WO1998021762A1 - Methode de commande d'un transducteur magneto-mecanique - Google Patents
Methode de commande d'un transducteur magneto-mecanique Download PDFInfo
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- WO1998021762A1 WO1998021762A1 PCT/RU1997/000321 RU9700321W WO9821762A1 WO 1998021762 A1 WO1998021762 A1 WO 1998021762A1 RU 9700321 W RU9700321 W RU 9700321W WO 9821762 A1 WO9821762 A1 WO 9821762A1
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- WO
- WIPO (PCT)
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- magnetic field
- οsnοvnοgο
- seρdechniκa
- naπρyazhennοsτi
- isποlniτelnοgο
- Prior art date
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- 238000000034 method Methods 0.000 title claims abstract description 10
- 239000000463 material Substances 0.000 claims abstract description 12
- 230000004308 accommodation Effects 0.000 claims description 3
- 230000005389 magnetism Effects 0.000 claims description 3
- 230000000694 effects Effects 0.000 claims 1
- 238000004870 electrical engineering Methods 0.000 abstract 1
- 230000001105 regulatory effect Effects 0.000 abstract 1
- 239000013598 vector Substances 0.000 abstract 1
- 239000011162 core material Substances 0.000 description 10
- 238000005265 energy consumption Methods 0.000 description 2
- 230000005415 magnetization Effects 0.000 description 2
- 238000001311 chemical methods and process Methods 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 238000007907 direct compression Methods 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 239000000696 magnetic material Substances 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 210000002966 serum Anatomy 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N35/00—Magnetostrictive devices
Definitions
- ch ⁇ is ⁇ lz ⁇ vanie in izves ⁇ n ⁇ m magni ⁇ me ⁇ aniches ⁇ m ⁇ e ⁇ b ⁇ az ⁇ va ⁇ ele is ⁇ chni ⁇ a magni ⁇ n ⁇ g ⁇ ⁇ lya as ele ⁇ iches ⁇ y ⁇ bm ⁇ i v ⁇ zbuzhdeniya ⁇ ebue ⁇ in ⁇ tsesse u ⁇ avleniya ⁇ be ⁇ m ⁇ s ⁇ yann ⁇ g ⁇ ele ⁇ ebleniya not ⁇ l ⁇ for ⁇ susches ⁇ vleniya ⁇ tsessa changes ⁇ dina ⁇ y ⁇ l ⁇ zheniya tsen ⁇ a mass is ⁇ lni ⁇ eln ⁇ g ⁇ zlemen ⁇ a, n ⁇ and s ⁇ aneniya v ⁇ v ⁇ emeni ⁇ e ⁇ n ⁇ l ⁇ giches ⁇ i zadann ⁇ g ⁇
- E ⁇ yavlyae ⁇ sya ⁇ ichin ⁇ y increase mass ⁇ gaba ⁇ i ⁇ ny ⁇ ⁇ aza ⁇ eley us ⁇ ys ⁇ va for ⁇ ealizatsii s ⁇ s ⁇ ba in tsel ⁇ m not ⁇ zv ⁇ lyae ⁇ ⁇ bes ⁇ echi ⁇ ne ⁇ b ⁇ dimuyu ⁇ chn ⁇ s ⁇ ⁇ zitsi ⁇ ni ⁇ vaniya ⁇ i is ⁇ lz ⁇ vanii izves ⁇ n ⁇ g ⁇ s ⁇ s ⁇ ba u ⁇ avleniya magni ⁇ me ⁇ aniches ⁇ im ⁇ e ⁇ b ⁇ az ⁇ va ⁇ elem in sis ⁇ ema ⁇ ⁇ etsizi ⁇ nn ⁇ g ⁇ ⁇ zitsi ⁇ ni ⁇ vaniya.
- ⁇ as ⁇ y ⁇ ie iz ⁇ b ⁇ e ⁇ eniya ⁇ ⁇ sn ⁇ vu zayavlenn ⁇ g ⁇ iz ⁇ b ⁇ e ⁇ eniya was ⁇ l ⁇ zhena task s ⁇ zdaniya ⁇ a ⁇ g ⁇ s ⁇ s ⁇ ba u ⁇ avleniya magni ⁇ me ⁇ aniches ⁇ im ⁇ e ⁇ b ⁇ az ⁇ va ⁇ ele, ⁇ y ⁇ zv ⁇ lil 6Li ⁇ susches ⁇ vlya ⁇ ⁇ tsess u ⁇ avlenie with minimal zne ⁇ g ⁇ za ⁇ a ⁇ ami on account of reduction zne ⁇ g ⁇ ebleniya in ⁇ tsesse changes ⁇ dina ⁇ y ⁇ l ⁇ zheniya tsen ⁇ a mass is ⁇ lni ⁇ eln ⁇ g ⁇ elemen ⁇ a and ⁇ ln ⁇ g ⁇ is ⁇ lyucheniya ene ⁇ g ⁇ ebleniya ⁇
- Fig. 3 - illustrates one of the different options for the execution of a large source of magnets.
- ⁇ ig.4 and ⁇ ig.5 - g ⁇ a ⁇ iches ⁇ i illyus ⁇ i ⁇ uyu ⁇ ⁇ e ⁇ li gis ⁇ e ⁇ ezisa zavisim ⁇ s ⁇ i magni ⁇ s ⁇ i ⁇ tsi ⁇ nn ⁇ g ⁇ se ⁇ dechni ⁇ a length change (or ch ⁇ ⁇ avn ⁇ znachn ⁇ changes ⁇ dina ⁇ y tsen ⁇ a mass is ⁇ lni ⁇ eln ⁇ g ⁇ elemen ⁇ a), ⁇ na ⁇ yazhenn ⁇ s ⁇ i ⁇ sn ⁇ vn ⁇ g ⁇ magni ⁇ n ⁇ g ⁇ ⁇ lya in z ⁇ ne se ⁇ dechni ⁇ a ⁇ i presence vs ⁇ m ⁇ ga ⁇ eln ⁇ g ⁇ magni ⁇ n ⁇ g
- the magnetic system includes the fully-available source 6 of a permanent magnetic source, such as a small one.
- ⁇ sn ⁇ vn ⁇ y u ⁇ avlyaemy is ⁇ chni ⁇ 2 magni ⁇ n ⁇ g ⁇ ⁇ l I magni ⁇ n ⁇ y sis ⁇ emy ⁇ as ⁇ l ⁇ zhen with v ⁇ zm ⁇ zhn ⁇ s ⁇ yu s ⁇ zdaniya in z ⁇ ne se ⁇ dechni ⁇ a 3 ⁇ sn ⁇ vn ⁇ g ⁇ magician ni ⁇ n ⁇ g ⁇ ⁇ lya as an s ⁇ vmeschenny ⁇ v ⁇ v ⁇ emeni im ⁇ ul s ⁇ v ⁇ sn ⁇ vn ⁇ g ⁇ magni ⁇ n ⁇ g ⁇ ⁇ lya, ⁇ e ⁇ tsii ve ⁇ v na ⁇ yazhenn ⁇ s ⁇ i ⁇ y ⁇ on ⁇ s se ⁇ dechni ⁇ a 3 s ⁇ v ⁇ adayuschuyu with na ⁇
- the invention relates to the use of a magnetic device according to the invention in accordance with the following general rules.
- the most optimal primary magnetic field in the middle of the core is to create in the form of not simultaneously pulsed parallel pulses between the magnetic field itself.
- the center of mass of the executive element 4 corresponds to point 7.
- tsen ⁇ mass is ⁇ lni ⁇ eln ⁇ g ⁇ zlemen ⁇ a 4 sam ⁇ izv ⁇ ln ⁇ (in ⁇ ezul ⁇ a ⁇ e presence in z ⁇ ne se ⁇ dechni ⁇ a 3 ⁇ s ⁇ yann ⁇ g ⁇ magni ⁇ n ⁇ g ⁇ ⁇ lya, gene ⁇ i ⁇ uem ⁇ g ⁇ vs ⁇ m ⁇ ga ⁇ elnym is ⁇ chni ⁇ m 6 mag
- tsi ⁇ lu ⁇ e ⁇ e ⁇ da tsen ⁇ a mass is ⁇ lni ⁇ eln ⁇ g ⁇ elemen ⁇ a 4 of ⁇ l ⁇ zheniya, s ⁇ ve ⁇ s ⁇ vuyuscheg ⁇ ⁇ ch ⁇ e 7 ⁇ l ⁇ zhenie, s ⁇ ve ⁇ s ⁇ vuyuschee ⁇ ch ⁇ e 1 che ⁇ ez ⁇ l ⁇ zhenie, s ⁇ ve ⁇ s ⁇ vuyuschee ⁇ ch ⁇ e 0 (or ⁇ l ⁇ zhenie, s ⁇ ve ⁇ s ⁇ vuyuschee ⁇ ch ⁇ e 8) s ⁇ ve ⁇ s ⁇ vue ⁇ ⁇ iv ⁇ lineyny ⁇ ez ⁇ 7 0-1 (7-0-8 0 or 1 ), correspondingly, for the hysteresis of the change in the linear size of the center 3 (corresponding to the change in the mass center of the main element).
- Tsi ⁇ l ⁇ e ⁇ emescheniya tsen ⁇ a mass is ⁇ lni ⁇ eln ⁇ g ⁇ elemen ⁇ a 4 of ⁇ l ⁇ zheniya, s ⁇ ve ⁇ s ⁇ vuyuscheg ⁇ ⁇ ch ⁇ e 1 ⁇ l ⁇ zhenie, s ⁇ ve ⁇ s ⁇ vuyuschee ⁇ ch ⁇ e 3 ⁇ susches ⁇ vlyae ⁇ sya on account s ⁇ zdaniya in z ⁇ ne se ⁇ dechni ⁇ a 3 ⁇ s ⁇ eds ⁇ v ⁇ m ⁇ sn ⁇ vn ⁇ g ⁇ u ⁇ avlyaem ⁇ g ⁇ is ⁇ chni ⁇ a 2 magni ⁇ n ⁇ g ⁇ ⁇ lya, im ⁇ ulsa ⁇ sn ⁇ vn ⁇ g ⁇ magni ⁇ n ⁇ g ⁇ ⁇ lya ( ⁇ iv ⁇ l ⁇ zhn ⁇ g ⁇ na ⁇ avleniya ⁇ ⁇ n ⁇ sheniyu ⁇
- tsen ⁇ mass is ⁇ lni ⁇ eln ⁇ g ⁇ elemen ⁇ a 4 sam ⁇ izv ⁇ ln ⁇ ⁇ e ⁇ emeschae ⁇ sya in ⁇ l ⁇ zhenie, s ⁇ ve ⁇ s ⁇ vuyuschee ⁇ ch ⁇ e 3 and bude ⁇ na ⁇ di ⁇ sya in z ⁇ m ⁇ i ⁇ si ⁇ vann ⁇ m ⁇ l ⁇ zh
- ⁇ a ⁇ ig. 4 for the mass center location of the Executive Unit 4 from the location corresponding to point 1 to the location corresponding to step 3 (after the end of 2 with the exit Corresponds to a short circuit 1 2 3 for the hysteresis of a change in the linear size of the center 3 (or, respectively, for a change in the mass center of the unit).
- P ⁇ tsess ⁇ susches ⁇ vleniya v ⁇ zv ⁇ a ⁇ a tsen ⁇ a mass is ⁇ lni ⁇ eln ⁇ g ⁇ elemen ⁇ a 4 of ⁇ l ⁇ zheniya, s ⁇ ve ⁇ s ⁇ vuyuscheg ⁇ ⁇ ch ⁇ e 3 ⁇ l ⁇ zhenie, s ⁇ ve ⁇ s ⁇ vuyuschee ⁇ ch ⁇ e 1 (is ⁇ dn ⁇ e ⁇ l ⁇ zhenie) ⁇ susches ⁇ vlyae ⁇ sya abs ⁇ lyu ⁇ n ⁇ iden ⁇ ichn ⁇ vyshe ⁇ isann ⁇ mu tsi ⁇ lu ⁇ e ⁇ e ⁇ da tsen ⁇ a mass of ⁇ l ⁇ zheniya, s ⁇ ve ⁇ s ⁇ vuyuscheg ⁇ ⁇ ch ⁇ e 7 ⁇ l ⁇ zhenie, s ⁇ ve ⁇ s ⁇ vuyuschee ⁇ ch ⁇ e 1 ( ⁇ .e., che ⁇ ez
- ⁇ a ⁇ ig. 4 tsi ⁇ lu ⁇ e ⁇ e ⁇ da tsen ⁇ a mass is ⁇ lni ⁇ eln ⁇ g ⁇ elemen ⁇ a 4 of ⁇ l ⁇ zheniya, s ⁇ ve ⁇ s ⁇ vuyuscheg ⁇ ⁇ ch ⁇ e 3 ⁇ l ⁇ zhenie, s ⁇ ve ⁇ s ⁇ vuyuschee ⁇ ch ⁇ e 1 che ⁇ ez ⁇ l ⁇ zhenie, s ⁇ ve ⁇ s ⁇ vuyuschee ⁇ ch ⁇ e 0 (or ⁇ l ⁇ zhenie, s ⁇ ve ⁇ s ⁇ vuyuschee ⁇ ch ⁇ e 8 ⁇ dina ⁇ y d ⁇ - ⁇ ) s ⁇ ve ⁇ s ⁇ vue ⁇ ⁇ iv ⁇ lineyny ⁇ ez ⁇ 3-0-1 (or 3 -0
- P ⁇ tsessy ⁇ e ⁇ emescheniya tsen ⁇ a mass is ⁇ lni ⁇ eln ⁇ g ⁇ elemen ⁇ a 4 of ⁇ l ⁇ zheniya, s ⁇ ve ⁇ s ⁇ vuyuscheg ⁇ ⁇ ch ⁇ e 1 ⁇ l ⁇ zheniya, s ⁇ ve ⁇ s ⁇ vuyuschie ⁇ ch ⁇ am 5 and 7, and ⁇ a ⁇ zhe v ⁇ zv ⁇ a ⁇ u ⁇ myanu ⁇ g ⁇ tsen ⁇ a masses is ⁇ dn ⁇ e ⁇ l ⁇ zhenie ( ⁇ l ⁇ zhenie, s ⁇ ve ⁇ s ⁇ vuyuschee ⁇ ch ⁇ e 1) ⁇ iziches ⁇ y ⁇ ch ⁇ i z ⁇ eniya ⁇ susches ⁇ vlyayu ⁇ sya anal ⁇ gichn ⁇ vyshe ⁇ isannym tsi ⁇ lam ⁇ e ⁇ emescheniya tsen ⁇ a weight of
- the aforementioned provisions
- ⁇ imenn ⁇ - ⁇ e ⁇ emeschenie tsen ⁇ a mass is ⁇ lni ⁇ eln ⁇ g ⁇ elemen ⁇ a 4 of ⁇ l ⁇ zheniya, s ⁇ v ⁇ s ⁇ vuyuscheg ⁇ ⁇ ch ⁇ e 1 ⁇ l ⁇ zhenie, s ⁇ ve ⁇ s ⁇ vuyuschee ⁇ ch ⁇ e 5 ⁇ susches ⁇ vlyae ⁇ sya on account s ⁇ zdaniya in z ⁇ ne se ⁇ dechni ⁇ a 3 ⁇ s ⁇ eds ⁇ v ⁇ m ⁇ sn ⁇ vn ⁇ g ⁇ u ⁇ avlyaem ⁇ g ⁇ is ⁇ chni ⁇ a 2 magni ⁇ n ⁇ g ⁇ ⁇ lya, im ⁇ ulsa ⁇ sn ⁇ vn ⁇ g ⁇ magni ⁇ n ⁇ g ⁇ ⁇ lya ( ⁇ iv ⁇ l ⁇ zhn ⁇ g ⁇ na ⁇ avleniya ⁇ ⁇ n ⁇ sheniyu
- I ⁇ PU'LSU ⁇ S ⁇ G ⁇ ⁇ aG ⁇ I ⁇ G ⁇ P ⁇ LYA) C ⁇ eLIChI ⁇ Y ⁇ 4- ⁇ na ⁇ yazhenn ⁇ s ⁇ i and reduce na ⁇ yazhenn ⁇ s ⁇ i e ⁇ g ⁇ im ⁇ ulsa ⁇ sn ⁇ vn ⁇ g ⁇ magni ⁇ n ⁇ g ⁇ ⁇ lya d ⁇ nulev ⁇ g ⁇ values ⁇ i z ⁇ m summa ⁇ naya value na ⁇ yazhenn ⁇ s ⁇ i magni ⁇ n ⁇ g ⁇ ⁇ lya in z ⁇ ne se ⁇ dechni ⁇ a 3 bude ⁇ ⁇ avna value ⁇ 4, and za ⁇ em umenshi ⁇ sya d ⁇ values ⁇ ;
- the indicated cycle is carried out after use, corresponding to point 4 (with a quick l- 1 '”) and ⁇ ⁇ 98/21762 0 ⁇ / ⁇ 7 / 00321 is short
- I ⁇ PULSU ⁇ S ⁇ G ⁇ ⁇ EG ⁇ I ⁇ G ⁇ P ⁇ LYA C ⁇ eLIChI ⁇ Y ⁇ b- ⁇ na ⁇ yazhenn ⁇ s ⁇ i and reduce na ⁇ yazhenn ⁇ s ⁇ i e ⁇ g ⁇ im ⁇ ulsa ⁇ sn ⁇ vn ⁇ g ⁇ magni ⁇ n ⁇ g ⁇ ⁇ lya d ⁇ nulev ⁇ g ⁇ values ⁇ i e ⁇ m summa ⁇ naya value na ⁇ yazhenn ⁇ s ⁇ i magni ⁇ n ⁇ g ⁇ ⁇ lya in z ⁇ ne se ⁇ dechni ⁇ a 3 bude ⁇ ⁇ avna value ⁇ b and za ⁇ em umenshi ⁇ sya d ⁇ ⁇ ;
- the indicated cycle is realized after use, which corresponds to point 6 (with a standard ⁇ -.
- U ⁇ avlenie magni ⁇ me ⁇ anich ⁇ s ⁇ im ⁇ e ⁇ b ⁇ az ⁇ va ⁇ elem s ⁇ glasn ⁇ s ⁇ eme u ⁇ avleniya ⁇ ⁇ ig.5 ⁇ susches ⁇ vlyae ⁇ sya ⁇ b ⁇ az ⁇ m follows: ⁇ e ⁇ emeschenie tsen ⁇ a mass is ⁇ lni ⁇ eln ⁇ g ⁇ elemen ⁇ a 4 of ⁇ l ⁇ zheniya, s ⁇ ve ⁇ s ⁇ vuyuscheg ⁇ ⁇ ch ⁇ e I in ⁇ l ⁇ zhenie, s ⁇ ve ⁇ s ⁇ vuyuschee ⁇ ch ⁇ e 3 ⁇ susches ⁇ vlyae ⁇ sya on account s ⁇ zdaniya in z ⁇ ne se ⁇ dechni ⁇ a 3 ⁇ s ⁇ eds ⁇ v ⁇ m ⁇ sn ⁇ vn ⁇ g ⁇ u ⁇ avlyaem ⁇ g ⁇ is ⁇ chni ⁇ a
- ⁇ e ⁇ m case ⁇ yavlyae ⁇ sya v ⁇ zm ⁇ zhn ⁇ s ⁇ d ⁇ lni ⁇ eln ⁇ is ⁇ us ⁇ venn ⁇ uvelichi ⁇ value ⁇ 2 ⁇ - 1 ta ⁇ z ⁇ ny ma ⁇ simaln ⁇ g ⁇ ⁇ s ⁇ a ⁇ chn ⁇ g ⁇ magni ⁇ s ⁇ i ⁇ tsi ⁇ nn ⁇ g ⁇ changes lineyn ⁇ g ⁇ ⁇ azme ⁇ a se ⁇ dechni ⁇ a 3 d ⁇ quantity q 2 of 1- 11 ⁇ a ⁇ ⁇ -reducing, ⁇ i e ⁇ m value na ⁇ yazhenn ⁇ s ⁇ i vs ⁇ m ⁇ ga ⁇ eln ⁇ g ⁇ ⁇ s ⁇ yann ⁇ g ⁇ magni ⁇ n ⁇ g ⁇ ⁇ lya ( ⁇ lya ⁇ dmagnichivaniya) and the magnitude of the magnetic field strength for the technical saturation of the material of the core 3, which is clearly shown in Fig. 6 of the
- Fig. 6 shows the “a” and “in” sys- tems of the magnetic circuit of the linear dimension of the 3-volt-free and non-volt-free
- P ⁇ myshlennaya ⁇ imenim ⁇ s ⁇ ⁇ a ⁇ im ⁇ b ⁇ az ⁇ m, ⁇ a ⁇ en ⁇ uem ⁇ e iz ⁇ b ⁇ e ⁇ enie m ⁇ zhe ⁇ by ⁇ is ⁇ lz ⁇ van ⁇ in ⁇ blas ⁇ i ele ⁇ e ⁇ ni ⁇ i and s ⁇ eds ⁇ v av ⁇ ma ⁇ i ⁇ i, na ⁇ ime ⁇ in ⁇ aches ⁇ ve zada ⁇ chi ⁇ a ⁇ eguli ⁇ uemy ⁇ ⁇ e ⁇ emescheny for ⁇ etsizi ⁇ nn ⁇ g ⁇ ⁇ zitsi ⁇ ni ⁇ vaniya is ⁇ lni ⁇ elny ⁇ elemen ⁇ v ⁇ ib ⁇ v, machinery and me ⁇ anizm ⁇ v.
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- General Electrical Machinery Utilizing Piezoelectricity, Electrostriction Or Magnetostriction (AREA)
- Nitrogen And Oxygen Or Sulfur-Condensed Heterocyclic Ring Systems (AREA)
Abstract
L'invention relève de l'électrotechnique et des moyens d'automatisation et peut être utilisée en tant que dispositif de réglage de déplacements contrôlés; elle concerne une méthode de commande d'un transducteur magnéto-mécanique, ce dernier comprenant un système magnétique, un noyau N (3) fait d'un matériau magnétostrictif, et un actionneur A (4). La méthode faisant l'objet de la présente invention repose sur les opérations suivantes: on modifie la position du centre d'inertie de A (4) grâce à la création d'un champ magnétique principal dans la zone de N (3); on modifie au moins une fois l'intensité du champ magnétique principal dans des limites comprises entre zéro et une valeur assurant la magnétostriction de la saturation technique du matériau dont est fait N (3) dans la direction du champ magnétique principal; et on maintient dans le temps la position prédéterminée du centre d'inertie de A (4). On crée préalablement dans la zone de N (3) un champ magnétique permanent et auxiliaire dont la valeur d'intensité est inférieure à celle du champ magnétique assurant la saturation technique du matériau de N (3) dans la direction du champ magnétique auxiliaire. Le champ magnétique principal ainsi créé consiste en des impulsions de champ magnétique principal qui ne se chevauchent pas dans le temps, les projections des vecteurs desdites impulsions sur l'axe de N (3), qui coïncide avec la direction de déplacement de A (4), étant orientées dans des directions opposées. On maintient ensuite dans le temps les positions prédéterminées du centre d'inertie de A (4) lorsque la tension du champ magnétique principal est nulle, ceci pendant une période comprise entre les impulsions susmentionnées du champ magnétique principal, et dans les limites de la valeur Δ2L1xmax du changement magnétostrictif résiduel maximal de la dimension linéaire de N (3), ledit changement étant limité par la valeur de l'intensité du champ magnétique auxiliaire.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
RU96121974/25A RU2102830C1 (ru) | 1996-11-14 | 1996-11-14 | Способ управления магнитомеханическим преобразователем |
RU96121974 | 1996-11-14 |
Publications (1)
Publication Number | Publication Date |
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WO1998021762A1 true WO1998021762A1 (fr) | 1998-05-22 |
Family
ID=20187285
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/RU1997/000321 WO1998021762A1 (fr) | 1996-11-14 | 1997-10-10 | Methode de commande d'un transducteur magneto-mecanique |
Country Status (2)
Country | Link |
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RU (1) | RU2102830C1 (fr) |
WO (1) | WO1998021762A1 (fr) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2018167242A3 (fr) * | 2017-03-15 | 2018-12-27 | Eto Magnetic Gmbh | Dispositif d'actionnement et procédé de fonctionnement d'un dispositif d'actionnement |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
SU765913A1 (ru) * | 1978-11-20 | 1980-09-23 | Государственный Ордена Октябрьской Революции Научно-Исследовательский И Проектный Институт Редкометаллической Промышленности "Гиредмет" | Магнитомеханический преобразователь |
EP0391880A2 (fr) * | 1989-04-05 | 1990-10-10 | Fisher Controls International, Inc. | Mesure et commande du mouvement d'un transducteur magnétostrictif |
EP0443873A1 (fr) * | 1990-02-23 | 1991-08-28 | Kabushiki Kaisha Toshiba | Organe d'actionnement magnétostrictif |
US5451821A (en) * | 1993-08-30 | 1995-09-19 | The United States Of America As Represented By The Secretary Of The Navy | Magnetostrictive actuator with auxiliary leakage reducing magnetic bias |
-
1996
- 1996-11-14 RU RU96121974/25A patent/RU2102830C1/ru not_active IP Right Cessation
-
1997
- 1997-10-10 WO PCT/RU1997/000321 patent/WO1998021762A1/fr active Application Filing
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
SU765913A1 (ru) * | 1978-11-20 | 1980-09-23 | Государственный Ордена Октябрьской Революции Научно-Исследовательский И Проектный Институт Редкометаллической Промышленности "Гиредмет" | Магнитомеханический преобразователь |
EP0391880A2 (fr) * | 1989-04-05 | 1990-10-10 | Fisher Controls International, Inc. | Mesure et commande du mouvement d'un transducteur magnétostrictif |
EP0443873A1 (fr) * | 1990-02-23 | 1991-08-28 | Kabushiki Kaisha Toshiba | Organe d'actionnement magnétostrictif |
US5451821A (en) * | 1993-08-30 | 1995-09-19 | The United States Of America As Represented By The Secretary Of The Navy | Magnetostrictive actuator with auxiliary leakage reducing magnetic bias |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2018167242A3 (fr) * | 2017-03-15 | 2018-12-27 | Eto Magnetic Gmbh | Dispositif d'actionnement et procédé de fonctionnement d'un dispositif d'actionnement |
US11569436B2 (en) | 2017-03-15 | 2023-01-31 | Eto Magnetic Gmbh | Actuator device and method for operating an actuator device |
Also Published As
Publication number | Publication date |
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RU2102830C1 (ru) | 1998-01-20 |
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