SONOTRODE

RELATED APPLICATION

The present application gains priority from US Provisional Patent Application 62/302,875 filed 3 March 2016, which is included by reference as if fully set-forth herein and is also attached hereto in its entirety as an Appendix.

FIELD AND BACKGROUND OF THE INVENTION

The invention, in some embodiments, relates to the field of treatment of body tissue with acoustically-delivered energy and more particularly, but not exclusively, to methods and devices for treatment of subcutaneous fat by simultaneously transdermaily inducing both ultrasonic transverse vibrations and ultrasonic longitudinal vibrations in subcutaneous tissue thereby acoustically delivering energy through the skin, for example for reduction of subcutaneous fat by applying ultrasonic vibrations to a skin surface,

In the art it is known to apply ultrasonic vibrations to a skin surface to transdermaily induce ultrasonic vibrations to acoustically deliver energy to subcutaneous tissue such as a subcutaneous fat layer to damage adipocytes, for example in the field of body sculpting.

Application of ultrasonic vibrations to a surface is typically performed by a device 10 (see Figure 1 ) that includes a proximal ultrasonic transducer 12 for generation of ultrasomc longitudinal vibrations (e.g., a Langevin-type transducer comprising a stack of piezoelectric elements) having a proximal face 14 functionally associated with an acoustic reflector 16 and a distal face 18 and a distal sonotrode 20 having a proximal face 22, a distal end 24 defining a working face 26 that constitutes an acoustic radiative surface and a sonotrode axis 28, where the proximal face 22 of the sonotrode 20 is acoustically coupled to the distal face 18 of the ultrasonic transducer 12.

For use, while the working face 26 of the sonotrode 20 is acoustically coupled to a surface 30 of a medium 32 (e.g., by direct contact or by indirect contact through a coupling substance, e.g., a liquid or gel), an alternating current (AC) oscillating at an ultrasonic driving frequency is supplied from an ultrasound power supply 34 to drive the ultrasonic transducer 12. The piezoelectric elements of the ultrasonic transducer 12 expand and relax at the driving frequency in response to the oscillations of the AC potential, thereby generating ultrasonic longitudinal vibrations with the frequency of the driving frequency. The generated ultrasomc longitudinal vibrations propagate in parallel with the axis 28 through the sonotrode 20 from the proximal face 22 to the working face 26, The working face 26 applies the ultrasonic longitudinal vibrations to the surface 30, inducing ultrasoni c longitudinal vibrations in the medium 32.

For practical use it is advantageous to configure a sonotrode to function as an acoustic amplitude transformer (also called a horn) that increases the amplitude of the ultrasonic longitudinal vibrations (i.e., the maximal displacement of distal working face 26) from being relatively small at the proximal face 22 of the sonotrode 20 to substantially larger at working face 26, typically to between 10 and 150 micrometers. Such configuration includes that the sonotrode tapers from a large cross section proximal end 22 to a small cross section working face 26 and that the total length 36 of the sonotrode (from proximal face 22 to working face 26) is an integral multiple of XL/2, XL being the wavelength of the ultrasonic longitudinal vibrations in the sonotrode which is dependent on the driving frequency and on the longitudinal speed of sound along the axis 28 so that the sonotrode functions as a half- wavelength resonator. The most popular such acoustic amplitude transformer configurations are schematically depicted in side cross section in Figures 2: Figure 2A a linear taper sonotrode 38a, Figure 2B an exponential taper sonotrode 38b, and Figure 2C a stepped taper sonotrode 38c.

When a sonotrode 20, 38a, 38b or 38c, as depicted in Figures 1, 2 A, 2B or 2C respectively is used, the ultrasonic vibrations in the sonotrode and that are induced in a medium are predominantly, if not entirely, longitudinal vibrations that propagate collinearly with the axis 28 of the sonotrode. The biological effects of energy transdermaliy delivered by ultrasonic longitudinal vibrations primarily arise from heating of tissue, especially heating of the dermis.

In patent publication US 201 1 /0213279 which is included by reference as if fully set- forth herein, some of the Inventors disclosed a "mushroom- shaped" sonotrode. In Figure 2d, such a mushroom-shaped sonotrode 38d is schematically depicted in side cross section having a tapering stem 40 that functions as an acoustic amplitude transformer as described above (particularly sonotrode 38c depicted in Figure 2C) and a broader cap 42. Cap 42 is lenticular, in side cross section resembling a lens having a curved back side 44 and a convex working face 26. Working face 26 of sonotrode 38d also includes concentric circular transverse-wave transferring ridges 46.

As detailed in US 201 1/0213279, a sonotrode such as 38d is operative to transdermaliy induce, depending on the value of the driving frequency, either ultrasonic longitudinal vibrations or ultrasonic transverse vibrations in subcutaneous tissue when the working face 26 is acoustically coupled with skin . Without wishing to be held to any one theory, it is currently believed that with some driving frequencies the ultrasonic longitudinal vibrations generated by an ultrasonic transducer 12 preferentially propagate in parallel with the axis 28 of mushroom-shaped sonotrode such as 38d from the proximal face 22 to the working face 26. These ultrasonic longitudinal vibrations primarily lead to ultrasonic longitudinal vibrations of the sonotrode 38d, which are applied by working face 26 to a skin surface acoustically coupled with working face 26, transdermally inducing ultrasonic longitudinal vibrations in the subcutaneous tissue.

However, with some other different driving frequencies the ultrasonic longitudinal vibrations generated by an ultrasonic transducer 12 preferentially produce ultrasonic shear wave vibrations in the cap 42 of sonotrode 38d, the ultrasonic shear wave vibrations being perpendicular to the longitudinal vibrations in the stem 40, that is to say, a greater proportion of the energy transferred by the transducer 12 into the sonotrode 38d is in ultrasonic shear wave vibrations in the cap 42 perpendicular to axis 28 rather than ultrasonic longitudinal vibrations parallel or collinear with axis 28. As a result, working face 26 substantially vibrates transversely, presumably alternately increasing and decreasing in diameter. When the vibrating working face 26 is applied to a skin surface, the ultrasonic shear wave vibrations induce ultrasonic transverse vibrations in the subcutaneous tissue by virtue of the convex shape of working face 26 and by virtue of the concentric circular transverse-wave transferring ridges 46 that can be considered as physically moving the skin and tissue transversely.

A device including a sonotrode such as 38d provides two modes of operation that are advantageously serially activated:

at a first driving frequency that is related to the wavelength XL for which the sonotrode 38d is configured to act as an acoustic amplitude transformer, a first "hot" or "longitudinal" mode where the energy transdermally delivered to subcutaneous tissue through the working face 26 is primarily by ultrasonic longitudinal vibrations that are perpendicular to the skin surface; and

at a second driving frequency different from the first driving frequency, a second "cold" or "transverse" mode where the energy transdermally delivered to

In some preferred embodiments described in US 201 1/0213279, ultrasonic longitudinal vibrations of the first mode and ultrasonic shear wave vibrations of the second mode are alternately applied through a mushroom -shaped sonotrode such as 38d described above. The ultrasonic longitudinal vibrations are applied by the working face to the skin surface (typically for a duration of about 5 seconds) to transdermally induce ultrasonic longitudinal waves that heat subcutaneous tissue such as the dermis. Subsequently ultrasonic shear wave vibrations are applied by the working face to the skin surface (typically for a duration of about 15 seconds) to induce ultrasonic transverse vibrations to disrupt the adipocytes. Because of the preceding heating by the ultrasonic longitudinal vibrations, the ultrasonic transverse vibrations penetrate more deeply and/or more effectively and/or a greater fraction of the energy penetrates to a given depth of the adipose tissue and/or the heated tissue has improved energy-absorbing properties.

Although highly effective in the field of body sculpting, a sonotrode such as described in US 201 1/0213279 is sometimes considered less than ideal for some uses because the shear wave vibrations are not applied continuously, because of the added complexity required for generating and switching between two different driving frequencies and because if a user moves the working face over different portions of a treated subjects too quickly, the results of a treatment might be considered less than ideal, SUMMARY OF THE INVENTION

The invention, in some embodiments, relates to the treatment of body tissue with energy and more particularly, but not exclusively, to methods and devices for treatment of subcutaneous fat by simultaneously transdermally inducing both ultrasonic transverse vibrations and ultrasonic longitudinal vibrations in subcutaneous tissue, for example for reduction of subcutaneous fat.

According to an aspect of some embodiments of the invention there is provided a device suitable for treating subcutaneous adipose tissue, comprising:

a. an ultrasonic transducer for generation of ultrasonic vibrations having a proximal face and a distal face, and

b. a sonotrode including a narrower proximal stem portion defining a sonotrode axis and a broader distal cap portion

wherein the stem portion has a distal end and bears a proximal face of the sonotrode, the sonotrode acoustically coupled to the distal face of the ultrasonic transducer through the proximal face of the sonotrode. wherein the cap portion has a proximally-facing back side, a distal working face of the sonotrode and a periphery,

wherein the distal end of the stem portion meets the back side of the cap portion,

wherein where the distal end of the stem portion meets the back side of the cap portion a cross sectional area of the cap portion perpendicular to the sonotrode axis is not less than 4 times greater than a cross sectional area of the distal end of the stem portion perpendicular to the sonotrode axis; and

wherein said sonotrode is configured as an acoustic amplitude transformer for a selected ultrasonic frequency.

According to an aspect of some embodiments of the invention, there is also provided a method of transdermally treating subcutaneous fat comprising:

i. providing a device according to the teachings herein, wherein the ultrasonic transducer is functionally associated with an ultrasound power supply:

ii. for a treatment event having a duration, maintaining the working face acoustically coupled with a skin surface while the ultrasound power supply is activated to supply a driving current having the selected ultrasonic frequency to the ultrasonic transducer,

thereby simultaneously transdermally inducing both:

ultrasonic longitudinal vibrations sufficient to convey sufficient energy to substantially heat subcutaneous tissue; and

ultrasonic transverse vibrations in subcutaneous tissue to convey sufficient energy to disrupt adipocytes in the subcutaneous tissue.

According to an aspect of some embodiments of the invention there is also provided a method of transdermally treating subcutaneous fat, comprising:

i. providing a plate having a working face,

ii. acoustically coupling the plate through the working face with a skin surface; and iii. forming ultrasonic-frequency cylindrical plate waves in the plate with a perpendicular line source,

wherein the cylindrical plate waves formed in the plate lead to ultrasonic flexural vibrations of the plate that transdermally induce ultrasonic transverse waves in subcutaneous tissue, thereby treating subcutaneous fat. In some embodiments, the ultrasonic transverse waves disrupt adipocytes in the subcutaneous tissue. In some embodiments, the perpendicular line source is an ultrasonic longitudinal wave. In some embodiments, the method further comprises simultaneously with the transdermally inducing ulltrasonic transverse waves in subcutaneous tissue, transdermaily inducing ultrasonic longitudinal waves in subcutaneous tissue. In some embodiments, the ultrasonic longitudinal waves heat the subcutaneous tissue. In some embodiments, the ultrasonic transverse waves are induced in the subcutaneous tissue with an ultrasonic longitudinal wave that propagates perpendicularly to the plate and constitutes the perpendicular line source.

Typically, the method is non-invasive, that is to say the skin surface remains intact, and is not punctured or otherwise penetrated. In some embodiments, the method is a non- surgical method, performed without breaking the skin. Embodiments of the method are performed by any suitable person, including medical personnel but typically aesthetic technicians such as beauticians.

US Provisional Patent Application 62/302,875 filed 3 March 2016, from which the instant application gains priority, is attached hereto in its entirety as an Appendix. The Appendix is an integral part of the application.

Unless otherwise defined, all technical and scientific terms used herein have the same meaning as commonly understood by one of ordinary skill in the art to which the invention pertains. In case of conflict, the specification, including definitions, will control,

As used herein, the terms "comprising", "including", "having" and grammatical variants thereof are to be taken as specifying the stated features, integers, steps or components but do not preclude the addition of one or more additional features, integers, steps, components or groups thereof. These terms encompass the terms "consisting of and "consisting essentially of .

As used herein, the indefinite articles "a" and "an" mean "at least one" or "one or more" unless the context clearly dictates otherwise. "

BRIEF DESCRIPTION OF THE FIGURES

Some embodiments of the invention are described herein with reference to the accompanying figures. The description, together with the figures, makes apparent to a person having ordinary skill in the art how some embodiments of the invention may be practiced. The figures are for the purpose of illustrative discussion and no attempt is made to show structural details of an embodiment in more detail than is necessary for a fundamental understanding of the invention. For the sake of clarity, some objects depicted in the figures are not to scale.

In the Figures:

FIG. 1 (prior art) schematically depicts a device for application of ultrasonic vibrations into a medium through a surface of the medium,

FIGS. 2A, 2B, 2C and 2D (prior art) schematically depict different sonotrodes configured to function as acoustic amplitude transformers: Figure 2A linear taper sonotrode, Figure 2B exponential taper sonotrode; Figure 2C stepped taper sonotrode; and Figure 2D mushroom sonotrode according to US 201 1/0213279; and

FIG. 3 schematically depicts an embodiment of a device according to the teachings herein.

DESCRIPTION OF SOME EMBODIMENTS OF THE INVENTION

The invention, in some embodiments, relates to the treatment of body tissue with energy and more particularly, but not exclusively, to methods and devices for treatment of subcutaneous fat by simultaneously transdermally inducing both ultrasonic transverse vibrations and ultrasonic longitudinal vibrations in subcutaneous tissue, thereby acoustically delivering energy through the skin to treat subcutaneous fat, by applying ultrasonic vibrations to a skin surface

The principles, uses and implementations of the teachings herein may be better understood with reference to the accompanying description and figures. Upon perusal of the description and figures present herein, one skilled in the art is able to implement the invention without undue effort or experimentation. In the figures, like reference numerals refer to like parts throughout.

Before explaining at least one embodiment in detail, it is to be understood that the invention is not necessarily limited in its application to the details of construction and the arrangement of the components and/or methods set forth herein. The invention is capable of other embodiments or of being practiced or carried out in various ways. The phraseology and terminology employed herein are for desciiptive purpose and should not be regarded as limiting.

As discussed above, in US 2011/0213279 are disclosed methods and devices for serially transdermally inducing ultrasonic transverse vibrations and ultrasonic longitudinal vibrations in a volume of subcutaneous tissue thereby acoustically conveying energy through the skin to treat subcutaneous fat. Energy conveyed by the ultrasonic transverse vibrations selectively and effectively disrupts adipocytes in the volume of tissue, while the energy conveyed by the ultrasonic longitudinal vibrations heats subcutaneous tissue, amplifying the efficacy of the ultrasonic transverse vibrations. Although highly effective in the field of body sculpting, a sonotrode such as described in US 201 1/0213279 is sometimes considered less than ideal for some uses because the ultrasonic shear wave vibrations that induce transverse vibrations in the tissue are not applied continuously, because of the added complexity required for generating and switching between two different driving frequencies and because if a user moves the working face over different portions of a treated subjects too quickly, the results of a treatment might be considered less than ideal.

Herein are disclosed methods and devices for treatment of subcutaneous fat by simultaneously transdermally inducing both ultrasonic transverse vibrations and ultrasonic longitudinal vibrations in subcutaneous tissue, thereby acoustically delivering energy through the skin to treat subcutaneous fat, by applying ultrasonic vibrations to a skin surface, for example for reduction of subcutaneous fat.

According to an aspect of some embodiments of the teachings herein, there is provided a device suitable for treating subcutaneous adipose tissue, comprising:

a. an ultrasonic transducer for generation of ultrasonic vibrations having a proximal face and a distal face; and

b. a sonotrode including a narrower proximal stem portion defining a sonotrode axis and a broader distal cap portion

wherein the stem portion has a distal end and bears a proximal face of the sonotrode, the sonotrode acoustically coupled to the distal face of the ultrasonic transducer through the proximal face,

wherein the cap portion has a proximally-facing back side, a distal working face of the sonotrode and a periphery,

wherein the distal end of the stem portion meets the back side of the cap portion, wherein where the distal end of the stem portion meets the back side of the cap portion the cross sectional area of the cap portion perpendicular to the sonotrode axis is not less than 4 times greater than the cross sectional area of the distal end of the stem portion perpendicular to the sonotrode axis; and

wherein the sonotrode is configured to function as an acoustic amplitude transformer for a selected ultrasonic frequency. In Figure 3, an embodiment of a device according to the teachings herein, device 48 is schematically depicted. A device 48 according to the teachings herein was actually constructed, tested and proved to successfully treat subcutaneous fat, see the reproductions of the photomicrographs on the last page of the Appendix. Device 48 includes an ultrasonic transducer 12 and a sonotrode 50.

Ultrasonic transducer 12 has a proximal face 14 and a distal face 18. Ultrasonic transducer 12 is a Langevin-type prestressed (at between 45N/rn to 100 N/rn) transducer that includes a stack of four 6mm diameter disks, configured to produce ultrasonic longitudinal frequencies of between 58 kHz to 60 kHz.

Sonotrode 50 includes a proximal stem portion 52 defining a sonotrode axis 28 and a distal cap portion 54. Sonotrode 50 is a monolithic block of aluminum 6061 (an alloy of aluminum that includes magnesium and silicon as alloying elements) so that stem portion 52 and cap portion 54 are integrally formed.

Stem portion 52 bears a proximal face 56 (also called "input surface") of sonotrode 50 and has a distal end 58. Sonotrode 50 is acoustically coupled to distal face 18 of transducer 12 through proximal face 56 of sonotrode 50. As will be discussed in greater detail below, stem portion 52 is configured substantially as a stepped taper sonotrode, having a circular cross section perpendicular to sonotrode axis 28, where the proximal part is 2.75 cm long and has a 40 mm diameter while the distal part, is 2.15 cm long and has a 20 mm diameter.

Cap portion 54 has a proximally-facing back side 60, a distal working face 62 (also called " contact area" or "output surface") of sonotrode 50 and a periphery 64. Cap portion 54 is substantially a disk have a circular cross section with a 88 mm diameter perpendicular to sonotrode axis 28 and is uniformly 6 mm thick.

Distal end 58 of stem portion 52 meets back side 60 of cap portion 54.

The axial length of sonotrode 50 from proximal face 56 to working face 62 is 55 mm, which is XL/2, XL being the wavelength of ultrasonic longitudinal vibrations of the selected ultrasonic frequency of 57.5 kHz for sonotrode 50.

An ultrasound power supply 34 is functionally associated with transducer 12.

For use, working face 62 of sonotrode 50 of device 48 is acoustically coupled with a skin surface (e.g., by direct contact or by indirect contact through a coupling substance, e.g., a liquid or gel), and an AC oscillating at the selected ultrasonic frequency of sonotrode 50 is supplied from ultrasound power supply 34 to drive ultrasonic transducer 12 to generate ultrasonic longitudinal vibrations. The generated ultrasonic longitudinal vibrations propagate in parallel with axis 28 through sonotrode 50 from proximal face 56 to the working face 62. As briefly discussed and as known in the art, a consequence the configuration of sonotrode 50 to function as an acoustic amplitude transformer for the selected ultrasonic frequency is that the relatively small-amplitude of the longitudinal vibrations at distal face 18 of transducer 12 are transformed to relatively large-amplitude longitudinal vibrations at working face 62 of sonotrode 50.

It has been surprisingly found that when using a device according to the teachings herein, both ultrasonic longitudinal vibrations and ultrasonic transverse vibrations are simultaneously transdermally induced in subcutaneous tissue, both modes of vibrations having sufficient intensity to deliver substantial energy to achieve a desired biological effect, e.g., substantial heating of tissue and substantial disrupting of adipocytes.

A non-trivial goal for simultaneous induction of transverse and longitudinal ultrasonic vibrations in subcutaneous tissue is that the energy delivered by the two modes of vibration be "balanced". It has been surprisingly found that this goal is achieved by a device according to the teachings herein, specifically, that the energy delivered by the two modes of vibration is "balanced", that is to say, during normal use by a body sculpting technician having ordinary skill in the art, the induced ultrasonic transverse vibrations are sufficiently intense to effectively disrupt adipocytes as described in US 2011/0213279 and the simultaneously- induced ultrasonic longitudinal vibrations are sufficiently intense to heat subcutaneous tissue sufficiently to increase the efficacy of the induced ultrasonic transverse vibrations without being so intense as to easily cause potentially catastrophic overheating of bodily tissue (e.g., bums, scarring).

The Inventors' current understanding is that simultaneous transdermal induction of both longitudinal and transverse vibrations in subcutaneous tissue cannot occur through the mechanism described in US 201 1/0213279 (generation of ultrasonic shear wave vibrations in a sonotrode cap to induce ultrasonic transverse vibrations in tissue), but apparently through an entirely different and unexpected mechanism. Without wishing to be held to any one theory, it is currently believed that in a device according to the teachings herein, ultrasonic longitudinal vibrations propagate through the sonotrode to the working face, and when applied to a skin surface acoustically coupled with the working face to induce ultrasonic longitudinal vibrations in the subcutaneous tissue in the same or similar fashion as described in the introduction for known sonotrodes. However, due to the particular characteristics of the cap portion of a sonotrode of a device according to the teachings herein, the ultrasomc longitudinal vibrations generated by the ultrasonic transducer act as a line source perpendicular to the cap portion of the sonotrode that is configured as a plate. As a result Lamb waves form in and propagate through the cap portion, (Strictly speaking, the waves formed are cylindrical plate waves, but as the same characteristic equations apply to both Lamb waves and cylindrical plate waves, for convenience the term Lamb waves and cylindrical plate waves will be used here as synonyms.). The Lamb waves lead to ultrasonic flexural vibrations of the cap portion. By some, not yet completely understood mechanism, when the working face is acoustically coupled with skin, the ultrasonic flexural vibrations in the cap portion transdermally induce substantial ultrasonic transverse vibrations in subcutaneous tissue.

Some embodiments of the teachings herein have one or more advantages compared to the teachings of US 201 /0213279 that, depending on the embodiment, include;

a simpler device that requires provision of only a single driving frequency rather than two driving frequencies that are alternately applied through some switching mechanism; potentially shorter or more effective treatment sessions as a greater proportion of the treatment time is dedicated to inducing adipocyte-disrupting ultrasonic transverse vibrations simultaneously with inducing tissue-heating ultrasonic longitudinal vibrations as opposed to inducing the ultrasonic transverse vibrations only part of the time, alternating with inducing ultrasonic longitudinal vibrations;

potentially shorter or more effective treatment sessions as the ultrasonic transverse vibrations are substantially always induced in or near tissue heated by ultrasonic longitudinal vibrations;

potentially shorter or more effective treatment sessions as some embodiments allow a larger working face that can treat a larger skin surface at any one time compared to the teachings of US 201 1/0213279, and

potentially shorter or more effective treatment sessions as the use of a device having simultaneous induction of ultrasonic transverse and longitudinal vibrations has been demonstrated to be less sensitive to the skill of the user.

Accordingly, in some embodiments, a device according to the teachings herein is configured to simultaneously transdermally induce substantial ultrasonic transverse vibrations and substantial ultrasonic longitudinal vibrations in a volume of subcutaneous tissue through skin with which the working face is acoustically coupled. In some embodiments, the ultrasonic transducer and the sonotrode are configured so that the volume of material is between 7 cm ³ and 56 cm .

In some embodiments, the substantial transdermaliy-induced ultrasonic longitudinal vibrations are sufficient to substantially raise the temperature of the volume of hypodermis, in some embodiments raising the temperature of the volume of tissue by not less than 2°C, in some embodiments by not less than 4°C, and in some embodiments by not less than 6°C. For typical treatments it is typically desirable to raise the temperature in the volume of tissue to between 42°C and 48°C, in some embodiments to between 42°C and 46°C and in some embodiments between 42°C and 45°C.

In some embodiments, the substantial transdermally-induced ultrasonic transverse vibrations are sufficient to initiate a process that leads to irreversible disruption of subcutaneous adipocytes Ultrasonic transducer

As noted above, in some embodiments, a device according to the teachings herein comprises an ultrasonic transducer for the generation of ultrasonic longitudinal vibrations, in Figure 3 ultrasonic transducer 12 where distal face 18 is the radiating surface of ultrasonic transducer 12.

The ultrasonic transducer of a device according to the teachings herein needs to be able to generate sufficiently powerful ultrasonic longitudinal vibrations to allow practice of the teachings herein. If the transducer is not powerful enough, the device will be ineffective while if the transducer is too powerful, a treated subject may be injured.

Accordingly, an ultrasonic transducer of a device according to the teachings herein is an ultrasonic transducer that, during use, is able to have an ultrasonic power output of the selected frequency of a suitable power, in some embodiments an ultrasonic power output of between 40 Watts and 120 Watts and in some embodiments between 45 Watts and 100 Watts. That said, it has been found that it is preferable that the ultrasonic transducer have an ultrasonic power output of the selected frequency of between 50 Watts and 80 Watts, and even of between 60 Watts and 70 Watts.

Any suitable type of ultrasonic transducer may be used in implementing the teachings herein, for example a prestressed Langevin-type ultrasonic transducer. Suitable such transducers are available from a variety of commercial sources. Acoustic reflector

In some embodiments, a device according to the teachings herein further comprises an acoustic reflector functionally associated with the ultrasonic transducer through the proximal face of the ultrasonic transducer. In Figure 3, device 48 comprises an acoustic reflector 16 functionally associated with ultrasonic transducer 12 through proximal face 14. Acoustic reflectors are well-known components in the art commercially available from a variety of sources. Some acoustic reflectors are fluid-filled stainless steel enclosures. In some embodiments such as device 48 depicted in Figure 3, an acoustic reflector is configured as a portion of a cooling assembly, e.g., includes a cooling fluid inlet 66 and a cooling fluid outlet 68,

Ultrasound power supply

As known in the art, an alternating current oscillating at an ultrasonic driving frequency is required to drive an ultrasonic transducer to generate ultrasonic vibrations. Such an alternating current is typically provided by an ultrasound power supply functionally associated with the ultrasonic transducer. Accordingly, in some embodiments a device according to the teachings herein comprises an ultrasound power supply functionally associated with the ultrasonic transducer, configured to provide to the ultrasonic transducer, when activated, an alternating current oscillating at the selected ultrasonic frequency. In Figure 3, device 48 comprises an ultrasound power supply 34 functionally associated with ultrasonic transducer 12

An ultrasound power supply suitable for implementing the teachings herein is configured to provide an alternating current oscillating at the selected ultrasonic frequency having sufficient power so that the ultrasonic transducer has a desired power output as discussed above. Accordingly, in some embodiments, the ultrasound power supply is configured to provide an alternating current oscillating at the selected ultrasonic frequency with a power so that the ultrasonic transducer has a power output of between 40 Watts and 120 Watts, in some embodiments between 45 Watts and 100 Watts, in some embodiments between 50 Watts and 80 Watts, and in some embodiments even between 60 Watts and 70 Watts,

Sonotrode

As depicted in Figure 3, sonotrode 50 includes a proximal stem portion 52 defining an axis 28 and a distal cap portion 54.

Selected ultrasonic frequencv and acoustic amplitude transformer

As noted above, a sonotrode of a device according to the teachings herein is configured to function as an acoustic amplitude transformer for a selected ultrasonic frequency. The selected ultrasonic frequency is the driving frequency of the ultrasonic transducer, the frequency of the ultrasonic longitudinal vibrations generated by the ultrasonic transducer and the frequency of the ultrasonic longitudinal vibrations transdermally induced in subcutaneous tissue.

The selected ultrasonic frequency is any suitable ultrasonic frequency, in some embodiments between 20 kHz and 150 kHz, and even between 20 kHz and 80 kHz. That said, due to limitations in size of the sub-assembly of the device that includes the transducer and the sonotrode (in some embodiments, a hand-piece that is preferably handheld during use in treating a subject), the requirement that the sonotrode be configured as an acoustic amplitude transformer for the selected ultrasonic frequency and the limited number of materials from which the sonotrode can be made (which limits the speed of sound through the sonotrode to certain values), in some preferred embodiments the selected ultrasonic frequency is between 55 kHz and 70 kHz

Length of sonotrode

A person having ordinary skill in the art knows that, in some embodiments, configuration of a sonotrode to function as an acoustic amplitude transformer for a selected ultrasonic frequency includes that the length of the sonotrode from the proximal face of the sonotrode (in Figure 3, 56) to the distal working face (62) along the sonotrode axis (28) is an integral multiple of XL/2, XL being the wavelength of ultrasonic longitudinal vibrations of the selected ultrasonic frequency, which is dependent on the longitudinal speed of sound along the sonotrode axis from the proximal face of the sonotrode to the working face. In Figure 3, the axial length of sonotrode 50 from proximal face 56 to working face 62 is 55 mm, which is XL/2, XL being the wavelength of ultrasonic longitudinal vibrations of the selected ultrasonic frequency of 57.5 kHz for sonotrode 50.

In some embodiments, the length of the sonotrode is set based on the longitudinal speed of sound through the sonotrode at room temperature (25°C).

In some embodiments, the length of the sonotrode is set based on the longitudinal speed of sound through the sonotrode to an expected operating temperature (e.g., 36° - 40°C).

That said, in some embodiments the length of a sonotrode from the proximal face of the sonotrode to the distal working face is not less than 50mm and not more than 300mm. Construction and material of sonotrode

A sonotrode of a device according to the teachings herein is made using any suitable method. That said, to avoid imperfections, seams and interfaces that could potentially compromise the vibration-transmission properties of the sonotrode, in some embodiments, the cap portion of the sonotrode is integrally formed with the rod portion of the sonotrode.

A sonotrode of a device according to the teachings herein is made of any suitable material. Due to need for low acoustic loss, high dynamic fatigue strength, resistance to cavitation erosion and chemical inertness suitable materials include titanium, titanium alloys, aluminum, aluminum alloys, aluminum bronze or stainless steel. Accordingly, in some embodiments the sonotrode is made of a material selected from the group consisting of titanium, titanium alloys, aluminum, aluminum alloys, aluminum bronze and stainless steel.

Of the listed materials, aluminum and aluminum alloys have an acoustic impedance closest to that of skin, so a sonotrode made of aluminum or aluminum alloys has superior acoustic transmission properties to skin. Accordingly, in some preferred embodiments the sonotrode is made of a material selected from the group consisting of aluminum and aluminum alloys.

In some such embodiments, the working face is coated with aluminum oxide, but such embodiments may leave an aluminum oxide residue on treated skin surfaces so are less preferred. In some embodiments, the working face is coated with an acoustic matching layer (e.g., PVDF or PTFE) on an aluminum oxide layer. Such double layer coating improves the acoustic coupling of the working face with tissue. In such embodiments, the aluminum oxide layer is not more than 75 micrometers thick, not more than 50 micrometers thick, not more than 40 micrometers thick, and even between 5 micrometers and 15 micrometers (e.g., 10 micrometers) while the acoustic matching layer applied to the surface of the aluminum oxide layer (e.g., of PVDF or PTFE) is typically 1 to 50 micrometers thick, preferably 5 to 20 micrometers thick.

In some embodiments where a sonotrode is made of aluminum, a hard anodization layer on the working face may give poor results, apparently the hard anodization layer having an acoustic impedance substantially different from that of skin. In contrast, a soft anodization layer on the working face gives acceptable results. Accordingly, in some embodiments the working face of the sonotrode comprises a soft anodization layer, in some embodiments between 5 and 20 micrometers thick, and in some embodiments, between 8 and 12 micrometers thick, e.g., 10 micrometers thick. Stem portion

As noted above and seen in Figure 3, a sonotrode 50 according to the teachings herein includes a narrower proximal stem portion 52 that defines the sonotrode axis 28 and a broader distal cap portion 54. The stem portion 52 bears the proximal face 56 of the sonotrode 50 through which the sonotrode 50 is acoustically coupled to the distal face 18 of the ultrasonic transducer 12. The distal end 58 of the stem portion 52 meets the back side 60 of the cap portion 54.

In preferred embodiments, the stem portion is coaxial with the sonotrode axis. In device 48 depicted in Figure 3, stem portion 52 is coaxial with sonotrode axis 28.

The stem portion has any suitable cross section perpendicular to the sonotrode axis. In preferred embodiments, the stem portion has a circular cross section perpendicular to the sonotrode axis. In device 48 depicted in Figure 3, stem portion 52 has a circular cross section perpendicular to sonotrode axis 28. Taper of stem portion

In some embodiments, configuration of a sonotrode to function as an acoustic amplitude transformer for a selected ultrasonic frequency includes that the stem portion is tapered. The term "taper" and variants thereof are used herein as understood by a person in the art of ultrasonic vibrations, that is to say that the cross sectional area of the proximal face is greater than the cross sectional area of the distal portion, and that the cross sectional area of the stem portion does not increase when moving from the proximal face towards the distal portion. As is known to a person having ordinary skill in the art, the ratio of the cross sectional area of the proximal face (A) to the cross sectional area of the distal end of the stem portion (a) determines the magnitude of amplitude amplification of an acoustic amplitude transformer. The most common taper configurations are as depicted in Figure 2A (linear taper, amplitude amplification is the square root of A/a), Figure 2B (exponential taper, amplitude amplifi cation is square root of A/a), and Figures 2C (stepped taper, amplification is A/a). In device 48 depicted in Figure 3, stem portion 52 has a stepped taper conf guration.

The ratio of the cross sectional area of the proximal face (A) to the cross sectional area of the distal end of the stem portion (a) is any suitable ratio. That said, in some preferred embodiments the ratio is such that the magnitude of amplitude amplification of ultrasonic longitudinal vibrations having the selected ultrasonic frequency is not less than 2,5 X, not less than 3.0 X, not less than 3.5 X and even not less than 4.0 X. In device 48 depicted in Figure 3, the diameter of proximal portion 56 is 40mm twice the diameter of the distal end 58 which is 20mm, so that the magnitude of the amplitude amplification is .0 X.

Size of distal end of stem portion

As discussed immediately above, the main determinant of the cross sectional area of the stem portion (when having a circular cross section as depicted in Figure 3, the diameter) is the configuration of the sonotrode as an acoustic amplitude transformer for the selected ultrasonic frequency.

That said, it is important that the stem portion be sufficiently thick to be robust for use. Accordingly, in some typical embodiments, the cross sectional area of the distal end of the stem portion where the stem portion meets the back side of the cap portion is not less than that of a 5mm diameter circle (20mm ² ), not less than that of a 7mm diameter circle (38mm ² ) and even not less than that of a 9mm diameter circle (64mm ² ). In device 48 depicted in Figure 3, the diameter of distal end 58 of stem portion 52 where stem portion 52 meets back side 60 of cap portion 64 is 20 mm, accordingly having a cross sectional area of 314 mm ² .

It is currently believed that it is preferable that near the cap portion the stem portion be as thin as possible, not only for increased amplitude amplification but also because it is believed that smaller dimensions lead to a more balanced energy distribution between the ultrasonic transverse and longitudinal waves transdermally induced in tissue. Although not wishing to be held to any one theory, it is currently believed that a smaller stem portion allows the cap portion to be "floppier" and therefore more easily subject to ilexural vibrations.

Accordingly, in some typical embodiments, the cross sectional area of the distal end of the stem portion where the stem portion meets the back side of the cap portion is not more than that of a 25 mm diameter circle (491 mm ² ), not more than that of a 23 mm diameter circle (415 mm ² ) and even not more than that of a 21 mm diameter circle (346 mm ² ).

Meeting of stem portion and cap portion

As noted above, the stem portion meets the back side of the cap portion.

In some embodiments, the distal end of the stem portion meets the back side of the cap portion at a right angle, for example, in device 48 depicted in Figure 3.

In some embodiments, the device further comprises a fillet (an inwardly curved meeting) where the distal end of the stem portion meets the back side of the cap portion, mechanically strengthening the meeting. In some embodiments, the device further comprises a chamfer (in a cross section that includes the sonotrode axis, a straight line segment that connects the shaft of the stem portion with the back side of the cap portion,) where the distal end of the stem portion meets the back side of the cap portion, mechanically strengthening the meeting.

Cap portion

As noted above and seen in Figure 3, in some embodiments cap portion 54 has a proximally-facing back side 60, a distal working face 62 of sonotrode 50 and a periphery 64, wherein distal end 58 of stem portion 52 meets back side 60 of cap portion 54, and wherein where distal end 28 of stem portion 52 meets back side 60 of cap portion 54, the cross sectional area of cap portion 54 perpendicular to sonotrode axis 28 is not less than 4 times greater than the cross sectional area of distal end 28 of stem portion 52 perpendicular to the sonotrode axis 28.

In preferred embodiments, the cap portion is coaxial with the sonotrode axis. In device 48 depicted in Figure 3, cap portion 54 is coaxial with sonotrode axis 28.

The cap portion has any suitable cross section perpendicular to the sonotrode axis. In preferred embodiments, the cap portion has a circular cross section perpendicular to the sonotrode axis. In device 48 depicted in Figure 3, cap portion 54 has a circular cross section perpendicular to sonotrode axis 28.

Working face and back side

The working face has any suitable shape perpendicular to the sonotrode axis. In preferred embodiments, the working face is circular. In device 48 depicted in Figure 3, working face 62 has a circular shape perpendicular to sonotrode axis 28.

In some embodiments, not less than 70% of the surface area of the working face is planar and perpendicular to the sonotrode axis. In some such embodiments, not less than 80%, not less than 90% and even not less than 95% of the surface area of the working face is planar and perpendicular to the sonotrode axis. In device 48 depicted in Figure 3, more than 95% of the surface area of working area 62 is planar and perpendicular to sonotrode axis 28.

In some embodiments, not less than 70% of the surface area of the back side is planar and perpendicular to the sonotrode axis. In some such embodiments, not less than 80%, not less than 90% and even not less than 95% of the surface area of the back side is planar and perpendicular to the sonotrode axis. In device 48 depicted in Figure 3, more than 95% of the surface area of back side 60 is planar and perpendicular to sonotrode axis 28. In some preferred embodiments, not less than 70% of the surface area of both the working face and of the back side are planar and mutually parallel. In some such embodiments, not less than 80%, not less than 90% and even not less than 95% of the surface area of both the working face and of the back side are planar mutually parallel. In some preferred embodiments, the planar and mutually parallel portions of the working face and of the back side are also perpendicular to the sonotrode axis. Without wishing to be held to any one theory, it is currently believed that when a substantial portion of both the working face and the back side are planar and mutually parallel, the cap portion more easily allows propagation of Lamb Waves, and the cap portion is "floppier" and therefore more easily subject to flexural vibrations. In device 48 depicted in Figure 3, more than 95% of the surface area of both working face 62 and back side 60 are planar, mutually parallel and perpendicular to sonotrode axis 28.

Smoothness of working face and back side

As discussed hereinabove in the introduction, the teachings of US 201 1/0213279 are preferably implemented when the working face of a sonotrode includes transverse-wave transferring ridges.

In contrast, it has been found that when implementing the teachings herein, it is preferable, and in some embodiments critical, that both the working face and the back side be smooth and featureless. It was found that 200 micrometer high concentric rings on an otherwise smooth working face were relatively ineffective in inducing Without wishing to be held to any one theory, it is currently believed that surface variations disrupt the formation and/or propagation of Lamb Waves and/or flexural vibrations.

Accordingly, in some embodiments, the planar part of the working face of the sonotrode is smooth.

In some embodiments, the planar part of the working face of the sonotrode is devoid of surface variations greater than 200 micrometers, 100 micrometers, 50 micrometers and even 20 micrometers.

In som e embodiments, the planar part of the back side of the cap portion is smooth. In some embodiments, the planar part of the back side of the cap is devoid of surface variations greater than 200 micrometers, 100 micrometers, 50 micrometers and even 20 micrometers.

In device 48 depicted in Figure 3, the planar parts of both working face 62 and back side 60 are smooth and have no surface variations greater than 20 micrometers. Thickness of cap portion

As used herein, the thickness of the cap portion is defined as the longitudinal dimension along the sonotrode axis. In general, it is desirable that the cap portion be as thin as possible, allowing the cap portion to be "floppier". At the same time, it is necessary that the cap portion be thick enough to be sufficiently robust.

In some embodiments, the thickness of the cap portion is less than or equal to XL/10, XL being the wavelength of ultrasonic longitudinal vibrations of the selected ultrasonic frequency.

In some embodiments, the cap portion is not less than 2 mm, not less than 3 mm, not less than 4mm and even not less than 5mm thick.

In some embodiments, the cap portion is not more than 10 mm, not more than 9 mm, not more than 8mm and even not more than 7mm thick.

In device 48 depicted in Figure 3, cap portion 54 is 6 mm thick. Periphery

The periphery of the cap portion of a sonotrode of a device according to the teachings herein is any suitable periphery. That said, in some embodiments the periphery, when viewed from the side is a straight line. That said, in some embodiments the periphery, when viewed from the side is a straight line parallel to the sonotrode axis. In device 48 depicted in Figure 3, when viewed from the side, periphery 64 of ring portion is a straight line parallel to sonotrode axis 28, Without wishing to be held to any one theory, it is currently believed that when the periphery is a straight line, especially a straight line parallel to the sonotrode axis, Lamb Waves more easily propagate in the cap portion.

The edges of the periphery where the periphery meets either the back side or the working face are of any suitable configuration.

In some embodiments, an edge of where the periphery of the cap portion meets the back side, the working face or both the back side and the working face is a right angle, that is to say the back side / working face intersect the periphery at a right angle. For example, in device 48 depicted in Figure 3, the edges where periphery 64 meets back side 60 are right angles.

A disadvantage of right angle edges, especially of the working face, is that these may- scrape or be otherwise uncomfortable to a person. Accordingly, in some embodiments, an edge of where the periphery of the cap portion meets the back side, the working face or both the back side and the working face is not a right angle (e.g., is beveled or rounded). For example, in device 48 depicted in Figure 3, the edges where periphery 64 meets working face 62 are rounded.

Cylindrical cap portion

As is clear to a person having ordinary skill in the art, in some preferred embodiments such as depicted in Figure 3, where not less than 90% of both the working face and the back side of the cap portion are planar and perpendicular to the sonotrode axis, and where the periphery of the cap portion, when viewed from the side is a straight line parallel to the sonotrode axis, a side cross section of the cap portion is a rectangle and the cap portion is substantially a right cylinder (excluding the edges, that may be rounded or beveled). It is currently believed that such embodiments are preferred for providing the most balanced transdermal induction of ultrasonic transverse and longitudinal waves in subcutaneous tissue.

Size of cap portion

The size of the cap portion (in terms of cross sectional area perpendicular to the sonotrode axis, or equivalently, the diameter of a circular cap portion) is any suitable size.

It is currently believed that it advantageous that the cap portion and working face be as large as possible as this allows the amplitude of flexural vibrations to be as large as possible and, all other things being equal, a larger cap portion is "floppier". On the other hand, a large cap portion with a working face that is too large to make adequate contact with a skin surface to be treated is presumably unsuitable for efficiently inducing transverse ultrasonic vibrations in subcutaneous tissue.

Accordingly, in some embodiments the area of a cross section perpendicular to the sonotrode axis of the cap portion through the longitudinal center of the cap portion (indicated by line 70 in Figure 3) is not more than that of a 150 mm diameter circle (17700 mm ² ), not more than that of a 130 mm diameter circle ( 13300 mm ² ) and even not more than that of a 100 mm diameter circle (7850 mm ² ). In device 48 depicted in Figure 3, the diameter of cap portion 54 is 88 mm, so that the area of a cross section perpendicular to sonotrode axis 28 of cap porti on 54 through the longitudinal center 70 of cap porti on 54 is 6080 mm .

As noted above, in some preferred embodiments, where the distal end (58 in Figure 3) of the stem portion (52) meets the back side (60) of the cap portion (54) the cross sectional area of the cap portion (54) perpendicular to the axis is not less than 4 times greater than the cross sectional area of the distal end (58) of the stem portion (52) perpendicular to the sonotrode axis (28). Without wishing to be held to any one theory, it is currently believed that a smaller cap portion will be insufficiently "floppy" for efficient flexurai vibration. In some embodiments, the cross sectional area of the cap portion is even larger, being not less than 6 times, not less than 8 times, not less than 10 times, not less than 12 times, not less than 14 times and even not less than 16 times greater than the cross sectional area of the distal end of the stem portion. In device 48 depicted in Figure 3, the diameter of cap portion 54 is 88 mm and the diameter of distal end 58 of stem portion 52 is 20 mm, so that where distal end 58 of stem portion 52 meets back side 60 of cap portion 54 the cross sectional area of cap portion 54 perpendicular to the sonotrode axis 28 is 19.4 times the cross sectional area of distal end 58.

Cooling assembly

As is known to a person having ordinary skill in the art, during operation of an ultrasonic transducer an associated sonotrode may be heated to a temperature that makes skin contact with the working face of the sonotrode uncomfortable or even harmful. Additionally, heating of subcutaneous tissue may lead to excessive heating of the skin.

To reduce the incidence of such undesirable effects when the device is used, in some embodiments the device is configured to actively cool at least a portion of the working face. To this end, in some embodiments, a device further comprises a cooling assembly configured, when activated, to cool at least a portion of the working face, directly or indirectly (e.g., by cooling a distal part of the transducer or the sonotrode which is in thermal communication with the working face. In some embodiments, a device further comprises cooling-fluid channels in thermal communication with the working face, e.g., the cooling-fluid channels are in thermal communication with the sonotrode.

During use of the device, such cooling-fluid channels can be functionally associated with an appropriately configured cooling device or cooling assembly that drives a cooling fluid through the cooling-fluid channels, thereby cooling the working face. In some embodiments, the device further comprises a cooling assembly functionally associated with the cooling-fluid channels configured, when activated, to drive a cooling fluid through the cooling-fluid channels, thereby cooling the working face.

Construction and use of such a cooling assembly is described in US 9,545,529 of the Applicant, which is included by reference as if fully set forth herein. Method of treatment, using the device

A device according to the teachings herein may be used in implementing a method of tran sdermally treating subcutaneous fat according to the teachings herein. According to an aspect of some embodiments of the teachings herein, there is provided a method of transdermally treating subcutaneous fat comprising:

i. providing a device according to the teachings herein, wherein the ultrasonic transducer is functionally associated with an ultrasound power supply,

ii. for a treatment event having a duration, maintaining the working face acoustically coupled with a skin surface while the ultrasound power supply is activated to supply a driving current having the selected ultrasonic frequency to the ultrasonic transducer,

thereby simultaneously transdermally inducing both:

ultrasonic longitudinal vibrations (perpendicular to the skin surface) sufficient to convey sufficient energy to substantially heat subcutaneous tissue; and

ultrasonic transverse vibrations (parallel to the skin surface) in subcutaneous tissue to convey sufficient energy to disrupt adipocytes in the subcutaneous tissue.

Typically, the method is non-invasive, that is to say the skin surface remains intact, and is not punctured or otherwise penetrated. In some embodiments, the method is a nonsurgical method, performed without breaking the skin. Embodiments of the method are performed by any suitable person, including medical personnel but typically aesthetic technicians such as beauticians.

In some embodiments, the simultaneous inducing of ultrasonic longitudinal vibrations and ultrasonic transverse vibrations initiates a process leading to a reduction of the amount of subcutaneous fat in proximity to the skin surface.

In some embodiments, the ultrasonic longitudinal vibrations convey sufficient energy to raise the temperature of the subcutaneous tissue, as discussed above with reference to the device of the teachings herein.

In some embodiments, a treatment session comprises one or more treatment events. During a treatment session (typically between 15 minutes and 60 minutes), an operator uses the device to tran sdermally treating subcutaneous fat of a subject. During each treatment event, the operator typically slides the working face over an area of the skin of the subject, ensuring homogeneous heating of the subcutaneous tissue in proximity of the area of the skin by the action of the induced longitudinal vibrations.

A single treatment event is of any suitable duration. In some embodiments, a single treatment event has a duration of not less than 30 seconds. In some embodiments, the ultrasound power supply is continuously activated to supply the driving current throughout the treatment event .

In some embodiments, the ultrasound power supply is intermittently activated during the treatment event.

In some embodiments, during the treatment event, the driving current having the selected frequency is the only driving current supplied to the ultrasonic transducer.

In some embodiments, the working face is directly acoustically coupled with a skin surface.

In some embodiments, the working face is indirectly acoustically coupled with a skin surface through a fluid (e.g., petroleum jelly, or an impedance-matching material such as an ultrasound gel (e.g., Graham-Field Ultrasound Gel, GF Health Products Inc., Atlanta, Georgia, USA),

In some embodiments, during the treatment event, maintaining a temperature of the working face at not more than 42°C. In some such embodiments, maintaining the temperature is performed by operating a cooling assembly that is part of the device.

In some embodiments a portion of the skin surface of the subject is actively cooled.

In some embodiments, the method further comprises, during a treatment event, cooling a portion of a skin surface proximal to the working face, in some embodiments, thereby effecting cooling of a portion of a skin surface proximal to the working face. In some such embodiments, the working face is cooled, for example by the passage of a cooling fluid in proximity thereto (for example near or through the sonotrode), to effect cooling of the portion of the skin surface.

It is appreciated that certain features of the invention, which are, for clarity, described in the context of separate embodiments, may also be provided in combination in a single embodiment. Conversely, various features of the invention, which are, for brevity, described in the context of a single embodiment, may also be provided separately or in any suitable subcombination or as suitable in any other described embodiment of the invention. Certain features described in the context of various embodiments are not to be considered essential features of those embodiments, unless the embodiment is inoperative without those elements.

Although the invention has been described in conjunction with specific embodiments thereof, it is evident that many alternatives, modifications and variations will be apparent to those skilled in the art. Accordingly, it is intended to embrace all such alternatives, modifications and variations that fall within the scope of the appended claims. Citation or identification of any reference in this application shall not be construed as an admission that such reference is available as prior art to the invention.

Section headings are used herein to ease understanding of the specification and should not be construed as necessarily limiting.

Appendix page 1 of 11

Description:

Sandwich type Lanoevin transducer (pre-stressed? consists oi four 6 msi piezoceraisic rings, Tbe frequency of operati in between 58--69 kHs Fig.l

The Rings are pxe-strss«sd with a torque 5: ny;¾ to 100 /ss.

Tbe piezoceraKric ring csn be simulated, by polarized capacitor iauch as electrolyti capacitors) , The transducer ia four capacitors; connected in parallel Fiq<2)

Appendix page 2 of 11

3, The- DC-current ons med fey t¾e transducer is u to 1500 ft. m ¾iiii is. The DC su plyi g: voltage SS VDC; therefore the input power of the resonant systeiu is 130 S,

Efficiency of conversion of IW ower to acoustic power is approximately ¾0"C50% therefore the ultrasound power la 60- 70 W,

the contact area of the sonotrode is 51 emr and the acoustic power flux ^intensity} is 1,1 - 1,2 ¾/ car ² .

4. Usually we use a resonan principle for excitation of the ultrasound transducer., which m ans at the chosen frequency the resonant inductor {L) is connected in series with capacitance (C) of the transducer .

The capacitance of the transducer is equal to 5,68 nf

{me surements at 100 kHz) .

Therefore, the resonant inductor at optimal frequency (£) 50,2 kHz is derived from resonant conditions

XL - Xc 2nfL-i/2i:fC

whe e :

XL - inductive reactance (Ohms) and

Xc ·· capaoitive reactance (Ohms)

The resonant inductor is equal to L~ 1.3 mH approximately

S.i We physio:aily divid the inducto into two parts:

11- Hon-tunable Inductor located in the high frequency (BF) generator and

12- Tunable inductor, located in the connector block of the handpiece. This inductor it: should be tuned for the individual ult asound transduce ,

6, The <KF>~qeners or operates ss s class E amplifier "Th

idea behind class E is to reduce or eliminate the effects the various capacitance within the MGSFET have on

efficiency and operation at high fregueneiesu The major operational condition is that the MOSFET is only switched (turned on) when there is no voltage across the device . This eliminates switching losses, a major loss component of most <HF> amplifiers'' ~™ source;

ht to ; / /u ^' UV: , c laaseradio , cotp theor y . hte Appendix page 3 of 11

3

7, The resonant circuitry described above is a low«o ic load for the class E m lifier,

8, The main tash of th circuitry tuning is an . ohiuyvesent of a coincidence of electrical and acoustic resonance. The tuning of this circuit includes a preliminary searching of the operative electrical frequency that produces a resonant acoustic wave. The specific geometry of the sonotrode and tuning provides this coincidence _t

9, The geometry of the sonotrode is showed by Figure 3.

The most important dimensions are the following; L3- thickness of the applicator

L3 should be much less than 3/ 2 (halt-wavelength 5 of the sound in sonotrode iuaterial aiu dnusa 061 .96 -99 % Al, 1 % Mg) , L3 should be thin enough to produce efficient flexure _* . In one eisbodi ent of the Invention, L3-c~ λ/10, L 3 can be thicker at higher powe . e sound velocity is 0^6300 /sec (approx.) Appendix page 4 of 11

4

Therefore the half-wavelength at resonant frequency will be- λ/2- o/Fw

wher F¾™ is operating frequency 1 . tkU: for example here Λ/2 ------ 11/2^ 5.5 cm

In our case w chose L3- 0-6 osn the is 0-1 of λ,/2 approxim tely

Sonotrode length L2 is equal to λ/2 (namely 5.5 era) . Hence, the maxinvarrs of a plitude of ultrasonic oscillations is at input surface Si of the sonotrode, and, consequen ly; a i Kiiauiu of the amplitude locates at the output surface S3 of the sonotroue is as well.

Let us analyse the am litude {stress} trans orisation through the length of the sosotrode, Figure 4 b low.

Appendix page 5 of 11

If am li u e in the surface SI is equal to A1 , on the surface S2 m li ude' A2 reaches 0 {maxim l stress) , F oi the surface £2 along the axis x the amplitude started to increase ap to vaive ¾3 defined by formula magnification factor (a)

a - D1/D2 {Fig.3) , in oar case ∞ 8 ,8 csn/2 cm ^■ *? 4,

Therefore, it the amplitude at the surface SI is 5 ym at the central area of surface S3 it achieves 22 u;a.

The central area of the applied surface S3 gets the strong vibration with high amplitude. The disc part of sonotrode is thin and flexible. It st rts the vibration froin the central area, generating plate {guided or Lamb) waves, which propagate for;:- the central part to the edge of the plate, therefore in the direction orthogonal to the initial wave propagation.

The type of this ave is symmet ic plate wave.

Citation:

"Plate waves are similar to surface waves except they can only be generated in materials a few wavelengths thick. Lamb waves are complex vibrational waves thai propagate parallel to the test surface throughout the thickness of the material. Propagation of Lamb waves depends on the density and the elastic material properties of a component They are also influenced a great deal by the test frequency and material thickness. Lamb waves are generated at an incident angle in which the parallel component of the velocity of the wave In the source is equal to the velocity of the wave In the test material

With Lamb waves, a number of modes of particle vibration are possible, but the two most common are symmetrical and asymmetrical The complex motion of the particles is similar to the elliptical orbits for surface

waves. Symmetrical Lamb waves move in a symmetrical fashion about the median plane of the plate. This is sometimes called the extensions! mode because the wave Is "stretching and compressing" the pfate in the wave moiion direction. Wave motion in the symmetrical mode is most efficiently produced when the exciting force Is parallel to the plate. The asymmetrical Lamb wave mode is often called the iiexurai mode" because a large portion of the motion moves in a normal direction to the plate, and a little motion Appendix page 6 of 11

occurs In the direction parallel to the plate. in this mode, the body of the piate bends as the two surfaces move in the same direction".

s arce : ht tps i //www„ nde- ei, orq/EdA.;cat ibnResources/Co!T^ nityCoi ieqe/Uitrasonics/Phys

The planar standing wave forms the distribution of the

ultrasound energy through the diameter D showed by Fig, 5:

Sistssfeas- (»>

The central are generating longitudinal portion of ultrasound uave is moat energetic. The edg area produces purs planar wave. The a r ximate path of the front of ultrasound wave is also shoved by Fig, 5 above and fig.6 below Appendix page 7 of 11

7

X wo ld like to emind a aain condition of planar (guided wav generation, th thickness of the plate should fee less than wavelength in the plats fasteriai (Fig below) sie Requirements

Fig, 6 Interaction of planar wave with biological tissue Appendix page 8 of 11

The picture above (Wavesoenda LLC) discusses a difference betwears shear (SH) nd Plate CL&ssb) waves .

The plate wav is complex of frexaral .and com ressions! motion of the particles of the plate material, therefore there are tee components of the wa e : Compressions! that coincides with the wa e propagation direction and Flexarai thst is orthogcaal to the ; e propagation and to the plate surface. The flexarai component of the wave is intensively absorbed by biological tissue. The compressions! can propagate deep.

The angle® of wave emission into biological tissue is different (see Fig, 9 beLow)

The cempresaional component is emitted practically in parallel with, applied surface of sonotrode bat fiexurai component is normal to this surface.

The penetration depth of this ultrasound is 11··- i 1 n . the compx ssionai component is also reflected from borders between different layers (der is/hypodermis and hypodetaiis/ muscles. Appendix page 9 of 11

Appendix page 10 of 11

Graph represents acoustic pressure as function of 3-D raster scan at different depth..

Testing performed with inim needle hydrophone.

Appendix page 1 1 of 11

Histology