4437464 Crow Mar 1984 A
4494541 Archibald Jan 1985 A
4643193 DeMarzo Feb 1987 A
4657015 Irnich Apr 1987 A
4658819 Harris et al. Apr 1987 A
4662369 Ensslin May 1987 A
4669468 Cartmell et al. Jun 1987 A
4699146 Sieverding Oct 1987 A
4722761 Cartmell et al. Feb 1988 A
4725713 Lehrke Feb 1988 A
4741334 Irnich May 1988 A
4745918 Feucht May 1988 A
4748983 Shigeta et al. Jun 1988 A
4750482 Sieverding Jun 1988 A
4754757 Feucht Jul 1988 A
4768514 DeMarzo Sep 1988 A
4770173 Feucht et al. Sep 1988 A
4788977 Farin et al. Dec 1988 A
4799480 Abraham et al. Jan 1989 A
4807621 Hagen et al. Feb 1989 A
4844063 Clark Jul 1989 A
4848335 Manes Jul 1989 A
4862889 Feucht Sep 1989 A
4873974 Hagen et al. Oct 1989 A
4895169 Heath Jan 1990 A
4942313 Kinzel Jul 1990 A
4947846 Kitagawa et al. Aug 1990 A
4955381 Way et al. Sep 1990 A
4961047 Carder Oct 1990 A
4969885 Farin Nov 1990 A
5000753 Hagen et al. Mar 1991 A
5004425 Hee Apr 1991 A
5010896 Westbrook Apr 1991 A
5038796 Axelgaard et al. Aug 1991 A
5042981 Gross Aug 1991 A
5061914 Busch et al. Oct 1991 A
5087257 Farin et al. Feb 1992 A
5114424 Hagen et al. May 1992 A
5152762 McElhenney Oct 1992 A
5160334 Billings et al. Nov 1992 A
5196008 Kuenecke et al. Mar 1993 A
5246439 Hebborn et al. Sep 1993 A
5271417 Swanson et al. Dec 1993 A
5276079 Duan et al. Jan 1994 A
5286255 Weber Feb 1994 A
5312401 Newton et al. May 1994 A
5336255 Kanare et al. Aug 1994 A
5352315 Carrier et al. Oct 1994 A
5362420 Itoh et al. Nov 1994 A
5370645 Klicek et al. Dec 1994 A
5385679 Uy et al. Jan 1995 A
5388490 Buck Feb 1995 A
5389376 Duan et al. Feb 1995 A
5390382 Hannant et al. Feb 1995 A
5409966 Duan et al. Apr 1995 A
5447513 Davison et al. Sep 1995 A
5449365 Green et al. Sep 1995 A
5452725 Martenson Sep 1995 A
5480399 Hebborn Jan 1996 A
5496312 Klicek Mar 1996 A
5496363 Burgio et al. Mar 1996 A
5520180 Uy et al. May 1996 A
5536446 Uy et al. Jul 1996 A
5540684 Hassler, Jr. Jul 1996 A
5599347 Hart et al. Feb 1997 A
5601618 James Feb 1997 A
5611709 McAnulty Mar 1997 A
5632280 Leyde et al. May 1997 A
5643319 Green et al. Jul 1997 A
5660892 Robbins et al. Aug 1997 A
5670557 Dietz et al. Sep 1997 A
5674561 Dietz et al. Oct 1997 A
5678545 Stratbucker Oct 1997 A
5688269 Newton et al. Nov 1997 A
5695494 Becker Dec 1997 A
5707369 Vaitekunas et al. Jan 1998 A
5718719 Clare et al. Feb 1998 A
5720744 Eggleston et al. Feb 1998 A
5766165 Gentelia et al. Jun 1998 A
5779632 Dietz et al. Jul 1998 A
5797902 Netherly Aug 1998 A
5800426 Taki et al. Sep 1998 A
5817091 Nardella et al. Oct 1998 A
5830212 Cartmell et al. Nov 1998 A
5836942 Netherly et al. Nov 1998 A
5846558 Nielsen et al. Dec 1998 A
5853750 Dietz et al. Dec 1998 A
5868742 Manes et al. Feb 1999 A
5924983 Takaki et al. Jul 1999 A
5947961 Netherly Sep 1999 A
5952398 Dietz et al. Sep 1999 A
5971981 Hill et al. Oct 1999 A
5976128 Schilling et al. Nov 1999 A
5985990 Kantner et al. Nov 1999 A
5999061 Pope et al. Dec 1999 A
6007532 Netherly Dec 1999 A
6010054 Johnson et al. Jan 2000 A
6030381 Jones et al. Feb 2000 A
6032063 Hoar et al. Feb 2000 A
6039732 Ichikawa et al. Mar 2000 A
6053910 Fleenor Apr 2000 A
RE36720 Green et al. May 2000 E
6059778 Sherman May 2000 A
6063075 Mihori May 2000 A
6083221 Fleenor et al. Jul 2000 A
6086249 Urich Jul 2000 A
6121508 Bischof et al. Sep 2000 A
6135953 Carim Oct 2000 A
6171304 Netherly et al. Jan 2001 B1
6200314 Sherman Mar 2001 B1
6203541 Keppel Mar 2001 B1
6214000 Fleenor et al. Apr 2001 B1
6232366 Wang et al. May 2001 B1
6240323 Calenzo, Sr. et al. May 2001 B1
6258085 Eggleston Jul 2001 B1
6275786 Daners Aug 2001 B1
6301500 Van Herk et al. Oct 2001 B1
6310611 Caldwell Oct 2001 B1
6347246 Perrault et al. Feb 2002 B1
6350264 Hooven Feb 2002 B1
6357089 Koguchi et al. Mar 2002 B1
6358245 Edwards et al. Mar 2002 B1
6379161 Ma Apr 2002 B1
6409722 Hoey et al. Jun 2002 B1
6413255 Stern Jul 2002 B1
6415170 Loutis et al. Jul 2002 B1
6454764 Fleenor et al. Sep 2002 B1
6488678 Sherman Dec 2002 B2
6537272 Christopherson et al. Mar 2003 B2
6544258 Fleenor et al. Apr 2003 B2
6546270 Goldin et al. Apr 2003 B1
6565559 Eggleston May 2003 B2
6569160 Goldin et al. May 2003 B1
6582424 Fleenor et al. Jun 2003 B2
6666859 Fleenor et al. Dec 2003 B1
6669073 Milliman et al. Dec 2003 B2
6736810 Hoey et al. May 2004 B2
6796828 Ehr et al. Sep 2004 B2
6799063 Carson Sep 2004 B2
6830569 Thompson et al. Dec 2004 B2
6849073 Hoey et al. Feb 2005 B2
6860881 Sturm Mar 2005 B2
6875210 Refior et al. Apr 2005 B2
6892086 Russell May 2005 B2
6905497 Truckai et al. Jun 2005 B2
6939344 Kreindel Sep 2005 B2
6948503 Refior et al. Sep 2005 B2
6953139 Milliman et al. Oct 2005 B2
6959852 Shelton, IV et al. Nov 2005 B2
6997735 Ehr et al. Feb 2006 B2
7025765 Balbierz et al. Apr 2006 B2
7128253 Mastri et al. Oct 2006 B2
7143926 Shelton, IV et al. Dec 2006 B2
7160293 Sturm et al. Jan 2007 B2
7166102 Fleenor et al. Jan 2007 B2
7169144 Hoey et al. Jan 2007 B2
7169145 Isaacson Jan 2007 B2
7182604 Ehr et al. Feb 2007 B2
7220260 Fleming et al. May 2007 B2
7229307 Ehr et al. Jun 2007 B2
7258262 Mastri et al. Aug 2007 B2
7267675 Stern et al. Sep 2007 B2
7278562 Mastri et al. Oct 2007 B2
7303107 Milliman et al. Dec 2007 B2
7308998 Mastri et al. Dec 2007 B2
7311560 Ehr et al. Dec 2007 B2
7357287 Shelton, IV et al. Apr 2008 B2
7380695 Doll et al. Jun 2008 B2
7422589 Newton et al. Sep 2008 B2
7473145 Ehr et al. Jan 2009 B2
7637907 Blaha Dec 2009 B2
7736357 Lee, Jr. Jun 2010 B2
7736359 McPherson Jun 2010 B2
7837680 Isaacson Nov 2010 B2
20030139741 Goble et al. Jul 2003 A1
20040150504 Nicholson Aug 2004 A1
20050021022 Sturm et al. Jan 2005 A1
20050085806 Auge, II et al. Apr 2005 A1
20050101947 Jarrard et al. May 2005 A1
20050251130 Boveja et al. Nov 2005 A1
20060041251 Odell et al. Feb 2006 A1
20060041252 Odell et al. Feb 2006 A1
20060041253 Newton et al. Feb 2006 A1
20060074411 Carmel et al. Apr 2006 A1
20060079872 Eggleston Apr 2006 A1
20060173250 Nessler Aug 2006 A1
20060217742 Messerly et al. Sep 2006 A1
20060224150 Arts et al. Oct 2006 A1
20070049914 Eggleston Mar 2007 A1
20070049916 Isaacson et al. Mar 2007 A1
20070049919 Lee, Jr. et al. Mar 2007 A1
20070073284 Sturm et al. Mar 2007 A1
20070074719 Danek et al. Apr 2007 A1
20070161979 McPherson Jul 2007 A1
20070167942 Rick Jul 2007 A1
20070203481 Gregg et al. Aug 2007 A1
20070244478 Bahney Oct 2007 A1
20080009846 Ward Jan 2008 A1
20080033276 Ehr et al. Feb 2008 A1
20080071263 Blaha Mar 2008 A1
20080083806 Scirica Apr 2008 A1
20080083813 Zemlok et al. Apr 2008 A1
20080249520 Dunning et al. Oct 2008 A1
20080249524 Dunning Oct 2008 A1
20080281309 Dunning et al. Nov 2008 A1
20080281310 Dunning et al. Nov 2008 A1
20080281311 Dunning et al. Nov 2008 A1
20090036884 Gregg et al. Feb 2009 A1
20090036885 Gregg Feb 2009 A1
Foreign Referenced Citations (47)
Number Date Country
1219642 Mar 1987 CA
3206947 Sep 1983 DE
3544443 Jun 1987 DE
42 38 263 May 1993 DE
4231236 Mar 1994 DE
197 17 411 Nov 1998 DE
198 01 173 Jul 1999 DE
103 28 514 Jun 2003 DE
102004010940 Sep 2005 DE
0262888 Apr 1988 EP
390937 Oct 1990 EP
836868 Apr 1998 EP
0 930 048 Jul 1999 EP
1 051 949 Nov 2000 EP
1076350 Feb 2001 EP
1 468 653 Oct 2004 EP
1 645 236 Apr 2006 EP
1707151 Oct 2006 EP
1 808 144 Jul 2007 EP
1902684 Mar 2008 EP
2276027 Jun 1974 FR
2516782 May 1983 FR
2 054 382 Feb 1981 GB
2374532 Oct 2002 GB
WO 9619152 Jun 1996 WO
WO 9737719 Oct 1997 WO
WO 9818395 May 1998 WO
WO 9853751 Dec 1998 WO
WO 9909899 Mar 1999 WO
WO 9911187 Mar 1999 WO
WO 0006246 Feb 2000 WO
WO 0032122 Jun 2000 WO
WO 0053113 Sep 2000 WO
WO 0065993 Nov 2000 WO
WO 0187175 Nov 2001 WO
WO 02058579 Aug 2002 WO
WO 02060526 Aug 2002 WO
WO 02099442 Dec 2002 WO
WO 03094766 Nov 2003 WO
WO 2004028385 Apr 2004 WO
WO 2004074854 Sep 2004 WO
WO 2005048809 Jun 2005 WO
WO 2005087124 Sep 2005 WO
WO 2005099606 Oct 2005 WO
WO 2005110263 Nov 2005 WO
WO 2005115262 Dec 2005 WO
WO 2008009385 Jan 2008 WO
Non-Patent Literature Citations (28)
Entry
International Search Report EP 05021944.3 dated Jan. 25, 2006.
International Search Report EP 05002027.0 dated May 12, 2005.
International Search Report EP 06006961 dated Aug. 3, 2006.
International Search Report EP 07000885.9 dated May 15, 2007.
International Search Report PCT/US2004/004196 dated Oct. 4, 2007.
International Search Report EP06006961.4 dated Oct. 5, 2007.
International Search Report EP07000885.9 dated May 2, 2007.
International Search Report EP07007783.9 dated Aug. 6, 2007.
International Search Report EP06018206.0 dated Oct. 13, 2006.
International Search Report EP07000567.3 dated Dec. 3, 2008.
International Search Report EP08006731 dated Jul. 14, 2008.
International Search Report EP08006735.8 dated Jan. 8, 2009.
International Search Report EP08008510.3 dated Oct. 27, 2008.
International Search Report EP08013758.1 dated Nov. 20, 2008.
International Search Report EP08013760.7 dated Nov. 20, 2008.
International Search Report EP08155779-partial dated Sep. 8, 2008.
International Search Report EP08155779 dated Jan. 23, 2009.
International Search Report EP09152032 dated Jun. 17, 2009.
International Search Report EP09152130.2 dated Apr. 6, 2009.
Boyles, Walt; “Instrumentation Reference Book”, 2002; Butterworth-Heinemann ; 262-264.
International Search Report EP06023756.7 dated Feb. 21, 2008.
International Search Report EP07018375.1 dated Jan. 8, 2008.
International Search Report EP07019173.9 dated Feb. 12, 2008.
International Search Report EP07019178.8 dated Feb. 12, 2008.
International Search Report EP07253835.8 dated Feb. 20, 2007.
International Search Report EP08006731.7 dated Jul. 29, 2008.
International Search Report EP08006734.1 dated Aug. 18, 2008.
European Search Report for European Application No. 11179857.5 dated Nov. 17, 2011.
Related Publications (1)
Number Date Country
20090036884 A1 Feb 2009 US