Patent Application
20080050702
a and 1b illustrates a root canal system including the main root canal and all of the accessory or lateral canals that branch off of the main canal (1a). Some of these accessory canals are very small and extremely difficult to reach in order to eliminate any bacteria and/or viruses. Such accessory canals may bend, twist, change cross-section and/or become long and small as they branch off from the main canal, making them very difficult to access or target therapeutically. 1b is a simplified graphical representation of the same.
The present invention is useful for treating dental, medical, and veterinary problems; primarily dental surface preparations. The present invention uses enhanced photoacoustic wave generation in dental, medical, and veterinary application during procedures that otherwise face reoccurring infection, inefficient performance and at an increase in expenses. The result of this invention has the potential to increase the effective cleaning of the root canal and accessory canals and the potential to reduce future failures over time.
The most preferred embodiment of the present invention utilizes an energy source is preferably a pulsed laser energy that is coupled to a solution in such a fashion that it produces and enhanced photoacoustic pressure wave. The laser light is delivered using a commercially available laser source 10 and an optical light fiber 15 attached at a proximate end to the laser source 10 and has an application tip 20 at the distal end. The application tip 20 may be flat or blunt, but is preferably a beveled or tapered tip having a taper angle 22 between 10 and 90 degrees. Preferably any cladding 24 on the optic fiber is stripped from approximately 2-12 mm of the distal end. The taper angle of the fiber tip 20 and removal of the cladding provide wider dispersion of the laser energy over a larger tip area and consequently produces a larger photoacoustic wave. The most preferred embodiment of the application tip includes a texturing 26 or deriviatization of the beveled tip, thereby increasing the efficacy of the conversion of the laser energy into photoacoustic wave energy within the solution. It should be noted that in the present invention this tapered tip, the surface treatment, and the sheath stripping is not for the purpose of diffusing or refracting the laser light so that it laterally transmits radiant optical light energy to the root surface. In the current invention these features are for the sole purpose of increasing the photoacoustic wave.
Herein derivatization means a technique used in chemistry that bonds, either covalently or non-covalently, inorganic or organic chemical functional group to a substrate surface.
It was found that the photoacoustic coupling of the laser energy to the solution provides enhanced penetration of the solution into the root canal and accessory canals, thereby allowing the solution to reach areas of the canal system that are not typically accessible.
The photoacoustic (PA) wave is generated when the laser energy transitions from the tip (usually quartz or similar material) of the laser device into the fluid (such as water, EDTA, or the like. The transmission from one medium to another is not 100% efficient and some of the light energy is turned into heat near the transition that the light makes from one media to the other. This heating is very rapid, locally heating some of the molecules of the fluid very rapidly, resulting in molecule expansion and generating the photoacoustic wave. In a pulsed laser, a wave is generated each time the laser is turned on, which is once per cycle. A 10 HZ pulsed laser then generates 10 waves per second. If the power level remains constant, the lower the pulse rate, the greater the laser energy per pulse and consequently the greater the photoacoustic wave per pulse.
The photoacoustic effect creates sound (pressure) waves that can potentially propagate throughout both the media and localized structure, e.g., the main root canal and the lateral or accessory canals. These sound waves provide vibrational energy, which expedites the breaking loose of and/or causing cell lysis of the biotics and inorganics in the root canal and lateral canal systems. In addition these vibrational waves helping the propagation of the fluids into and throughout the main and lateral canal systems. In fact such radiant light energy can fuse the root canal wall surface making it impossible to clean and debride the small passages behind the fused areas.
In general, light travels in a straight line, however, in a fluid light can be bent and transmitted around corners, but this transmission is minimal compared to the straight-line transmissibility of light. A sonic or shock wave on the other hand is easily transmitted around corners and through passages in a fluid. For example, air is a fluid. If you stood in one room and shined a bright light from that room into a hallway that was at right angles to that room, the intensity of the light would decrease the farther you go down the hallway. If you then went into a room at the end of the hallway and went to a back corner of the room, the light might be very dim. However, if while standing at the same location as the light source, you yelled vocally at the hallway, you could most likely hear the sound in the back corner of the back room. This is because sound is propagated spherically by the vibration of molecules instead of primarily in a straight line like light.
Although the laser light cannot turn corners easily and cannot propagate easily into the lateral canals, the sonic wave produced by the photoacoustic effect is easily transmitted through the lateral canals. Also, since the canals are tapered in a concave fashion, the photoacoustic wave will be amplified as it transverses toward the end of the lateral canals. Since the cross-sectional area of the lateral canals decreases as the wave traverses toward the canal end, the amplitude of the wave increases much as a Tsunami wave increases as it approaches a beach where the cross sectional area of the water channel constantly decreases.
The tip design can affect the magnitude and direction of the produced photoacoustic wave. A tapered tip has the effect of diverting the laser energy over the larger cone area (compared to the circular area of the standard tip) and thereby creating a larger photoacoustic wave. The same applies to any stripped sheath section of the tip.
Testing using a MEMS Pressure sensor:
A small plastic vial was fitted with a fluid connection (bottom of vial at right angles to axis of vial) that was close coupled hydraulically to a miniature MEMS piezo-resistive pressure sensor (Honeywell Model 24PCCFA6D). The sensor output was run through a differential amplifier and coupled to a digital Oscilloscope (Tektronics Model TDS 220). This model oscilloscope will hold a trace on the screen and allow a digital image to be taken of the trace. The vial and sensor were filled with water. The laser tip was submerged below the fluid level in the vial and fired (laser frequency was 10 HZ) at various power setting. A trace was recorded of the resulting photoacoustic pressure waves.
A 170% increase in the photoacoustic wave was observed for the tapered and stripped tip versus the blunt-ended tip. A 580% increase in the photoacoustic wave was observed for textured (frosted) tapered/stripped tip versus the standard blunt-ended tip. The tapered tip has a greater exposed area than the blunt straight tip. The fiber optic tip is coated with a polyamide sheath, which reflects the laser beam internally, not allow it to escape and propagating the laser energy down the fiber to the tip. On the straight or blunt-end tip, the exposed area is the circular cross-sectional area of the end of the tip. On the tapered tip and textured tip the exposed area is the area of the tapered cone, which is greater than the exposed area of the blunt straight tip. This invention is on the ability of these features to increase the photoacoustic wave not to refract or redirect the radiant optical properties of the laser energy.
During a previous experiment, fluid was placed into a Dampen dish located on a Formica surface. The laser tip was placed into the fluid and fired repetitively. The photoacoustic wave vibrated the Dampen dish on the Formica surface making an audible sound. For a specific tip this audible sound increased with an increasing power level of the laser. This implies that the audible sound is somewhat proportional to the amplitude of the photoacoustic wave. This was verified by placing a sound level meter one inch away from the Dampen dish and recording the dB level. Next, the laser power level was held constant and the tip was changed. The tapered and stripped sheath tip produced a greater photoacoustic wave than the standard straight or blunt-end tip. A tapered and stripped tip was then frosted or etched. This tip was tested and showed a greater photoacoustic wave generated than the non-frosted version. This was verified to be true at three different power levels. It would appear that since the power level was held constant, the photoacoustic wave amplitude would also be proportional to the exposed area and the surface treatment.
An increase in photoacoustic wave generation was seen by stripping the polyamide sheath away for 2-12 mm from the tapered end. Although laser light is coherent and travels in a straight line, some light bounces off of the polyamide sheath at an angle. As this light travels down the light path it continues bouncing off of the inside of the polyamide sheath and will eventually exit at an angle to the sheath once the sheath stops and exposes a non sheathed section. Therefore, some of the laser energy would also exit where the polyamide sheath has been removed, just upstream of the tapered tip. A tip with the sheath removed for 2 to 12 mm directly upstream of the tapered section was placed in the above-mentioned test set up.
The photoacoustic wave will propagate primarily perpendicular to the exposed surface and secondarily spherically with respect to the exposed surface. The standard straight end tip would have the PA wave propagating primarily in line with the tips The tapered tip produced PA wave would be primarily propagated in a more lateral pattern. The tapered tip with the shinned sheath would propagate the PA wave in a more spherical pattern than the other two.
The standard straight blunt end tip would be less desirable because it directs the photoacoustic wave toward the apical end of the tooth and would have more propensities to drive the fluid from the nerve hole in the apical end and outward into the gum which could create medical complications. Since there may be lateral or accessory canals anywhere along the main root canal, it is more desirable to have a spherical wave distribution to direct waves to as many lateral canals as possible. Therefore the tapered tip with the skinned sheath produces a more desirable effect within the tooth.
Resultant Scanning Electron Micrographs (SEM's) show the reticular surface of the dentin to be devoid of infection and malady and allowing for rinsed removal of the debris elements.
The present invention also includes embodiments of the individual components, kits, methods, their manufacture, and their assembly into one singular procedure. Still further herein included are methods and processes for use of the individual components and the integration in biological applications.
All publications and patent applications are herein incorporated by reference to the same extent as if each individual publication or patent application was specifically and individually indicated to be incorporated by reference. Although the present invention has been described in some detail by way of illustration and example for purposes of clarity and understanding, it will be apparent that certain changes and modifications may be practiced within the scope of the appended claims.
The preferred embodiment of the invention is described above in the Drawings and Description of Preferred Embodiments. While these descriptions directly describe the above embodiments, it is understood that those skilled in the art may conceive modifications and/or variations to the specific embodiments shown and described herein. Any such modifications or variations that fall within the purview of this description are intended to be included therein as well. Unless specifically noted, it is the intention of the inventor that the words and phrases in the specification and claims be given the ordinary and accustomed meanings to those of ordinary skill in the applicable art(s). The foregoing description of a preferred embodiment and best mode of the invention known to the applicant at the time of filing the application has been presented and is intended for the purposes of illustration and description. It is not intended to be exhaustive or to limit the invention to the precise form disclosed, and many modifications and variations are possible in the light of the above teachings. The embodiment was chosen and described in order to best explain the principles of the invention and its practical application and to enable others skilled in the art to best utilize the invention in various embodiments and with various modifications as are suited to the particular use contemplated.
This application is a continuation-in part of provisional application Ser. No. 60/840,282 filed on Aug. 24, 2006.
| Number | Date | Country | |
|---|---|---|---|
| 60840282 | Aug 2006 | US |
