This Application is a National Stage of International Application No. PCT/JP2017/024491 filed Jul. 4, 2017, claiming priority based on Japanese Patent Application No. 2016-134423 filed Jul. 6, 2016 and 2016-134424 filed Jul. 6, 2016.
The present invention relates to an electric power steering apparatus that has a function to estimate a coil temperature of a poly-phase motor, and in particular to an electric power steering apparatus that is capable of estimating a coil temperature considering a heat transfer phenomenon between respective phases which is caused by a difference in temperature between coils of the respective phases and a heat transfer phenomenon between the coil and a control substrate.
An electric power steering apparatus (EPS) which provides a steering system of a vehicle with a steering assist torque (an assist torque) by means of a rotational torque of a motor, applies a motor driving force as the steering assist torque to a steering shaft or a rack shaft by means of a transmission mechanism such as gears or a belt through a reduction mechanism, and performs assist control. In order to accurately generate the assist torque, such a conventional electric power steering apparatus performs feedback control of a motor current. The feedback control adjusts a voltage supplied to the motor so that a difference between a steering assist command value (a current command value) and a detected motor current value becomes small, and the adjustment of the voltage supplied to the motor is generally performed by an adjustment of a duty ratio of pulse width modulation (PWM) control.
A general configuration of the conventional electric power steering apparatus will be described with reference to
Further, the steering angle sensor 14 is not indispensable and may not be provided, and it is possible to obtain the steering angle from a rotational angle sensor such as a resolver connected to the motor 20.
A controller area network (CAN) 40 to exchange various information of a vehicle is connected to the control unit 30, and it is also possible to receive the vehicle speed Vel from the CAN 40. Further, it is also possible to connect a non-CAN 41 exchanging a communication, analog/digital signals, a radio wave or the like except with the CAN 40 to the control unit 30.
The control unit 30 mainly comprises a CPU (including an MPU, an MCU and so on), and general functions performed by programs within the CPU are shown in
The control unit 30 will be described with reference to
A rotational angle sensor 21 such as a resolver is connected to the motor 20, and a rotational angle θ is detected and outputted by the rotational angle sensor 21.
A compensation signal CM from a compensation signal generating section 34 is added to the adding section 32A, and a characteristic compensation of the steering system is performed by the addition of the compensation signal CM so as to improve a convergence, an inertia characteristic and so on. The compensation signal generating section 34 adds a self-aligning torque (SAT) 343 and an inertia 342 at an adding section 344, further adds the result of addition performed at the adding section 344 with a convergence 341 at an adding section 345, and then outputs the result of addition performed at the adding section 345 as the compensation signal CM.
In the case that the motor 20 is a three-phase brushless motor, details of the PWM-control section 36 and the inverter 37 have a configuration as shown in
In such an electric power steering apparatus, a large current can flow in a motor in accordance with a steering situation (for example, a case where a steering wheel keeps hitting an end and being locked for a long time in a static steering state). When a coil in the motor has a high temperature, for example, more than or equal to 180 degrees Celsius, a problem of damage of the coil or the like occurs. Therefore, it is necessary to take measures not to overheat the coil from the viewpoint of safety of a vehicle, and to do so, it is necessary to estimate or measure a temperature of the coil (a coil temperature). However, since it is difficult to measure the coil temperature directly, methods to estimate the coil temperature have been proposed.
For example, the publication of Japanese Patent No. 5211618 B2 (Patent Document 1) constructs a temperature estimation model considering a relationship between heat transfer phenomena between poly-phase coils and a motor rotational velocity, and a relationship between a radiation coefficient and the motor rotational velocity, and estimates the coil temperature. Specifically, Patent Document 1 identifies heat transfer coefficients between a coil of any phase in a poly-phase motor and outside air environment and between any phase and another phase in accordance with a change of the motor rotational velocity, and estimates a temperature of a coil of each phase or a magnet in the motor by using a substrate temperature and a current (or a current command value) of each phase. The publication of Japanese Patent No. 4483298 B2 (Patent Document 2) estimates a temperature of amotor coil by utilizing that a calorific value of a motor is proportional to an integrated value of a square value of a current passing through the motor coil and that a temperature change of the motor coil affected by radiation (refrigeration) of the motor coil has a relationship of a primary delay function in a practically applicable temperature range (−40 to 180 degrees Celsius). Specifically, Patent Document 2 estimates the temperature of the motor coil by averaging a value obtained by squaring and integrating a value of the current passing through the motor coil, and making the result pass the primary delay function twice.
Patent Document 1: Japanese Patent No. 5211618 B2
Patent Document 2: Japanese Patent No. 4483298 B2
However, though Patent Document 1 uses a temperature of an ECU as input data considering a heat transfer between respective phase coils, it does not consider a heat transfer between each phase coil and the ECU, so that there is a possibility that an error occurs in an estimated temperature by an influence from the ECU. Since Patent Document 2 does not especially consider the influence from the ECU, there is the possibility that the error occurs in the estimated temperature by the influence from the ECU more than an apparatus in Patent Document 1.
The present invention has been developed in view of the above-described circumstances, and an object of the present invention is to provide an electric power steering apparatus that enables more precise estimation of a coil temperature by considering a heat transfer phenomenon between a control substrate and a poly-phase coil in addition to a heat transfer phenomenon between respective phases of the coil.
The present invention relates to an electric power steering apparatus that comprises a control substrate that controls a poly-phase motor, the above-described object of the present invention is achieved by that comprising: a temperature sensor that detects a substrate temperature of the control substrate; and a coil temperature estimating section that estimates coil temperatures of respective phases of the poly-phase motor by a motor current of the phase and the substrate temperature based on a heat transfer phenomenon between the respective phases that is caused by a difference in temperature between coils of the respective phases and a heat transfer phenomenon between the coil and the control substrate.
The above-described object of the present invention is more effectively achieved by that wherein the heat transfer phenomenon is expressed by a frequency characteristic; or wherein the coil temperature estimating section comprises: a coil calorific value calculating section that obtains a coil calorific value of the phase by the motor current, a substrate calorific value calculating section that obtains a substrate calorific value of the control substrate by the motor current, and a coil temperature calculating section that obtains the coil temperature by the coil calorific value, the substrate calorific value and the substrate temperature based on the frequency characteristic; or wherein the coil calorific value calculating section changes a coil resistance of the phase used to obtain the coil calorific value, depending on the coil temperature of a corresponding phase, and wherein the substrate calorific value calculating section changes a substrate resistance used to obtain the substrate calorific value, depending on the substrate temperature; or wherein the frequency characteristic includes a calorific value frequency characteristic that is a frequency characteristic from the coil calorific value or the substrate calorific value to the coil temperature or the substrate temperature, and an outside air temperature frequency characteristic that is a frequency characteristic from an outside air temperature to the coil temperature or the substrate temperature; or wherein the coil temperature calculating section defines the calorific value frequency characteristic and the outside air temperature frequency characteristic as a transfer function, and obtains the coil temperature by a linear combination of the coil calorific value, the substrate calorific value and the substrate temperature; or wherein the heat transfer phenomenon is expressed by a differential equation; or wherein the coil temperature estimating section comprises: a coil calorific value calculating section that obtains a coil calorific value of the phase by the motor current, a substrate calorific value calculating section that obtains a substrate calorific value of the control substrate by the motor current, and a coil temperature calculating section that obtains the coil temperature by the coil calorific value, the substrate calorific value and the substrate temperature based on the differential equation; or wherein the coil calorific value calculating section changes a coil resistance of the phase used to obtain the coil calorific value, depending on the coil temperature of a corresponding phase, and wherein the substrate calorific value calculating section changes a substrate resistance used to obtain the substrate calorific value, depending on the substrate temperature; or wherein the differential equation includes difference information between the coil temperature and the substrate temperature.
Since estimating the coil temperatures of respective phases by using the relational expression that is obtained by considering the heat transfer phenomenon between the coil and the control substrate in addition to the heat transfer phenomenon between the respective phases which is caused by the difference in temperature between the coils of the respective phases, the electric power steering apparatus according to the present invention enables more precise estimation of the temperature.
In the accompanying drawings:
The present invention estimates temperatures of coils (coil temperatures) in respective phases (a U-phase, a V-phase and a W-phase) of a poly-phase motor on the basis of a heat transfer phenomenon (a heat conduction, a heat radiation, a heat convection, and so on) between respective phases and a heat transfer phenomenon between each coil and a substrate (a control substrate) of a control unit (ECU). In the poly-phase motor, a difference in calorific values of respective coils occurs by such as dispersion of currents (motor currents) passing through the coils in respective phases, and that causes a difference in temperature between respective coils. This difference in temperature causes heat transfer phenomena between respective phases and between each coil and outside air environment, while a difference in temperature occurs also between the control substrate and each coil. Since the control substrate and the motor are generally close, heat transfer phenomena also occur between the control substrate and each coil and between the control substrate and the outside air environment. The present invention estimates the coil temperature using a motor current and a temperature of the control substrate (a substrate temperature), for example, by expressing those heat transfer phenomena by a frequency characteristic, formulating a relationship between the calorific value and the coil temperature, and obtaining the calorific value from the motor current, or by expressing those heat transfer phenomena by a differential equation, and including difference information between the coil temperature and the substrate temperature in the differential equation.
Hereinafter, an embodiment of the present invention will be described with reference to the accompanying drawings.
An electric power steering apparatus of the present embodiment drives and controls a three-phase (the U-phase, the V-phase and the W-phase) brushless motor, and an object for estimation of the coil temperature is a coil shown by the circle in
In
In
The coil calorific value calculating sections 310, 320 and 330 respectively calculate calorific values (coil calorific values) QU, QV and QW of coils in respective phases. Though a calorific value can be obtained from an expression of electric power occurring in a resistance, a resistance of a coil (a coil resistance) in each phase is changed depending on the coil temperature in each phase. Therefore, the coil calorific values QU, QV and QW are calculated in accordance with the following expressions 1 to 3 by dealing with the coil resistance as a function of the coil temperature.
QU=RU(TU)×iu(t)2 [Expression 1]
QV=RV(TV)×iv(t)2 [Expression 2]
QW=RW(TW)×iw(t)2 [Expression 3]
Here, RU(TU), RV(TV) and RW(TW) are the coil resistances of the U-phase, the V-phase and the W-phase respectively, and TU, TV and TW are the coil temperatures of the U-phase, the V-phase and the W-phase respectively. The motor currents iu, iv and iw are expressed as functions of time t.
Moreover, the coil resistances RU(T), RV(T) and RW(T) in the case that the coil temperature is T, can be calculated in accordance with the following expressions 4 to 6 when the coil resistances at a reference temperature Tb are RU0, RV0 and RW0 respectively.
RU(T)=RU0×{1+αU×(T−Tb)} [Expression 4]
RV(T)=RV0×{1+αV×(T−Tb)} [Expression 5]
RW(T)=RW0×{1+αW×(T−Tb)} [Expression 6]
Here, αU, αV and αW are temperature coefficients of the U-phase, the V-phase and the W-phase respectively, for example, become 4.4×10−3 [1/° C.] when the coil is a copper, and may be finely adjusted by an experiment and so on.
The coil calorific values QU, QV and QW can be calculated in accordance with the following expressions 7 to 9 by substituting the expressions 4 to 6 for the expressions 1 to 3 respectively.
QU=RU0{1+αU×(TU−Tb)}×iu(t)2 [Expression 7]
QV=RV0×{1+αV×(TV−Tb)}×iv(t)2 [Expression 8]
QW=RW0×{1+αW×(TW−Tb)}×iw(t)2 [Expression 9]
The coil calorific value calculating sections 310, 320 and 330 calculate the coil calorific values QU, QV and QW by using the above expressions 7 to 9 respectively.
The substrate calorific value calculating section 340 also calculates a calorific value of the control substrate (a substrate calorific value) QE from an expression of electric power occurring in a resistance, and it obtains a magnitude of a current needed for the calculation by the motor currents iu, iv and iw. A calorific equivalent resistance of the control substrate (a substrate resistance) is changed depending on a temperature (the substrate temperature TE in the case of the control substrate) as with the coil resistance. Further, since the control substrate has heating corresponding to standby power such as feeble heating of a semiconductor switching element and heating caused by operations of a microcomputer or other semiconductors without a current passing through the coil in a state where an ignition is turned on, it is necessary to consider it in the calculation of the calorific value. Consequently, the calorific value QE of the control substrate is calculated in accordance with the following expression 10.
QE=RE(TE)×(iu(t)2+iv(t)2+iw(t)2)+QE0 [Expression 10]
Here, RE(TE) is the substrate resistance, and QE0 a calorific value corresponding to standby power. The substrate resistance RE(T) in the case that the substrate temperature is T is calculated in accordance with the following expression 11 when the substrate resistance at the reference temperature Tb is RE0 and a temperature coefficient of the control substrate is αE.
RE(T)=RE0×{1+αE×(T−Tb)} [Expression 11]
The substrate calorific values QE can be calculated in accordance with the following expression 12 by substituting the expression 11 for the expression 10.
QE=RE0×{1+αE×(TE−Tb)}×(iu(t)2+iv(t)2+iw(t)2)+QE0 [Expression 12]
In a case where there is no influence of a calorific value corresponding to standby power, a case where the calorific value corresponding to standby power is negligibly minute, and so on, it is possible to delete the QE0 in the above expressions 10 and 12
The substrate calorific value calculating section 340 calculates the substrate calorific value QE by using the above expression 12.
A coil temperature calculating section 350 calculates coil temperatures TU, TV and TW in respective phases from the coil calorific values QU, QV and QW, the substrate calorific value QE, and the substrate temperature TE. Derivation of expressions to calculate them will be described.
Transfer functions from the coil calorific values QU, QV and QW, the substrate calorific value QE and an outside air temperature T0 to the coil temperatures TU, TV and TW in respective phases and the substrate temperature TE can be expressed by the following expressions 13 to 16.
TU=GUU(s)QU+GVU(s)QV+GWU(s)QW+GEU(s)QE+G0U(s)T0 [Expression 13]
TV=GUV(s)QU+GVV(s)QV+GWV(s)QW+GEV(s)QE+G0v(s)T0 [Expression 14]
TW=GUW(s)QU+GVW(s)QV+GWW(s)QW+GEW(s)QE+G0W(s)T0 [Expression 15]
TE=GUE(s)QU+GVE(s)QV+GWE(s)QW+GEE(S)QE+G0E(s)T0 [Expression 16]
Here, GXY(s) is a frequency characteristic (a calorific value frequency characteristic) from a calorific value QX to a coil temperature TY in a Y-phase (X and Y are any of U, V, W and E), G0X is a frequency characteristic (an outside air temperature frequency characteristic) from the outside air temperature T0 to a coil temperature TX in a X-phase (X is any of U, V, W and E), and the control substrate is regarded as an E-phase to simplify the explanation. “s” is a Laplace operator. In the case that a relationship between a group of the calorific value and the outside air temperature and the temperature (the coil temperature or the substrate temperature) in each phase is approximately a linear combination, the above frequency characteristic is defined as a transfer function having a predetermined value.
The following expressions 17 to 19 are obtained by solving the above expression 16 for T0, substituting the result for the above expressions 13 to 15, and arranging the substitution results (hereinafter, “(s)” is omitted to make the expression easy to see by simplification).
TU=GUU′QU+GVU′QV+GWU′QW+GEU′QE+GTUTE [Expression 17]
TV=GUV′QU+GVV′QV+GWV′QW+GEV′QE+GTVTE [Expression 18]
TW=GUW′Q+GVW′QV+GWW′QW+GEW′QE+GTWTE [Expression 19]
Here, GTB=G0B/G0E, GAB′=GAB−GTBGAE, and GEB′=GEB−GTBGEE (A and B are any of U, V and W).
The coil temperatures TU, TV and TW are inputted into an abnormality processing section 210, and at the same time, are retained in memories 360, 370 and 380 respectively to be used for the next calculation of the calorific value at the coil calorific value calculating sections 310, 320 and 330.
The abnormality processing section 210 performs, for example, processing at an abnormality judging section 25 and a motor current limiting section 23 described in a publication of Japanese Patent No. 4356295 B2. That is, as with the processing at the abnormality judging section 25, the abnormality processing section 210 judges whether the coil temperatures TU, TV and TW exceed a preset tolerance limit temperature of the motor 20 or not, and judges that the motor 20 is overheated when they exceed it. When judging the overheating state, the abnormality processing section 210 gradually decreases the current command value with the elapse of time and gradually decreases the motor current with the elapse of time as with the processing at the motor current limiting section 23, or sets the current command value to zero and cuts off the motor current. It is possible to mount a temperature detecting circuit 31 and a temperature detecting section 26 described in the same publication and judge an abnormality of the temperature detecting circuit 31.
A coil temperature estimating section comprises the above coil calorific value calculating sections 310, 320 and 330, the substrate calorific value calculating section 340 and the coil temperature calculating section 350.
In such a configuration, an operating example of estimation of the coil temperature will be described with reference to a flowchart in
The U-phase motor current iu, the V-phase motor current iv and the W-phase motor current iw which are detected by the motor current detector 38 are inputted into the coil calorific value calculating sections 310, 320 and 330 respectively, and at the same time, are inputted into the substrate calorific value calculating section 340 (Step S10). The temperature sensor 200 detects the temperature of the control substrate (Step S20), and outputs the substrate temperature TE to the substrate calorific value calculating section 340 and the coil temperature calculating section 350. Moreover, the detection of the motor current and the detection of the substrate temperature may interchange in order, or may be performed in parallel.
The coil calorific value calculating sections 310 calculates the coil calorific value QU in the U-phase by using the U-phase motor current iu and the previously estimated coil temperature TU′ retained in the memory 360 in accordance with the expression 7. Similarly, the coil calorific value calculating sections 320 calculates the coil calorific value QV in the V-phase by using the V-phase motor current iv and the coil temperature TV′ retained in the memory 370 in accordance with the expression 8, and the coil calorific value calculating sections 330 calculates the coil calorific value QW in the W-phase by using the W-phase motor current iw and the coil temperature TW′ retained in the memory 380 in accordance with the expression 9 (Step S30). The reference temperature Tb, the coil resistances RU0, RV0 and RW0 at the reference temperature Tb and the temperature coefficients αU, αV and αW are preset.
The substrate calorific value calculating section 340 calculates the substrate calorific value QE by using the inputted motor currents iu, iv and iw and the substrate temperature TE in accordance with the expression 12 (Step S40). The reference temperature Tb, the substrate resistance RE0 at the reference temperature Tb, the temperature coefficient αE and the calorific value QE0 are preset.
The coil calorific values QU, QV and QW and the substrate calorific value QE are inputted into the coil temperature calculating section 350 with the substrate temperature TE. The coil temperature calculating section 350 calculates the coil temperatures TU, TV and TW by the coil calorific values QU, QV and QW, the substrate calorific value QE and the substrate temperature TE on the basis of the expressions 17 to 19 (Step S50). The coil temperatures TU, TV and TW are inputted into the abnormality processing section 210, and at the same time, are retained in the memories 360, 370 and 380 respectively (Step S60).
Moreover, it is possible to merge the coil calorific value calculating sections 310, 320 and 330, and calculate the coil calorific values QU, QV and QW in accordance with the expressions 7, 8 and 9. Further, memories 360, 370 and 380 may be also merged, or a shared memory may be used.
A second embodiment of the present invention will be described.
Though a whole configuration of the second embodiment is similar to one of the first embodiment, a configuration of the coil temperature calculating section is different.
The setting shown by the following expression 20 can be applied to the expressions 17 to 19 which the calculation at the coil temperature calculating section 350 of the first embodiment is based on because of symmetry of the phases.
GUU′=GVV′=GWW′=GL
GUV′=GVU′=GUW′=GWU′=GVW′=GWV′=GM
GEU′=GEV′=GEW′=GE
GTU=GTV=GTW=GTE [Expression 20]
The following expressions 21 to 23 are obtained by substituting the above expression 20 for the expressions 17 to 19, and arranging the substitution results.
TU=GLQU+GM(QV+QW)+GEQE+GTETE [Expression 21]
TV=GLQV+GM(QW+QU)+GEQE+GTETE [Expression 22]
TW=GLQW+GM(QU+QV)+GEQE+GTETE [Expression 23]
Comparing an operation of estimation of the coil temperature in the second embodiment with one in the first embodiment, the only above operation of the coil temperature calculating section is different, and other operations are the same.
In the above embodiments (the first embodiment and the second embodiment), though the coil temperature calculating section performs the calculations with the configuration shown in
A third embodiment of the present invention will be described.
A configuration example of the third embodiment is shown in
The coil temperature calculating section 550 calculates the coil temperatures TU, TV and TW in respective phases on the basis of a differential equation of heat conduction.
The differential equations of heat conduction with respect to the coils in the U-phase, the V-phase and the W-phase are the following expressions 24, 25 and 26 respectively.
Here, CL is a heat capacity of the coil, KL is a heat loss coefficient of the coil, KLL is a heat transfer coefficient between the coils, and KLE is a heat transfer coefficient between the coil and the control substrate. Difference information of the fifth term of the right side in each of the above expressions 24 to 26 expresses the heat conduction between each phase and the control substrate.
The differential equation of heat conduction with respect to the control substrate is the following expression 27.
Here, CE is a heat capacity of the control substrate, and KE is a heat loss coefficient of the control substrate. Difference information from the third term to the fifth term of the right side in the above expression 27 expresses the heat conduction between each phase and the control substrate.
The following expressions 29 to 32 are obtained by arranging the above expression 24 to 27 and setting values as shown by the following expression 28.
The following expression 33 is obtained by transforming the above expression 32 and solving the transformation result for the outside air temperature T0.
Therefore, it is possible to obtain renewed coil temperatures TU, TV and TW by obtaining the outside air temperature T0 using the expression 33 by the substrate temperature TE, the coil temperatures TU, TV and TW and the substrate calorific value QE, obtaining differential values of the coil temperatures TU, TV and TW using the expressions 29 to 31 by the outside air temperature T0, the coil calorific values QU, QV and QW, the coil temperatures TU, TV and TW and the substrate temperature TE, and integrating the differential values.
The coil temperature calculating section 550 calculates the coil temperatures TU, TV and TW in respective phases on the basis of the above expressions 29 to 31 and 33. A configuration example of the coil temperature calculating section 550 is shown in
The coil temperatures TU, TV and TW calculated at the coil temperature calculating section 550 are inputted into the abnormality processing section 210, and at the same time, are retained in the memories 360, 370 and 380 respectively to be used in next calculations of the coil calorific values and next calculations of the coil temperatures.
An operating example of estimation of the coil temperature in the third embodiment will be described with reference to a flowchart in
The third embodiment performs the same operations as the first embodiment until calculating the substrate calorific value QE (Steps S10 to S40).
The coil calorific values QU, QV and QW and the substrate calorific value QE are inputted into the coil temperature calculating section 550.
The outside air temperature calculating section 552 in the coil temperature calculating section 550 inputs the addition result (TU+TV+TW) retained in the memory 556 with the calorific value QE and the substrate temperature TE, calculates the outside air temperature T0 in accordance with the expression 33 (Step S41), and outputs it to the differential equation calculating section 551. The differential equation calculating section 551 calculates the differential values DTU, DTV and DTW of the coil temperatures by the coil calorific values QU, QV and QW, the substrate temperature TE, the outside air temperature T0 and the coil temperatures TU′, TV′ and TW′ retained in the memories 360, 370 and 380 respectively in accordance with the expressions 29 to 31 (Step S42). The integrating sections 553, 554 and 555 input the differential values DTU, DTV and DTW respectively, integrate them, and calculate the coil temperatures TU, TV and TW (Step S43). The coil temperatures TU, TV and TW are outputted, and at the same time, are added at the adding sections 557 and 558. The addition result (TU+TV+TW) is retained in the memory 556 for the next calculation of the outside air temperature (Step S44).
The coil temperatures TU, TV and TW outputted from the coil temperature calculating section 550 are inputted into the abnormality processing section 210, and at the same time, are retained in the memories 360, 370 and 380 respectively (Step S60) Though the coil temperature calculating section 550 retains the addition result of the coil temperatures TU, TV and TW in the memory 556, it is possible to use an addition result of the coil temperatures TU′, TV′ and TW′ retained in the memories 360, 370 and 380 respectively when the outside air temperature calculating section 552 calculates the outside air temperature T0. Further, though the coil temperature calculating section 550 calculates the coil temperature based on the differential equation, it is also possible to calculate it after transforming the differential equation into a difference equation that is generally used and is capable of being mounted in the ECU, or to calculate it after transforming the differential equation into a transfer function.
Though the above embodiments (the first to the third embodiments) target the three-phase motor, the present invention can be applied to a motor where the number of phases is other than three.
Number | Date | Country | Kind |
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2016-134423 | Jul 2016 | JP | national |
2016-134424 | Jul 2016 | JP | national |
Filing Document | Filing Date | Country | Kind |
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PCT/JP2017/024491 | 7/4/2017 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
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WO2018/008633 | 1/11/2018 | WO | A |
Number | Name | Date | Kind |
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6854881 | Nada | Feb 2005 | B2 |
Number | Date | Country |
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2003-134869 | May 2003 | JP |
2009-089531 | Apr 2009 | JP |
4483298 | Jun 2010 | JP |
5211618 | Jun 2013 | JP |
Entry |
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International Search Report for PCT/JP2017/024491, dated Oct. 10, 2017. |
Number | Date | Country | |
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20190337560 A1 | Nov 2019 | US |