Application No. 15/396,073
`Reply to Office Action dated 03/24/2017
`
`Attorney Dkt. No. 066964-8034.U800
`
`Amendments to the Specification:
`
`Please amend the Specification as follows:
`
`Please amend [0016] as follows:
`
`[0016]
`
`Figures 4a and 4b illustrate a combined treatment with optical waves
`
`generating device powered by magnetic field generated by magnetic field generating
`
`device.
`
`LIST OF REFERENCE NUMBERS
`
`1
`
`2
`
`3
`
`4
`
`5
`
`6
`
`7
`
`8
`
`9
`
`10
`
`11
`
`12
`
`13
`
`14
`
`15
`
`16
`
`optical treatment device
`
`energy source
`
`hardware panel for optical treatment
`
`optical waves generating device
`
`optical treatment applicator
`
`magnetic treatment device
`
`energy source
`
`hardware panel for magnetic treatment
`
`magnetic field generating device
`
`magnetic treatment applicator
`
`combined treatment device
`
`energy source
`
`hardware panel for optical treatment
`
`optical waves generating device
`
`optical treatment applicator
`
`hardware panel for magnetic treatment
`
`66964-8034.US00/134971137.1
`
`

`

`Application No. 15/396,073
`Reply to Office Action dated 03/24/2017
`
`Attorney Dkt. N0. 066964-8034.USOO
`
`17
`
`18
`
`magnetic field generating device
`
`magnetic treatment applicator
`
`19
`
`combined treatment device
`
`2O
`
`21
`
`22
`
`23
`
`24
`
`25
`
`energy source
`
`hardware panel
`
`optical waves generating device
`
`optical treatment applicator
`
`magnetic field generating device
`
`magnetic treatment applicator
`
`26
`
`combined treatment device
`
`27
`
`28
`
`29
`
`3O
`
`31
`
`32
`
`energy source
`
`hardware panel for optical treatment
`
`optical waves generating device
`
`applicator
`
`hardware panel for magnetic treatment
`
`magnetic field generating device
`
`33
`
`combined treatment device
`
`34
`
`35
`
`36
`
`37
`
`38
`
`39
`
`energy source
`
`hardware panel
`
`optical waves generating device
`
`magnetic field generating device
`
`applicator
`
`magnetic field generating device
`
`66964-8034.US00/134971137.1
`
`

`

`Application No. 15/396,073
`Reply to Office Action dated 03/24/2017
`
`Attorney Dkt. No. 066964-8034.USOO
`
`40
`
`conductor loop
`
`41
`
`42
`
`light source
`
`coil
`
`43
`
`circuit wires
`
`44
`
`45
`
`46
`
`47
`
`48
`
`49
`
`50
`
`51
`
`fastening point
`
`blower
`
`applicator
`
`arrows
`
`casing
`
`outlet
`
`connecting tube
`
`conduit
`
`52
`
`switch
`
`53
`
`coil
`
`54
`
`55
`
`56
`
`57
`
`58
`
`59
`
`energy storage device
`
`ener
`
`source
`
`protecting circuitry
`
`coil
`
`energy storage device
`
`switch
`
`60
`
`ener
`
`source
`
`66964-8034.US00/134971137.1
`
`

`

`Application No. 15/396,073
`Reply to Office Action dated 03/24/2017
`
`Attorney Dkt. No. 066964-8034.U800
`
`At page 5, after paragraph 0016 (as amended above) and before “LIST OF
`
`REFERENCE NUMBERS”, please add new paragraphs 0016.1- 0016.5 as follows:
`
`[0016.1]
`
`Figure 5 is a cross section of view of a coil winding.
`
`[0016.2]
`
`Figure 6 is an illustrative embodiment of cross-section of the magnetic
`
`applicator.
`
`[0016.3]
`
`Figure 7 is an illustrative embodiment of a casing of
`
`the magnetic
`
`applicator.
`
`[0016.4]
`
`Figure 8A and 8B illustrate circuit for providing high power impulses to a
`
`stimulating coil.
`
`[0016.5]
`
`Figure 9 is a graph showing voltage drop in the energy storage device.
`
`Please add new paragraphs 0037.1 to 0037. 21 as follows:
`
`[0037.1]
`
`The methods recites above may be enabled by a device described in
`
`Figures 5 to 9.
`
`[0037.2]
`
`Fig. 5 illustrates a cross section of winding of a coil for a magnetic
`
`stimulation device. The coil may be constructed from litz-wire, wherein each wire is
`
`insulated separately. Each individual conductor is coated with non-conductive material
`
`so the coil constitutes multiple insulated wires. Unlike existing magnetic coil conductors,
`
`the present coil
`
`is not made of bare wire e.g.
`
`litz-wire without insulation, or conductive
`
`tapes, conductive strips, or copper pipe with hollow inductors. The insulation of wires
`
`separately is a substantial improvement, since this leads to a significant reduction of the
`
`induced eddy currents. Power loss due to eddy currents, per single wire, is described by
`
`Equation 1 below. The small diameter wires of the present coil significantly reduce self-
`
`66964-8034.US00/134971137.1
`
`10
`
`

`

`Application No. 15/396,073
`Reply to Office Action dated 03/24/2017
`
`Attorney Dkt. No. 066964-8034.USOO
`
`heating of the coil and therefore increases efficiency of the present magnetic stimulation
`
`device.
`
`72-2 'B2 'd2 “f2
`P =P—,
`6"“ka
`EDDY
`
`E . 1
`q
`
`[0037.3]
`
`where:
`
`PEDDy is power loss per unit mass (W-kg'1); Bp is the peak of
`
`magnetic field (T); f is frequency (Hz); d is the thickness of the sheet or diameter of the
`
`wire (m); k is constant equal to 1 for a thin sheet and 2 for a thin wire; p is the resistivity
`
`of material (Q-m); D is the density of material (kg-m3).
`
`[0037.4]
`
`The individual
`
`insulation of each wire reduces eddy currents. The
`
`individually insulated wires may be wound either one by one or
`
`in a bundle of
`
`individually insulated wires so as to form a coil, which will serve as a magnetic field
`
`generator. The coil provides an improvement in the efficiency of energy transfer in the
`
`LC resonant circuit and also reduces or eliminates unwanted thermal effects.
`
`[0037.5]
`
`The coil may have a planar coil shape where the individually insulated
`
`wires may have cross-section wires with conductor diameter less than 3 mm even more
`
`preferably less than 0.5 mm and most preferably less than 0.05 mm. The wires are
`
`preferably made of materials with higher density and higher resistivity e.g. gold,
`
`platinum or copper. The diameters of the single wires should be minimal. On the other
`
`hand the total diameter should be maximal because of inverse proportion between the
`
`cross-section of all wires forming the coil and the electrical resistance. Therefore the
`
`ohmic part of the heat is then lower. Eq. 2 describes power loss of the coil:
`
`66964-8034.US00/134971137.1
`
`
`
`11
`
`

`

`Application No. 15/396,073
`Reply to Office Action dated 03/24/2017
`
`Attorney Dkt. No. 066964-8034.USOO
`
`[0037.6]
`
`Where:
`
`PR is the power loss heat dissipation (W);,o is the resistance
`
`(Q-m); /is the length of wire (m); S is the surface area (m2);
`
`/ is the current (A) and m is
`
`1 kg of wire material.
`
`[0037.7]
`
`Total power loss is (Eq.3):
`
`[0037.8]
`
`Where: PTOT is
`
`the total power
`
`losses (W-kg'1); PEDDy is
`
`the power
`
`PTOTZPEDDY+PR’
`
`Eq'3
`
`dissipation of eddy currents (W-kg'1); PR is the power loss heat dissipation (W-kg'1).
`
`[0037.9]
`
`Dynamic forces produced by current pulses passing through the wires of
`
`the coil cause vibrations and unwanted noise. The individual insulated wires of the coil
`
`may be impregnated under pressure so as to eliminate air bubbles between the
`
`individual insulated wires. The space between wires can be filled with suitable material
`
`which causes unification, preservation and electric insulation of the system. Suitable
`
`rigid impregnation materials like resin, and elastic materials like PTE can be also used.
`
`With the coil provided as a solid mass,
`
`the vibrations and resonance caused by
`
`movements of
`
`the individual
`
`insulated wires are suppressed. Therefore noise is
`
`reduced.
`
`[0037.10]
`
`The coil may be attached to the case of the applicator, such as a hand
`
`held applicator of the magnetic stimulation device; build-in applicator in e.g. chair, bed;
`
`or stand-alone applicator e.g. on mechanical fixture. The attachment may be provided
`
`by an elastic material e.g., silicone, gum; or other flexible manner. Connection with the
`
`coil of the applicator’s case can be ensured by several points. The several fastening
`
`points ensure the connection of the coil to the casing by flexible material so that the
`
`main part of the coil and the main part of the casing of applicator are spaced apart. The
`
`66964-8034.US00/134971137.1
`
`12
`
`

`

`Application No. 15/396,073
`Reply to Office Action dated 03/24/2017
`
`Attorney Dkt. No. 066964-8034.U800
`
`spacing should be at least 0.1 mm so that air can easily flow. The gap between the coil
`
`and the casing can be used either for spontaneous or controlled cooling. The coil may
`
`optionally be connected to the case of the applicator by only one fastening point. The
`
`fastening points eliminate vibrations of wires which could be transferred to housing of
`
`the applicator and therefore reduce noise of the magnetic stimulation device.
`
`[0037.11]
`
`Fig. 6 is a cross-section of the magnetic applicator which allows better
`
`flow on the lower and upper sides of the coil and thus more efficient heat dissipation.
`
`The magnetic stimulation device includes a coil 42,
`
`the circuit wires 43 and the
`
`fastening points 44 for connection of the coil to the casing of the applicator (not shown).
`
`The fastening points 44 are preferably made of flexible material however the rigid
`
`material may be used as well. The fastening points 44 may be located on the outer
`
`circumferential side of the coil. However, alternatively it
`
`is possible to put
`
`these
`
`fastening points to a lower or upper side of the coil.
`
`[0037.12]
`
`The fastening points 44 connect the coil to the case of the applicator in at
`
`least one point. The fastening points 44 maintain the coil and the main part of the case
`
`of the applicator spaced apart so that fluid (which may be air or any liquid) can flow
`
`between them. At least one blower 45 can be placed around the circumference of the
`
`coil, or perpendicular to the coil. The blower can be any known kind of device for
`
`directing the fluid e.g. outer air directed into the case of
`
`the applicator. This
`
`arrangement of the blower allows air to bypass the coil from upper and lower (patient’s)
`
`sides.
`
`In still another embodiment the outer air can be cooled before directing into the
`
`case. The blower can have an inlet placed around the circumference of the coil for
`
`injecting air, to remove heat from the coil. A connecting tube (not shown) can ensure
`
`66964-8034.US00/134971137.1
`
`13
`
`

`

`Application No. 15/396,073
`Reply to Office Action dated 03/24/2017
`
`Attorney Dkt. No. 066964-8034.U800
`
`connection of the applicator 46 with the energy source and/or control unit of magnetic
`
`stimulation device. The connecting tube may also contain a conduit of the fluid.
`
`[0037.13]
`
`The arrows 47 indicate the air flow through the applicator 46. This
`
`arrangement of the blower allows the air to bypass the coil from upper and lower
`
`(patient’s) side. Outlet may be preferably placed on upper side of the casing. By placing
`
`the blower around the circumference of the coil instead of on the top/below the coil, the
`
`blower 45 does not interfere with the magnetic flux peak and therefore its lifespan and
`
`reliability is increased.
`
`[0037.14]
`
`Fig. 7 is an illustrative embodiment of a casing of the magnetic applicator.
`
`The overview drawing contains casing itself 48, which might contain an outlet 49
`
`preferably placed on upper side of the casing 48. A connecting tube 50 may not only
`
`ensure connection of the applicator with the energy source and/or control unit of
`
`magnetic stimulation device, but also connection to a source of the fluid; however the
`
`conduit of the fluid 51 may also be connected separately.
`
`[0037.15]
`
`Fig. 8A and Fig. 8B illustrate circuits for providing high power pulses to the
`
`stimulating coil. Fig. 8A shows a circuit for providing high power magnetic pulses. Fig.
`
`8B shows a circuit for providing high power pulses.
`
`[0037.16]
`
`The state of art magnetic stimulation device achieves magnetic flux
`
`density of a few tenths to several ones of Tesla. To achieve this level of magnetic flux
`
`density, the energy source used generates sufficient voltage. This voltage can reach
`
`thousands of volts.
`
`In Fig. 8A the circuits for providing high power pulses to the
`
`stimulating coil contain a series connection to the switch 52 and the coil 53. The switch
`
`52 and the coil 53 together are connected in parallel with an energy storage device 54.
`
`66964-8034.US00/134971137.1
`
`14
`
`

`

`Application No. 15/396,073
`Reply to Office Action dated 03/24/2017
`
`Attorney Dkt. No. 066964-8034.U800
`
`The energy storage device 54 is charged by the energy source 55 and the energy
`
`storage device 54 then discharges through the switching device 52 to the coil 53.
`
`[0037.17]
`
`During second half-period of LC resonance,
`
`the polarity on the energy
`
`storage device 54 is reversed in comparison with the energy source 55.
`
`In this second
`
`half-period, there is a conflict between energy source 55, where voltage on positive and
`
`negative terminals is typically thousands of Volts. The energy storage device 54 is also
`
`charged to the positive and negative voltage generally to thousands of Volts. As a
`
`result, there is in the circuit, consequently, twice the voltage of the energy source 55.
`
`Hence the energy source 55 and all parts connected in the circuit are designed for a
`
`high voltage load. Therefore, the protective resistors and/or protection circuitry 56 must
`
`be placed between energy source 55 and energy storage device 54. Disadvantage of
`
`state of art solution is
`
`large amount of energy transformed to undesired heat
`
`in
`
`protective resistors and/or protection circuitry 56.
`
`[0037.18]
`
`Fig. 8B shows a circuit for providing high power pulses for improved
`
`function of the magnet stimulation device. The coil 57 and an energy storage device 58
`
`are connected in series and disposed in parallel to the switch 59. The energy storage
`
`device 58 is charged through the coil 57. To provide an energy pulse, controlled
`
`shorting of energy source 60 takes place through the switch 46.
`
`In this way the high
`
`voltage load at the terminals of the energy source 60 during the second half-period of
`
`LC resonance associated with known devices is avoided. The voltage on the terminals
`
`of energy source 60 during second half-period of LC resonance is a voltage equal to the
`
`voltage drop on the switch 59.
`
`66964-8034.US00/134971137.1
`
`15
`
`

`

`Application No. 15/396,073
`Reply to Office Action dated 03/24/2017
`
`Attorney Dkt. No. 066964-8034.U800
`
`[0037.19]
`
`The switch 59 can be any kind of switch such as diode, MOSFET, JFET,
`
`IGBT, BJT, thyristor or their combination. Depending on the type of component the load
`
`of energy source 60 is reduced to a few Volts, e.g., 1-10 volts. Consequently, it is not
`
`necessary to protect the energy source 60 from a high voltage load, e.g., thousands of
`
`Volts. The use of protective resistors and/or protection circuits is reduced or eliminated.
`
`The present designs simplify the circuits used, increase efficiency of energy usage and
`
`provide higher safety.
`
`[0037.20]
`
`Fig. 9 shows an exponential voltage drop in the energy storage device.
`
`Energy savings during time-varying magnetic therapy may be characterized by reduced
`
`voltage drop in the energy storage device between the first, second and subsequent
`
`maximums of
`
`the resonant oscillation. The magnitude of
`
`the individual voltage
`
`oscillations is exponentially dampened up to establishing the energy balance. This
`
`allows increasing the maximum possible frequency/repetition rate of magnetic pulses,
`
`since the frequency/repetition rate is dependent on the speed with which it is possible to
`
`recharge the energy storage device. Since the energy storage device is recharged by
`
`the amount of energy loss during the previous pulse,
`
`it
`
`is possible to increase the
`
`frequency/repetition rate of the device up to hundreds of magnetic pulses per second
`
`without the need to increase the input power. The voltage drop between any of the
`
`successive amplitudes is not higher than 21 %, even more preferably not higher than
`
`14 % and most preferably not higher than 7 %.
`
`[0037.21]
`
`The device can be used for treatment/successive treatments in continual,
`
`interrupted or various duty cycle regime. The duty cycle may be higher than 10 %,
`
`which means interrupted regime with the ratio up to 1 active to 9 passive time units. The
`
`66964-8034.US00/134971137.1
`
`16
`
`

`

`Application No. 15/396,073
`Reply to Office Action dated 03/24/2017
`
`Attorney Dkt. No. 066964-8034.USOO
`
`ratio may possibly change during the therapy. The device enables operation defined by
`
`the peak to peak magnetic flux density on the coil surface at least 3 T, more preferably
`
`at least 2.25 T, most preferably at least 1.5 T at repetition rates above 50 Hz, more
`
`preferably at repetition rates above 60 Hz, even more preferably at repetition rates
`
`above 70, most preferably at repetition rates above 80 Hz with treatment/successive
`
`treatments lasting several seconds or longer, for example, for at least 5, 10, 30, 60, 120
`
`or 240 seconds, or longer. The total power consumption is below 1.3 kW and the width
`
`of pulses is in the range of hundreds of us.
`
`66964-8034.USOO/134971137.1
`
`17
`
`

`

`Application No. 15/396,073
`Reply to Office Action dated 03/24/2017
`
`Attorney Dkt. No. 066964-8034.U800
`
`Please amend paragraph 0038 as follows:
`
`[0038]
`
`A magnetic treatment device may include at
`
`least one energy source
`
`and/or connection to the energy source, at least one switching device, at least one
`
`energy storage device, e.g. a capacitor, and at least one magnetic field generating
`
`device, e.g. a coil. The generated magnetic field may be time varying, preferably pulsed.
`
`The magnetic treatment is provided by a peak to peak magnetic flux density on the coil
`
`surface of at least 0.1, 0.5, 0.8, 1, 1.5, 2, 2.4 or up to 7 Tesla at repetition rate of at least
`
`0.1, 0.5, 1, 10, 30, 50, 55, 60, 80 or up to 700 Hertz with treatment/successive
`
`treatments lasting several seconds or longer, e.g. at least 5, 10, 30, 60, 120 or 240
`
`seconds, or longer. The pulse width is in the range of tens to hundreds of us, preferably
`
`in the range of 100 to 600 us, most preferably in the range of 250 to 350 us. Based on
`
`achievement of repetition rates in order of few hundreds the device also enables
`
`assemblin the ma netic ulses into the various sha es e.
`
`.
`
`trian ular
`
`rectan ular
`
`exponential), with the shape widths from 6 ms to several seconds or longer. The
`
`magnetic treatment may vary the amplitude,
`
`repetition rate and/or impulse duration
`
`during the treatment,
`
`i.e.
`
`the magnetic treatment may be modulated in amplitude
`
`domain, repetition rate domain and/or in impulse duration domain. The shape of the
`
`magnetic treatment may be adjusted following the patient’s needs.
`
`Please delete paragraphs 0040 and 0041 entirely.
`
`66964-8034.US00/134971137.1
`
`18
`
`

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