TW200424545A - Azimuth measuring method and apparatus, and recording medium having stored the azimuth measuring method - Google Patents
Azimuth measuring method and apparatus, and recording medium having stored the azimuth measuring method Download PDFInfo
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- TW200424545A TW200424545A TW093107202A TW93107202A TW200424545A TW 200424545 A TW200424545 A TW 200424545A TW 093107202 A TW093107202 A TW 093107202A TW 93107202 A TW93107202 A TW 93107202A TW 200424545 A TW200424545 A TW 200424545A
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- 238000001514 detection method Methods 0.000 claims description 126
- 238000005259 measurement Methods 0.000 claims description 32
- 230000006870 function Effects 0.000 claims description 6
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- 238000000691 measurement method Methods 0.000 claims 2
- 230000005389 magnetism Effects 0.000 abstract 2
- 238000006243 chemical reaction Methods 0.000 description 10
- 230000005358 geomagnetic field Effects 0.000 description 10
- 238000010586 diagram Methods 0.000 description 8
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- 230000035945 sensitivity Effects 0.000 description 3
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- 101100087530 Caenorhabditis elegans rom-1 gene Proteins 0.000 description 1
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Classifications
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- G—PHYSICS
- G04—HOROLOGY
- G04B—MECHANICALLY-DRIVEN CLOCKS OR WATCHES; MECHANICAL PARTS OF CLOCKS OR WATCHES IN GENERAL; TIME PIECES USING THE POSITION OF THE SUN, MOON OR STARS
- G04B47/00—Time-pieces combined with other articles which do not interfere with the running or the time-keeping of the time-piece
- G04B47/06—Time-pieces combined with other articles which do not interfere with the running or the time-keeping of the time-piece with attached measuring instruments, e.g. pedometer, barometer, thermometer or compass
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01C—MEASURING DISTANCES, LEVELS OR BEARINGS; SURVEYING; NAVIGATION; GYROSCOPIC INSTRUMENTS; PHOTOGRAMMETRY OR VIDEOGRAMMETRY
- G01C17/00—Compasses; Devices for ascertaining true or magnetic north for navigation or surveying purposes
- G01C17/02—Magnetic compasses
- G01C17/28—Electromagnetic compasses
-
- G—PHYSICS
- G04—HOROLOGY
- G04B—MECHANICALLY-DRIVEN CLOCKS OR WATCHES; MECHANICAL PARTS OF CLOCKS OR WATCHES IN GENERAL; TIME PIECES USING THE POSITION OF THE SUN, MOON OR STARS
- G04B47/00—Time-pieces combined with other articles which do not interfere with the running or the time-keeping of the time-piece
- G04B47/06—Time-pieces combined with other articles which do not interfere with the running or the time-keeping of the time-piece with attached measuring instruments, e.g. pedometer, barometer, thermometer or compass
- G04B47/065—Time-pieces combined with other articles which do not interfere with the running or the time-keeping of the time-piece with attached measuring instruments, e.g. pedometer, barometer, thermometer or compass with a compass
-
- G—PHYSICS
- G04—HOROLOGY
- G04R—RADIO-CONTROLLED TIME-PIECES
- G04R20/00—Setting the time according to the time information carried or implied by the radio signal
- G04R20/08—Setting the time according to the time information carried or implied by the radio signal the radio signal being broadcast from a long-wave call sign, e.g. DCF77, JJY40, JJY60, MSF60 or WWVB
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- G—PHYSICS
- G04—HOROLOGY
- G04R—RADIO-CONTROLLED TIME-PIECES
- G04R60/00—Constructional details
- G04R60/06—Antennas attached to or integrated in clock or watch bodies
- G04R60/10—Antennas attached to or integrated in clock or watch bodies inside cases
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- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Electromagnetism (AREA)
- Measuring Magnetic Variables (AREA)
- Electric Clocks (AREA)
Abstract
Description
200424545 玖、發明說明: (一) 發明所屬之技術領域 本發明係關於方位計測裝置、方位計測方法及記錄媒體。 (二) 先前技術 近年來’具有依據檢測地磁之方向而計測方位的方位感 測器之電子機器甚爲普及。於此種電子機器所具有方位感 測器,一般乃一方向具磁場感度的2個棒狀磁性感測器(磁 場檢測元件),安裝有垂直配置的模組,根據由此等磁性感 測器所檢測2方向磁力來計測方位。 又於如此的方位感測器,配置偏壓線圈於磁性感測器之 上方,用施加偏壓磁場在磁性感測器狀態檢測地磁的方法 爲眾所周知。此施加偏壓磁場係緩和對測定的磁性感測器 之磁滯影響,爲了正確地檢測地磁之方向或大小。 然而,在上述先前的方位感測器,係預先配置2個磁性 感測器爲垂直的模組,於工廠出貨時已安裝於電子機器, 但實際上,欲預先確定地互相垂直配置此等2個磁性感測 器於模組事態,每每有困難致有不能確定地計測方位的問 題。爲了避免此問題就在工廠出貨時,有所謂的須要實行 調整模組內磁性感測器配置的作業問題。再者,2個磁性 感測器因配置爲互相於垂直方向,所以有磁性感測器之安 裝效率不好的問題。 (三) 發明內容 於是,本發明,於具備方位感測器(方位計測裝置)的電 子機器,將互相獨立的2個磁性感測器,作成磁場檢測方 、90 200424545 向交叉的角度爲90度以上180度以下,或大於〇度 度以下來配置。 依此,可以提高磁性感測器之配置自由度。又由於 磁性感測器之配置狀況算出方位,變成可檢測確定的戈 (四)實施方式 以下,參照圖式詳細說明本發明之實施形態。本實 形態,係對本發明適用於腕帶型之電波鐘錶狀況說明 本發明之適用並不限定於該實施形態。 首先,說明於本實施形態的構成。 第1圖,表示於本發明實施形態的電波鐘錶1 0 0槪 視圖。又第2圖表示第1圖之II-II部剖面圖。如第2 示在電波鐘錶1 00,具備有收容鐘錶模組1在內部作 殻體之鐘錶外殻2,鐘錶外殼2之上部中央藉由襯墊 裝鐘錶玻璃3。鐘錶模組1所具備的框狀構件5,係配 其上部頂接在鐘錶玻璃3。再者,此鐘錶模組2之下 由防水環7安裝背蓋6,設緩衝構件8於鐘錶模組1 蓋6之間。又此鐘錶外殻2之上部外周設有外蓋9。 鐘錶外殻2,藉由帶軸2Α安裝鐘錶帶24。 鐘錶模組1具有類比功能者。如第2圖所示鐘錶模 ,具備有作爲中間構件的上部殼1 0及下部殻1 1,配 字盤12在上部殼10之上面,其文字盤12之上面配置 狀構件5。又爲框狀構件5之下方,在具有預先規定 的上部殻1 〇與下部殼1 1之間,配置有作電子基板之 基板1 3。鐘錶模組1,係成安裝此等文字盤1 2、上部 因應 •位。 施之 ,但 略平 圖所 爲外 4組 置爲 面藉 與背 再於 組1 置文 有框 間隔 電路 殼10 -6- 200424545 、電路基板1 3、及下部殼1 1於鐘錶外殼2之中框4構造。 又,上部殻1 〇具備有類比指針機構1 5、下部殻1 1,例 如組裝有爲了類比指針機構1 5等動作用之電池(省略圖示)。 再者,在上部殻1 〇具有天線3 0。 天線3 0係卷繞在以電波所磁化的磁性體3 1之一部分, 具有根據磁性體3 1產生的磁場大小流電流的導體3 4等。 磁性體3 1,具有由捕捉時刻資訊電波的電波捕捉部3 2 ,對電波捕捉部32獨立形成,予以卷繞導體34的天線本 體部3 3。 電波捕捉部3 2用肥粒鐵等構成,沿上部殻1 0彎曲成帶 狀配置在上部殻1 〇。電波捕捉部3 2,設於夾持天線本體部 3 3互相相對的位置,例如3點之位置與9點之位置,於天 線本體部3 3之各端部連結電波捕捉部3 2及天線本體部3 3。 天線本體部3 3,設成可連結於電波捕捉部3 2,其兩端部 支撐於配置電波捕捉部3 2的上部殼1 0。 又,在天線本體部3 3,例如卷繞有銅線等導體34爲線 圈狀,以電波磁化天線本體部3 3,伴隨在所磁化天線本體 部33產生磁場大小之電流就流於導體34。 又,對應上部殻1 0之6點鐘地方,具備方位感測器1 1 2 。方位感測器1 1 2,由2個棒狀之磁場檢測元件(磁性感測 器)X、Y,及偏壓線圈C所構成。磁場檢測元件X及磁場 檢測元件Y,使對應各個磁性檢測方向的直線Lx、Ly,成 規定之角度Φ地配置在電路基板1 3上。具體的係配置成磁性 檢測方向交叉的角度Φ爲π /2以上7Γ以下,2等分角φ/2之 -7- 200424545 方向爲1 2點方向。(或者,亦可配置成磁性檢測方向交叉 的角度Φ大於Οττ /2以下,2等分角φ/2之方向爲12點方 向。)方位感測器1 1 2之近旁,須避免配置容易受到磁場影 響的零件。尙方位感測器11 2在工廠出貨時安裝於電波鐘 錶 1 0 0。 偏壓線圈C如第2圖所示,對上述2等分角φ/2方向垂 直的方向卷繞於L字型心子之一部分(參照第1圖),心子 之一端固定在電路基板1 3上。 尙,使用於方位感測器1 1 2使用之磁場檢測元件,其驅 動方式爲相同,只要是一方向具磁場感度的元件(MR元件 、Μ I元件等)即可,亦可爲不同的磁場檢測元件X與磁場 檢測元件Υ之製造廠商。 類比指針機構1 5,具有從設於文字盤1 2的軸孔1 2 a延 伸其上方的指針軸1 7,及安裝在此指針軸1 7的時針、分 針等指針1 8,構成爲此指針1 8在文字盤1 2之上方運轉針 。在此,文字盤1 2與指針1 8於規定之地方,設予以受光 分別來自發光元件之光來發光的發光部19。 框狀構件5,例如由具光透射性的合成樹脂、特別是透 明的合成樹脂形成。此框狀構件5如第2圖所示,用頂接 於鐘錄玻璃3之周緣邰下邰及文字盤1 2 (上部殼1 0 )之周緣 部上面狀態,組裝於鐘錶外殼2之內周面。又此框狀構件 5之規定地方,例如第1圖所示對應丨2點及6點的地方, 配置有稱謂不可見光的紫外線發光元件2 0 1。配置紫外線 發光元件2 0 1的框狀構件5,爲亦兼備作保護構件或緩衝 -8- 200424545 構件功能的構件。紫外線發光元件20 1,例如由發光波長 254〜420nm(毫微米)之紫外線、或波長3 74〜3 89nm之紫外 線、理想爲3 6 5 n m附近之紫外線的紫外線燈或紫外線發光 二極體(LED)等構成。 又’此紫外線發光元件2 0 1如第2圖所示,由頂接紫外 線發光兀件2 0 1的接點構件2 1,及對此接點構件2 1賦予 能作賦予能構件的螺旋彈簧22構成的連接構件21 a支撐、 固疋。此接點構件2 1 ’具有對應於紫外線發光元件2 〇〗電 極端(省略圖示)的一對支持軸21a,其支持軸21a頂接在電 極端子。 接點構件2 1具導電性,其中央部係插入設於上部殼j 〇 的芽通孔10a內,同時通過設在文字盤12的穿通孔i2b、 及設在框狀構件5穿通孔5a,框狀構件5上端部配置成突 出於上方。頂接紫外線發光元件2〇丨於該突出的上端部(一 對支持軸2la)。在紫外線發光元件2〇1與鐘錶玻璃3之間 安裝有緩衝構件23。 螺fe彈簧2 2具導電性,插入設於上部殼丨〇的穿通孔i 〇 a 內,其下端部以彈性接觸於電路基板13所形成連接端子τ ,上贿部刼性接觸在接點構件2 }之下端部。並依此,螺旋 弓早簧22將接點構# 21向紫外線發光元件2〇ι側賦予能, 弓早性的支撐。又由接點構件2 2及螺旋彈簧22構成的連接 構件2 1 A,電氣的紫外線發光元件2 〇丨及電路基板丨3。 發光部1 9如第2圖所示,於文字盤i 2的規定地方,例 如作爲樹脂部’印刷部或塗裝部形成於標記部分或時字上 冬 200424545 面、或於類比指針機構1 5的指針1 8規定之地方。其發光 部1 9之上面用外敷層(省略圖示)所覆蓋保護爲理想。此等 發光部19’例如反應波長350〜420nm、或254〜365nm之 紫外線作有色發光,未照射紫外線的通常狀態時呈透明的 狀S?'者。亦即,藉由從紫外線發光元件2 0 1輸出的紫外線 、或具光透射性的框狀構件5反應所出射紫外線,發光部 作有色發光。200424545 (1) Description of the invention: (1) Technical field to which the invention belongs The present invention relates to a bearing measuring device, a bearing measuring method and a recording medium. (2) Prior art In recent years, electronic devices having an azimuth sensor that measures the azimuth based on the direction of the geomagnetism have become widespread. The azimuth sensor in such an electronic device is generally two rod-shaped magnetic sensors (magnetic field detection elements) with magnetic field sensitivity in one direction, and a vertically arranged module is installed. According to the magnetic sensors The azimuth is measured by the detected magnetic force in two directions. Further, in such an orientation sensor, a method is known in which a bias coil is disposed above the magnetic sensor and a bias magnetic field is applied to detect the geomagnetism in the state of the magnetic sensor. The bias magnetic field is applied to alleviate the hysteresis effect on the measured magnetic sensor, in order to detect the direction or magnitude of the geomagnetism correctly. However, in the above-mentioned prior orientation sensors, two magnetic sensors were arranged in a vertical module in advance, and they were already installed in an electronic device at the time of shipment from the factory. Two magnetic sensors are in the module state, and often there is a problem that the position cannot be measured with certainty. In order to avoid this problem, there is a so-called operation problem that requires adjustment of the magnetic sensor configuration in the module when it is shipped from the factory. Furthermore, since the two magnetic sensors are arranged perpendicular to each other, there is a problem that the mounting efficiency of the magnetic sensor is not good. (3) Summary of the Invention Therefore, in the present invention, in an electronic device provided with an orientation sensor (azimuth measuring device), two magnetic sensors that are independent of each other are used to form a magnetic field detection angle. Above 180 degrees or less, or above 0 degrees. According to this, the degree of freedom of configuration of the magnetic sensor can be improved. In addition, the orientation of the magnetic sensor is calculated to determine the orientation, and it becomes detectable. (4) Embodiments Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings. This embodiment is a description of the condition of the radio-controlled timepiece to which the present invention is applied to a wristband type. The application of the present invention is not limited to this embodiment. First, the structure of this embodiment will be described. FIG. 1 is a view of a radio-controlled timepiece 100 according to an embodiment of the present invention. Fig. 2 is a cross-sectional view of part II-II of Fig. 1. As shown in the second figure, the radio-controlled timepiece 100 includes a timepiece case 2 that houses the timepiece module 1 as a case inside, and a watch glass 3 is mounted on the center of the upper part of the timepiece case 2 through a gasket. The frame-shaped member 5 included in the timepiece module 1 is connected to the timepiece glass 3 at its upper portion. Furthermore, a back cover 6 is mounted under the watch module 2 by a waterproof ring 7, and a buffer member 8 is provided between the cover 6 of the watch module 1. An outer cover 9 is provided on the outer periphery of the upper part of the timepiece case 2. The watch case 2 is attached with a watch band 24 via a belt shaft 2A. The clock module 1 has an analog function. As shown in Fig. 2, the timepiece mold is provided with an upper case 10 and a lower case 11 as intermediate members. A dial 12 is disposed on the upper case 10, and a shape member 5 is disposed on the dial 12 of the dial. Further below the frame-like member 5, a substrate 13 serving as an electronic substrate is arranged between a predetermined upper case 10 and a lower case 11. The clock module 1 is to be fitted with these dials 1 2. The upper part corresponds to the • position. It is applied, but the outer plan is shown in the plan view, and the outer 4 groups are placed on the surface and the back. In group 1, there are framed circuit cases 10-6-200424545, circuit board 1 3, and lower case 1 1 on the watch case 2. Frame 4 structure. In addition, the upper case 10 is provided with an analog pointer mechanism 15 and the lower case 11, for example, a battery (not shown) for the analog pointer mechanism 15 and the like is assembled. The upper case 10 has an antenna 30. The antenna 30 is wound around a part of the magnetic body 31 which is magnetized by an electric wave, and has a conductor 34 which flows a current in accordance with the magnitude of the magnetic field generated by the magnetic body 31. The magnetic body 31 has an antenna body portion 3 3 formed by a radio wave capturing portion 3 2 that captures time information radio waves. The magnetic wave capturing portion 32 is formed independently and a conductor 34 is wound. The radio wave capturing portion 32 is made of ferrous iron or the like, and is bent along the upper shell 10 into a band shape and is arranged on the upper shell 10. The radio wave capturing section 32 is provided at a position where the antenna main body section 33 is opposed to each other, for example, at 3 o'clock and 9 o'clock, and the radio wave capturing section 32 and the antenna body are connected to each end of the antenna main body section 33. Department 3 3. The antenna body portion 33 is provided so as to be connectable to the radio wave capturing portion 32, and both end portions thereof are supported by the upper case 10 where the radio wave capturing portion 32 is arranged. In the antenna body portion 33, a conductor 34 such as a copper wire is wound in a coil shape. The antenna body portion 33 is magnetized by radio waves, and a current having a magnitude of a magnetic field generated in the magnetized antenna body portion 33 flows through the conductor 34. In addition, corresponding to the 6 o'clock o'clock position of the upper case 10, an orientation sensor 1 1 2 is provided. The azimuth sensor 1 1 2 is composed of two rod-shaped magnetic field detection elements (magnetic sensor) X, Y, and a bias coil C. The magnetic field detection element X and the magnetic field detection element Y are arranged on the circuit board 13 with the straight lines Lx and Ly corresponding to the respective magnetic detection directions at a predetermined angle Φ. The specific system is arranged such that the angle Φ crossing the magnetic detection direction is π / 2 or more and 7Γ or less, and the direction of the bisected angle φ / 2 -7- 200424545 is the direction of 12 points. (Alternatively, the angle at which the magnetic detection direction intersects Φ is greater than Οττ / 2, and the direction of the bisecting angle φ / 2 is 12 o'clock.) Near the azimuth sensor 1 1 2, you must avoid disposing it easily. Magnetic field affected parts.尙 Azimuth sensor 11 2 is attached to a radio-controlled timepiece 100 when it is shipped from the factory. As shown in FIG. 2, the bias coil C is wound around a part of the L-shaped core (see FIG. 1) in a direction perpendicular to the bisecting angle φ / 2 direction, and one end of the core is fixed on the circuit board 13. . Alas, the magnetic field detection element used in the orientation sensor 1 12 has the same driving method, as long as it is an element with magnetic field sensitivity in one direction (MR element, MI element, etc.), it can also be a different magnetic field. Manufacturers of detection element X and magnetic field detection element Υ. The analog pointer mechanism 15 includes a pointer shaft 17 extending from a shaft hole 1 2 a provided on the dial 12 and a pointer 18 such as an hour hand and a minute hand mounted on the pointer shaft 17. 1 8 Turn the needle over the dial 12. Here, the dial 12 and the pointer 18 are provided at predetermined positions, and a light-emitting portion 19 is provided which receives light and emits light from the light-emitting elements, respectively. The frame-like member 5 is made of, for example, a light-transmitting synthetic resin, particularly a transparent synthetic resin. As shown in FIG. 2, this frame-shaped member 5 is assembled on the inner periphery of the watch case 2 in a state of being attached to the peripheral edge 邰 of the clock recording glass 3 and the upper surface of the dial 12 (upper case 10). surface. In addition, in a predetermined place of the frame-like member 5, for example, in the places corresponding to 2 o'clock and 6 o'clock shown in FIG. 1, an ultraviolet light emitting element 21 of invisible light is arranged. The frame-shaped member 5 in which the ultraviolet light-emitting element 2 01 is arranged is a member that also serves as a protective member or a buffer member. The ultraviolet light-emitting element 201 is, for example, an ultraviolet light or an ultraviolet light-emitting diode (LED) having a wavelength of 254 to 420 nm (nm), or a wavelength of 3 74 to 3 89 nm, or an ultraviolet light near 3 6 5 nm. ) And so on. Also, as shown in FIG. 2, the ultraviolet light emitting element 2 01 is provided with a contact member 21 that is connected to the ultraviolet light emitting element 2 01 and a coil spring that can be used as an energizing member is provided to the contact member 21. The connecting member 21a constituted by 22 is supported and fixed. This contact member 2 1 ′ has a pair of supporting shafts 21a corresponding to the electric terminal (not shown) of the ultraviolet light-emitting element 20, and the supporting shaft 21a is abutted on the electric terminal. The contact member 21 is electrically conductive, and a central portion thereof is inserted into a bud through hole 10a provided in the upper case j 0, and at the same time passes through a through hole i2b provided in the dial 12 and a through hole 5a provided in the frame member 5, The upper end portion of the frame-like member 5 is arranged to protrude upward. The ultraviolet light emitting element 20 is attached to the protruding upper end portion (a pair of supporting shafts 2la). A buffer member 23 is mounted between the ultraviolet light emitting element 201 and the timepiece glass 3. The helical spring spring 22 is electrically conductive, and is inserted into the through-hole i 0a provided in the upper case. The lower end portion thereof elastically contacts the connection terminal τ formed by the circuit board 13. The upper bridging portion is in contact with the contact member. 2} lower end. In accordance with this, the spiral bow early spring 22 energizes the contact structure # 21 to the ultraviolet light emitting element 20 side, and the bow is supported early. Furthermore, a connection member 2 1 A composed of a contact member 22 and a coil spring 22, an electric ultraviolet light emitting element 2 0, and a circuit board 3. As shown in FIG. 2, the light-emitting portion 19 is formed at a predetermined place on the dial i 2, for example, it is formed as a resin portion, a printing portion or a coating portion, on a mark portion or a time character on the winter 200424545 surface, or on an analog pointer mechanism 1 5 Pointer 18 places required. The light-emitting portion 19 is preferably covered and protected with an overcoat layer (not shown). These light-emitting portions 19 'are, for example, colored ultraviolet light having a reaction wavelength of 350 to 420 nm, or 254 to 365 nm, and are transparent when they are not irradiated with ultraviolet light. In other words, the ultraviolet light emitted from the ultraviolet light emitting element 201 or the ultraviolet light emitted from the frame-like member 5 having a light transmissive reaction reacts, and the light emitting portion emits colored light.
又,於第1圖,表示了棒狀之磁場檢測元件X與磁場檢 測元件Y,近接於對應6點地方所配置狀況,但作第3圖 之變形例如電波鐘錶200所示,亦可以分別將各棒狀之磁 場檢測元件,使離開對應於磁性檢測方向的直線Lx、Ly 上來配置也可以。磁場檢測元件X,配置在對應電路基板 1 3 (參照第4圖)上的3點〜5點地方,磁場檢測元件Y,配 置在對應電路基板1 3上之7點〜9點地方。In FIG. 1, the rod-shaped magnetic field detection element X and the magnetic field detection element Y are arranged close to the corresponding six points. However, as a modification of FIG. 3, for example, as shown in the radio-controlled timepiece 200, it is also possible to separately Each of the rod-shaped magnetic field detection elements may be arranged away from the straight lines Lx and Ly corresponding to the magnetic detection direction. The magnetic field detection element X is arranged at 3 to 5 o'clock on the corresponding circuit board 13 (refer to FIG. 4), and the magnetic field detection element Y is arranged at 7 to 9 o'clock on the corresponding circuit board 13.
如第3圖,以離開配置磁場檢測元件X與磁場檢測元件 Y時,在磁場檢測元件X之上方,配置偏壓線圈Cx於垂直 磁場檢測元件X之磁性檢測方向的方向,磁場檢測元件Y 之上方,配置偏壓線圈Cy於垂直平行磁場檢測元件Y之 磁性檢測方向的方向。卷繞於偏壓線圈C X與C y的線圈爲 相同材質,卷繞的次數亦爲相同。磁場檢測元件X,配置在 對應電路基板1 3 (參照第4圖)上的3點〜5點地方,磁場 檢測元件Y,配置在對應電路基板1 3上的7點〜9點地方 。又偏壓線圈Cx、Cy,爲同樣構造而卷繞於L字型之磁性 心子之一部分,此磁性子心之一端固定於電路基板1 3上。 -10- 200424545 偏壓線圈Cx與Cy,分別配置在磁場檢測元件X與磁場檢 測元件Y的上部。 又,於第1圖,表示各磁場檢測元件之磁性檢測方向交 叉的角度Φ爲7Γ /2以上7Γ以下時(參照第5A圖),但於φ 爲大於0小於71 /2(參照第5B圖)時亦可以適用本發明。 再者,第1圖〜第4圖,係爲了施加相同偏壓磁場於磁 場檢測元件,表示配置了偏壓線圈C ; Cx、Cy的狀況,但 代替偏壓線圈予以配置永久磁鐵也可以。As shown in FIG. 3, when the magnetic field detection element X and the magnetic field detection element Y are disposed away from each other, a bias coil Cx is disposed above the magnetic field detection element X in the direction of the magnetic detection direction of the vertical magnetic field detection element X. Above, a bias coil Cy is arranged in the direction of the magnetic detection direction of the vertical parallel magnetic field detection element Y. The coils wound around the bias coils C X and C y are made of the same material, and the number of windings is also the same. The magnetic field detection element X is disposed at 3 to 5 o'clock on the corresponding circuit board 13 (see FIG. 4), and the magnetic field detection element Y is disposed at 7 o'clock to 9 o'clock on the corresponding circuit board 13. The bias coils Cx and Cy have the same structure and are wound around a part of an L-shaped magnetic core. One end of the magnetic core is fixed to the circuit board 13. -10- 200424545 Bias coils Cx and Cy are respectively arranged above the magnetic field detection element X and the magnetic field detection element Y. In Fig. 1, the angle at which the magnetic detection direction of each magnetic field detection element intersects is 7 Γ / 2 or more and 7 Γ or less (refer to Fig. 5A), but when φ is greater than 0 and less than 71/2 (refer to Fig. 5B). ) Can also be applied to the present invention. In addition, Figs. 1 to 4 show the state in which the bias coils C; Cx and Cy are arranged in order to apply the same bias magnetic field to the magnetic field detection element, but permanent magnets may be arranged instead of the bias coils.
<電波鐘錶之功能的構成>< Functional configuration of radio-controlled timepiece >
其次,參照第6圖及第7圖,說明關於電波鐘錶1 0 0之 功能的構成。第6圖係於本實施形態表示電波鐘錶1 0 0之 電路構成一例區塊圖。電波鐘錶1 〇 〇如第6圖所示具備: 控制部 1 01 ;輸入部 1 〇 2 ;顯示部 1 0 3 ; R A M ( R a n d 〇 ni A c c e s s Memory)104; ROM(Read Only Memory)105;接收控制部 1 0 6 ;時間碼變換部1 0 7 ;計時電路部1 0 8 ;振盪電路部1 0 9 及方位感測器1 1 〇所構成,除了振盪電路部1 09的各部係 以匯流條連接。又計時電路部1 〇 8連接振盪電路部1 0 9。 控制部 1〇1 具備 CPU(Central Processing Unit),讀出儲 存在ROM 1 05的各種程式擴展於RAM 1 04內,按照其等 之程式予以集中控制電波鐘錶1 〇 〇之各部。以下,詳細說 明依控制部1 〇 1的各種控制動作。 控制部1 0 1具備方位演算部1 〇 1 a,從來自方位感測器1 1 〇 所輸入資料,算出對規定之座標軸(磁場檢測元件X之檢測 方向、後述之X軸)地磁方向(北方向)之角度。又,控制部 -11- 200424545 1 ο l,根據由方位演算部1 〇1 a的算出結果,判定北方向是 否一致於1 2點方向,判定北方向爲一致於1 2點方向時, 點燈顯示部1 03之背照光(參照第1 1圖)。 又,控制部1 0 1,於緊接著方位計測及每一規定時間控 制接收控制部1 〇 6實行標準電波之接收處理,根據從時間 碼變換部1 〇 7輸入的標準時間碼,修正在計時電路部丨〇 8 所計時現在時刻資料。 <地磁方向之角度算出方法> 第8圖表示於二維的平面之地磁Η,與磁場檢測元件X 及Υ之磁性檢測方向關係圖。此二種的平面與鐘錶外殼2 之盤面平行,固定於電波鐘錶1 00的平面·。在以下,由磁 場檢測元件X的磁性檢測方向X、y之直線,與由磁場檢測 元件Y交叉磁性檢測方向之直線角度爲Φ。又由磁場檢測 元件X的磁性檢測方向爲X軸、由磁場檢測元件γ的磁性 檢測方向爲y軸。 本實施形態如第8圖所示,檢測地磁Η之方向爲從X軸 以反時鐘方向僅傾斜0弧度者,將此X軸之正區域作爲〇 弧度的反時鐘方向之旋轉角度0看成地磁Η之方向。又地 磁Η之大小爲H s。依第8圖地磁Η之X軸方向成分Η X (以下稱「X成分」。)、y軸方向之成分Hy(以下稱「y成 分」。)變成爲如以下之(1 )式及(2 )式。 [式1]Next, the functional configuration of the radio-controlled timepiece 100 will be described with reference to Figs. 6 and 7. Fig. 6 is a block diagram showing an example of a circuit configuration of a radio-controlled timepiece 100 according to this embodiment. The radio-controlled timepiece 1 00 is provided with a control unit 1 01; an input unit 102; a display unit 103; a RAM (R and Oni Access Memory) 104; a ROM (Read Only Memory) 105; The reception control unit 106 is composed of a time code conversion unit 107, a timing circuit unit 108, an oscillation circuit unit 109, and an orientation sensor 1110, except that each unit of the oscillation circuit unit 1009 is converged. Connection. The timing circuit section 108 is connected to the oscillation circuit section 109. The control section 101 is provided with a CPU (Central Processing Unit), reads out various programs stored in the ROM 105, and expands them into the RAM 104, and centrally controls each section of the radio-controlled timepiece 100 according to the programs. Hereinafter, various control operations by the control unit 101 will be described in detail. The control unit 101 includes an azimuth calculation unit 1 〇1 a, and calculates a geomagnetic direction (north) from a data input from the azimuth sensor 1 1 〇 with respect to a predetermined coordinate axis (a detection direction of a magnetic field detection element X and an X-axis described later). Direction). In addition, the control unit-11- 200424545 1 ο l determines whether the north direction is consistent with the 12 o'clock direction based on the calculation result of the bearing calculation unit 1 〇1 a. When it is determined that the north direction is consistent with the 12 o'clock direction, the light is turned on. Backlight of display section 03 (see Figure 11). In addition, the control unit 101 performs a standard radio wave reception process immediately after the azimuth measurement and controls the reception control unit 10 every predetermined time. Based on the standard time code input from the time code conversion unit 107, the time is corrected. The current time data of the circuit section 丨 〇8. < Method for calculating angle of geomagnetic direction > Fig. 8 is a graph showing the relationship between the geomagnetic field 二维 on a two-dimensional plane and the magnetic detection directions of the magnetic field detection elements X and Υ. These two kinds of planes are parallel to the dial surface of the timepiece case 2, and are fixed to the plane of the radio-controlled timepiece 100. In the following, a straight line of the magnetic detection directions X and y by the magnetic field detection element X and a straight line crossing the magnetic detection direction by the magnetic field detection element Y is Φ. The magnetic detection direction by the magnetic field detection element X is the X axis, and the magnetic detection direction by the magnetic field detection element γ is the y axis. In this embodiment, as shown in FIG. 8, the direction of the detection of the geomagnetic Η is only inclined by 0 radians from the X axis in the counterclockwise direction, and the positive area of the X axis is regarded as the rotation angle 0 of the counterclockwise direction of 0 radians as the geomagnetic field. The direction of Η. The size of the geomagnetic field is H s. The X-axis component Η X (hereinafter referred to as the “X component”) and the Hy component in the y-axis direction (hereinafter referred to as the “y component”) according to FIG. 8 are as follows: (1) and (2) )formula. [Formula 1]
Hx = Hsxcos θ (1)Hx = Hsxcos θ (1)
Hy = Hsxcos(())-0) (2) -12- 200424545 檢測地磁Η的角度0,從(1)式及(2)式例如算出如以卞 依加法定理成爲 )=cos+cos0 +sin#sin0 、 H y / Η x = c o s φ + s i η φ t a η 0 ,因而檢測地磁Η的角度(9輪 矣、成 爲如(3 )式。 [式2] 0 =arctani-^-^l (3)Hy = Hsxcos (())-0) (2) -12- 200424545 Detects the angle 0 of the geomagnetic radon. Calculate from the formulas (1) and (2), for example, using the Zijia law) = cos + cos0 + sin # sin0 、 H y / Η x = cos φ + si η φ ta η 0, so the angle of the geomagnetic Η is detected (9 rounds 矣, which becomes the formula (3). [Formula 2] 0 = arctani-^-^ l ( 3)
[Hx sin φ sin φ J 又,由於爲 sin(|) = cos((|)-7r/2)、cos(|) = -sin((j)-7r/2),(3) 式可換寫爲如以下之(4)式 [式3] Θ =a r c t a η[Hx sin φ sin φ J, since sin (|) = cos ((|) -7r / 2), cos (|) = -sin ((j) -7r / 2), (3) is interchangeable It is written as the following (4) Formula [Formula 3] Θ = arcta η
Hy cos x Hx L 2」 + tan φ — (4) 於磁場檢測元件X及磁場檢測元件γ施加同樣之偏壓磁 場時,如第9A圖、第9B圖所示,磁場檢測元件X與磁場 檢測元件Y之各磁性檢測方向,於交叉角度φ之2等分角 φ/2之方向施加根據偏壓線圈C所誘導的偏壓磁場Vi。第 9A圖表示φ爲ΤΓ/2以上π以下之狀況,第9B圖表示φ爲 0以上7Γ /2以下狀況。 第1 0圖表示施加偏壓磁場V i的方向,與磁性檢測方向 之關係。以偏壓磁場V丨之大小爲B ’則偏壓磁場V i之χ 成分Β X、y成分B y係如(5)式變成相同之値。 [式4]Hy cos x Hx L 2 ″ + tan φ — (4) When the same bias magnetic field is applied to the magnetic field detection element X and the magnetic field detection element γ, as shown in FIGS. 9A and 9B, the magnetic field detection element X and the magnetic field are detected. In each of the magnetic detection directions of the element Y, a bias magnetic field Vi induced by the bias coil C is applied in a direction in which the crossing angle φ is equal to two equal angles φ / 2. FIG. 9A shows a situation where φ is greater than τΓ / 2 and less than π, and FIG. 9B shows a situation where φ is greater than 0 and 7Γ / 2. Fig. 10 shows the relationship between the direction in which the bias magnetic field V i is applied and the magnetic detection direction. When the magnitude of the bias magnetic field V 丨 is B ', the χ component B X and the y component B y of the bias magnetic field V i become the same as in Equation (5). [Formula 4]
B c o s — 2 -13- 200424545 反之,各磁場檢測元件須要的偏壓磁場之大金爲^ =B c o s — 2 -13- 200424545 Conversely, the amount of bias magnetic field required by each magnetic field detection element is ^ =
Bx = By),其應予施加磁場大小之β,變成如以了之(6)式 [式5] (6) β sec — 2 實際由磁場檢測元件X所檢測磁場’因係地磁之Χ成本 Η X與偏壓磁場之X成分/3之和,所以由於從檢測的磁場減 掉偏壓磁場之大小/5 ’予以算出地磁之χ成分Ηχ °同樣實 際由磁場檢測元件γ檢測的磁場,因爲地磁之y成分Hy 與偏壓磁場之y成分石之和,所以由於從檢測的磁場減掉 偏壓磁場之大小yS算出地磁之y成分H y ° 回到第6圖輸入部1 0 2,爲了對電波鐘錶1 〇 〇實行各種 功能用方位計測鈕l〇2a(參照第1圖)等鈕構成,將由按壓 此等之鈕的操作信號輸出於控制部1 〇 1。方位計測鈕1 〇2a 係爲指示開始方位計測用之鈕。 顯示部103,由顯示器部103a、文字盤12、背照光部l〇3b 等所構成。顯示器部1 0 3 a,由小型液晶顯示等之顯示裝置 來構成。隨著從控制部1 〇 1輸入的顯示信號,實行所要的 顯不處理。背照光部 103b,由 LED(Light Emitting Diode) 等構成,配置在顯示器部1 〇 3 a或文字盤1 2之背面。背照 光部1 〇 3 b,隨著從控制部1 0 1輸入的控制信號,對顯示器 部1 0 3 a或文字盤1 2照射光。 RAM 1 04 ’由控制部1 0 1實行的各種程式擴展於程式儲 存區域,同時以輸入部1 0 2輸入的輸入指示、輸入資料、 由貫fr上述程式產生的處理結果等資料暫時儲存在工作記 -1 ‘ 200424545 憶體。 R Ο Μ 1 5,係儲存有關控制電波鐘錶1 〇 〇的系統程式或應 用程式及實行此等程式時所利用的資料等。例如R0M 1 〇5 ’係儲存爲了實行方位計測用之方位計測處理程式(參照第 1 1 圖)。 接收控制部1 0 6,係截割天線所接收長波標準電波不要 的頻率成分,取出適用的頻率信號變換爲對應頻率信號的 號輸出。 計時電路部1 0 8,予以計數從振盪電路部1 0 9輸入的信 號,獲得現在時刻資料等。然後輸出該現在時刻資料於控 制部1 0 1。振盪電路部1 09係經常輸出一定頻率信號的電 路。 時間碼變換部1 0 7,根據從接收控制部1 〇 6輸出的信號 ’生成包含標準時刻碼、積累日碼及星期碼等之鐘錶功能 必要的資料之標準時間碼來輸出於控制部1 0 1。 方位感測器部1 1 0如第7圖所示,由驅動電路1 1 1 '方 位感測器1 1 2、放大部1 1 3、A/D變換電路1 1 4等構成。 驅動電路η 1,依照從控制部1 〇 1輸入的控制信號驅動 方位感測器1 1 2。 方位感測器1 1 2如第9 Α圖、第9Β圖所示,由2個磁場 檢測元件X、Y及偏壓線圈C構成。磁場檢測元件X檢測 磁場X成分之値,將檢測結果作爲類比方位信號輸出於放 大部1 1 3。磁場檢測元件Y檢測磁場y成分之値,將檢測 結果作爲方位信號輸出於放大部1 1 3。 -15- 200424545 放大部1 1 3,係放大從方位感測器1 1 2輸入的類比方位 信號,輸出於A/D變換電路1 14。 A/D變換電路114,數位變換從放大部113輸入的方位信 號,輸出於方位演算部1 0 1 a。 其次,說明於本實施形態的動作。 參照第1 1圖之流程圖,說明於電波鐘錶1 〇〇實行的方位 計測處理 。 由於按壓方位計測鈕l〇2a,指示方位計測(步驟S 1 ;是) 時由驅動電路1 1 1驅動方位感測器1 1 2,由於流電流在偏 壓線圈C,施加偏壓磁場於磁場檢測元件X、Y(步驟S 2)。 接著,由磁場檢測元件X檢測磁場之X成分(步驟S3), 由磁場檢測元件Y檢測磁場之y成分(步驟s 4)。接著於方 位演算部1 〇 1 a,由於從檢測磁場之X成分減掉偏壓磁場/3 算出地磁之X成分Hx,由於從檢測磁場之y成分減掉偏壓 磁場/3,算出地磁之y成分Hy。然後,由於代入地磁之X 成分Hx及y成分Hy於(4)式右式,算出地磁之方向,亦即 北方向之角度0 (步驟S5)。 算出了北方向之角度Θ ,就判定此角度Θ是否相等於規 定値(步驟S6)。在此所謂的規定値,係對X軸的12點方向 之角度爲Φ/2。於步驟S6不是0 =φ/2時(步驟S6 ;否),回 到步驟S 3。裝有電波鐘錶1 〇〇的使用者,由於改變腕或身 體的方向,改變電波鐘錶1 〇〇之方向,於控制部1 〇 1因應 電波鐘錶1〇〇之方向,反覆從步驟S3至步驟S6之處理。 於步驟S6成爲(9 =φ/2,12點方向一致於北方向時(步驟 200424545 S6 ;是),結束施加偏壓磁場(步驟S 7),點燈背照光部 (步驟S 8 )。 接著,由接收控制部106,接收時刻資訊(步驟S 9) 據其接收的時刻資訊修正現在時刻(步驟S 1 0 ),結束本 計測處理 。 如此在方位計測後接收時刻資訊來修正現在時刻, 加於方位計測時的偏壓磁場,由於給與影響鐘錶電路 部分有對時刻產生誤差的可能性。因而,第1 1圖之流 爲在方位計測後爲了顯示更正確的時刻,使於方位計 作成也可以接收時刻資訊。 又,第1 1圖之流程圖1 2點方向一致在北方向時, 點燈背照光部1 〇3b來報知,但報知手段並不限定於此 如,亦可作成以聲音來報知。 如以上,依本實施形態之電波鐘錶100,由於將互 立的磁場檢測元件X、γ,作成爲可配置於互相不同的 檢測方向向自由的方向位置,特別是安裝於小型電子 時可提高配置之自由度,同時可提高磁場檢測元件之 效率。又由於因應於磁場檢測元件之配置狀況算出方 變成可正確地檢測方位,同時變成不要先前所實施的 磁場檢測元件之配置作業。 再者,將磁場檢測元件X與磁場檢測元件Y,由於 成所檢測磁場之方向交叉的角度Φ爲7Γ 72以上或7Γ /2 ,所以與如先前固定Φ爲7Γ /2時比較可提高於製品安 配置自由度,同時可提高磁場檢測元件之安裝效率。 103b ,根 方位 係施 之一 程圖 測後 由於 ,例 相獨 磁性 機器 安裝 位, 調整 配置 以下 裝的 -17- 200424545 又,在步驟S 3至步驟S 6係1 2點方向之角度φ / 2作規定 値’由於算出的北方向之角度Θ是否與12點方向之角度 Φ / 2相等來決定方位,但從算出的角度β算出地磁η之大 小H s,以地磁Η之大小H s最成大的地磁η之方位定爲北 方向,將此北方向作成輸出也可以。 在求出地磁Η之大小H s,例如將在上述算出的角度$及 地磁之X成分Η X,代入(1 )式即可。亦即依(丨)式地磁η之 大小,成爲 Hs = Hxxsec<9。 又’由於將方位計測結果以點燈背照光或聲音來報知, 不必要新設置爲了報知計測結果之特別的手段,可予以抑 制電波鐘錶1 〇 〇之製造成本。 <變形例> 第1 1圖所示流程圖,係表示1 2點方向一致於北方向時 報知的狀況,但以下表示通知1 2點方向所示方位時之動作 。作如此動作之一例參照第1 2圖之流程圖,說明於電波鐘 錶1 〇〇所實行方位計測處理②。 由於按壓方位計測鈕1 〇2a,指示方位計測(步驟S丨丨;是) 時以驅動電路1 1 1驅動方位感測器1 1 2,由於電流流於偏 壓線圈C施加偏壓磁場在磁場檢測元件X、γ(步驟s】 接著,由磁場檢測元件X檢測磁場之x成分(步驟S 1 3 ) ,並由磁場檢測元件Y檢測磁場之y成分(步驟S 1 4 ),接 著於方位演算部1 〇 1 a根據在步驟S 1 3及步驟s 1 4檢測的磁 場,算出北方向之角度0 〇 (步驟S 1 5)。 算出了北方向之角度0 〇,就判定此角度0 〇是否等於規 -18- 200424545 定値φ/2 (步驟S16)。於步驟S16不是0 〇 = φ/2時(步驟si6 •’否)回到步驟S 1 3。裝著有電波鐘錶1 〇〇的使用者,由於 改變腕或身體之方向來改變電波鐘錶1 00的方向,另於控 制部1 0 1則因應電波鐘錶1 〇 0的方向,反覆從步驟S 1 3至 步驟S16之處理。 於步驟S16成爲0 〇 = φ/2,如第13Α圖所示12點方向一致 於北方向時(步驟S16 ;是),點燈背照光部l〇3b (步驟Sl7)。 例如’此時觀測者之身體向北時,改變方向爲目的的進 行方向後始實行其次之步驟。 背照光部l〇3b之點燈後,由再度按壓方位計測鈕1〇2a ’指示了方位計測(步驟S 1 8 ;是)就由磁場檢測元件X檢 測磁場之X成分(步驟S 1 9),並由磁場檢測元件γ檢測磁 場之y成分(步驟S20)。接著於方位演算部l〇la,根據在 步驟S 1 8及步驟S 1 9檢測的磁場,算出北方向的角度0 i (步驟S 2 1)。 算出了北方向之角度Θ i就結束施加偏壓磁場(步驟S 22) ’由在步驟S15算出的角度0 G(0 α = φ/2),與在步驟S2算出 的0 1之差0 0 !,予以算出12點方向之方位(步驟S 23)。 當檢測1 2點方向之方位.時,由於其所檢測方位就顯示在 顯示器部103a來通知(步驟S24),結束本方位計測處理 。 例如弟13B圖所不,爲0〇-01 = φ/ 2- 0ι = -7τ/4時,12點 向之方位係成北東。又如第13C圖所示爲0 Q-0 1 = φ/ΐ-θ ^ + π /4時,1 2點方向之方位成北西。 如上所述,予觀測觀測者進行方向之方位。 -19- 200424545 又,步驟S 2 4,由於將1 2點方向之方位顯示在顯示部1 〇 3 a 來通知,但通知方法並不限定於此,例如用指針來通知也 可以。 依第1 2圖所示方位計測處理②,作爲表示電波鐘錶1 〇 〇 之規定地方的方位(1 2點方向之方位),因也可以通知北方 向以外之方位,所以可提高方位感測器之便利性。 依本發明,變成可將互相獨立的2個磁性感測器,配置 成磁場檢測方向交叉角度爲9 0度以上1 8 0度以下,或比0 度大9 0度以上,可以提高配置磁性感測器之自由度。 又由於依據磁性感測器之配置狀況來算出方位,變成可 以昇出正確的方位。 又’於本實施形態的記述內容,在不逸脫本發明之宗旨 範圍可予以適宜變更。 (五)圖式簡單說明 第1圖爲於本發明實施形態的電波鐘錶1 〇 〇槪略平視圖。 第2圖爲第1圖之π -!丨部剖面圖。 第3圖爲於本發明實施形態之變形例的電波鐘錶2 〇 〇槪 路平視圖。 第4圖爲第3圖之iv_IV部剖面圖。 第5 A圖爲表示使構成方位感測器1丨2的磁場檢測元件X 與磁場檢測元件Y交叉角度以9 0度以上1 8 0度以下時之配 置例圖。 第5 B圖爲表示使構成方位感測器1 1 2的磁場檢測元件X 與磁場檢測元件Υ交叉角度比〇度大9 0度以下時之配置列 -20- 200424545 圖。 第6圖爲表示電波鐘錶1 〇 〇之電路構成一例的區塊圖。 第7圖爲表示第6圖所示方位感測器1 1 〇之電路構成一 例的區塊圖。 第8圖爲表示地磁Η與磁場檢測方向之關係圖。 第9Α圖爲表示使磁場檢測元件X與磁場檢測元件γ交 叉的角度爲9 0度以上1 8 0度以下時之磁場檢測元件X、磁 場檢測元件Υ、偏壓線圈C的配置例圖。 第9 Β圖爲表示使磁場檢測元件X與磁場檢測元件γ交 叉的角度爲比0大9 0度以下時之磁場檢測元件X、磁場檢 測元件Υ、偏壓線圈C之配置例圖。 第1 〇圖爲表示施加偏壓磁場Β的方向,與磁場檢測方向 之關係圖。 第1 1圖爲表示於電波鐘錶1 0 0所實行方位計測處理①的 流程圖。 第1 2圖爲於本實施形態之變形例,表示依電波鐘錶1 〇 〇 所實行方位計測處理②的流程圖。 第1 3 Α圖爲於第1 2圖之方位計測處理②,在1 2點方向 一致於北方向時,表示磁場檢測方向與北方向(地磁方向) 及1 2點方向之關係圖。 第1 3 B圖爲於第1 2圖之方位計測處理②,在1 2點方向 之方位成爲北東時,表示磁場檢測方向與北方向(地磁方向) 及1 2點方向之關係圖。 第1 3 C圖爲於第1 2圖之方位計測處理②,在1 2點方向 -21- 200424545 之方位成爲北西時,表示磁場檢測方向與北方向(地磁方向) 及1 2點方向之關係圖。 主要部分之代表符號說明 B、/3 偏壓磁場之大小 V i 偏壓磁場 C ; Cx、Cy偏壓線圈 Η 地磁 Ηχ Hy Lx、Ly X、Y I θ 0〇、θ 10 1a 102a 1 03 103a 103b 106 1 07 108 110 111 地磁X軸方向之X成分 地磁y軸方向之y成分 磁性檢測方向 磁場檢測元件(磁性感測器) 磁性檢測方向交叉的角度 地磁Η檢測的角度 北方向之角度 方位演算部 方位計測鈕 顯示部 顯示器部 背照光部 接收控制部 時間碼變換部 計時電路部 方位感測器部 驅動電路 -22- 200424545 112 方位感測器(方位計測裝置) 1 1 3 放大部 114 A / D變換電路 -23-Bx = By), the β of the magnitude of the magnetic field to be applied becomes as follows: (6) Equation [Eq. 5] (6) β sec — 2 The magnetic field actually detected by the magnetic field detection element X is due to the cost of geomagnetism X Η The sum of X and the X component of the bias magnetic field / 3, so since the magnitude of the bias magnetic field is subtracted from the detected magnetic field / 5 'to calculate the χ component of the geomagnetism Η ° ° The magnetic field actually detected by the magnetic field detection element γ is The sum of the y component Hy of the geomagnetic field and the y component stone of the bias magnetic field, because the magnitude yS of the bias magnetic field is subtracted from the detected magnetic field, the y component H y of the geomagnetic field is calculated. Return to the input part 1 2 of FIG. 6 in order to The radio-controlled timepiece 100 is configured with buttons such as an azimuth measuring button 102a (refer to FIG. 1) for performing various functions, and an operation signal for pressing these buttons is output to the control unit 101. Bearing measurement button 1 〇 2a is a button for instructing the start of bearing measurement. The display unit 103 includes a display unit 103a, a dial 12, a backlight unit 103b, and the like. The display unit 10 3 a is constituted by a display device such as a small liquid crystal display. With the display signal input from the control unit 101, the desired display processing is performed. The backlight unit 103b is composed of an LED (Light Emitting Diode) or the like, and is arranged on the back of the display unit 103a or the dial 12. The backlight unit 103b is irradiated with light on the display unit 103a or the dial 12 in accordance with a control signal input from the control unit 101. RAM 1 04 'The various programs executed by the control section 101 are extended to the program storage area, and at the same time, data such as input instructions, input data, and processing results generated by the programs described above are temporarily stored in the work. Book-1 '200424545 Memory. R Ο Μ 1 5 is a system program or application program for controlling radio-controlled timepieces 1 00 and data used in the execution of such programs. For example, ROM 1 〇5 ′ is used to store an azimuth measurement processing program for performing azimuth measurement (refer to FIG. 11). The receiving control unit 106 cuts the frequency components that are not needed for the long-wave standard radio wave received by the antenna, takes out the applicable frequency signal, and converts it to the corresponding frequency signal and outputs it. The timing circuit section 108 counts signals input from the oscillation circuit section 109, and obtains current time data and the like. Then the current time data is output to the control unit 101. The oscillating circuit section 109 is a circuit that always outputs a certain frequency signal. The time code conversion unit 107 generates a standard time code including data necessary for clock functions such as a standard time code, an accumulated day code, and a week code based on a signal output from the reception control unit 106, and outputs the standard time code to the control unit 10. 1. As shown in FIG. 7, the orientation sensor unit 1 10 is composed of a drive circuit 1 1 1 ′, an orientation sensor 1 1 2, an amplifier unit 1 1 3, an A / D conversion circuit 1 1 4, and the like. The driving circuit η 1 drives the azimuth sensor 1 12 in accordance with a control signal input from the control section 101. As shown in Figs. 9A and 9B, the orientation sensor 1 1 2 is composed of two magnetic field detection elements X and Y and a bias coil C. The magnetic field detection element X detects the difference between the components of the magnetic field X, and outputs the detection result as an analog azimuth signal to the amplifier 1 1 3. The magnetic field detection element Y detects a component of the magnetic field y, and outputs the detection result as an azimuth signal to the amplifying section 1 1 3. -15- 200424545 The amplifying section 1 1 3 amplifies the analog azimuth signal input from the azimuth sensor 1 1 2 and outputs it to the A / D conversion circuit 1 14. The A / D conversion circuit 114 digitally converts the azimuth signal input from the amplifying section 113 and outputs it to the azimuth calculating section 1 0 1 a. Next, the operation in this embodiment will be described. Referring to the flowchart in FIG. 11, the azimuth measurement processing performed in the radio-controlled timepiece 100 will be described. Since the orientation measurement button 102a is pressed, the orientation sensor 1 1 1 is driven by the drive circuit 1 1 1 when the orientation measurement is instructed (step S 1; Yes), because a current flows in the bias coil C, a bias magnetic field is applied to the magnetic field. The detection elements X, Y are detected (step S 2). Next, the X component of the magnetic field is detected by the magnetic field detection element X (step S3), and the y component of the magnetic field is detected by the magnetic field detection element Y (step s4). Next, in the azimuth calculation unit 10a, the X component Hx of the geomagnetism is calculated by subtracting the bias magnetic field / 3 from the X component of the detection magnetic field, and the y of the geomagnetic field is calculated by subtracting the bias magnetic field / 3 from the y component of the detection magnetic field. Ingredient Hy. Then, since the X component Hx and the y component Hy of the geomagnetism are substituted into the right expression of the formula (4), the direction of the geomagnetism, that is, the angle 0 in the north direction is calculated (step S5). After the angle Θ in the north direction is calculated, it is determined whether the angle Θ is equal to the predetermined value 値 (step S6). Here, the so-called regulation 値 means that the angle with respect to the 12 o'clock direction of the X axis is Φ / 2. When step S6 is not 0 = φ / 2 (step S6; No), the process returns to step S3. The user equipped with the radio-controlled timepiece 100 has to change the direction of the wrist or body, and change the direction of the radio-controlled timepiece 100. The control unit 100 responds to the direction of the radio-controlled timepiece 100 repeatedly from step S3 to step S6. Its processing. When step S6 becomes (9 = φ / 2, the 12 o'clock direction coincides with the north direction (step 200424545 S6; YES), the application of the bias magnetic field is ended (step S 7), and the backlight portion is turned on (step S 8). The reception control unit 106 receives the time information (step S 9), corrects the current time based on the received time information (step S 10), and ends the measurement process. In this way, the time information is received to correct the current time after the bearing measurement, and The bias magnetic field during the azimuth measurement may affect the timepiece circuit part, which may cause an error in the time. Therefore, the flow in Figure 11 is to make the azimuth meter to display a more accurate time after the azimuth measurement. It is also possible to receive time information. In addition, when the two-point direction in the flowchart in FIG. 11 is consistent with the north direction, the backlighting unit 103b is used for reporting, but the reporting method is not limited to this. As described above, according to the radio-controlled timepiece 100 according to this embodiment, the magnetic field detection elements X and γ which are mutually independent are arranged so that they can be arranged in mutually different detection directions to a free direction, especially When installed in small electronics, it can increase the freedom of arrangement and improve the efficiency of the magnetic field detection element. As the calculation is based on the configuration of the magnetic field detection element, the orientation can be detected correctly, and it becomes unnecessary to implement the magnetic field detection element previously implemented. Moreover, the angle Φ crossing the magnetic field detection element X and the magnetic field detection element Y in the direction of the detected magnetic field is 7Γ 72 or more or 7Γ / 2, so it is compared with the case where the fixed Φ is 7Γ / 2 as before. It can improve the installation freedom of the product, and also improve the installation efficiency of the magnetic field detection element. 103b After the root orientation is measured, it is due to the installation position of the single magnetic machine. In step S3 to step S6, the angle φ / 2 in the 12-point direction is specified. The orientation is determined based on whether the calculated angle Θ in the north direction is equal to the angle φ / 2 in the 12-point direction. Calculate the magnitude H s of the geomagnetic field η with the angle β of the angle β. Set the orientation of the geomagnetic field η where the magnitude H s of the geomagnetic field is the largest, and set the north direction as the output. Yes. To find the magnitude H s of the geomagnetic ,, for example, the angle $ and the X component 及 X of the geomagnetism calculated above can be substituted into the formula (1). That is, the magnitude of the geomagnetic η according to the formula (丨) becomes Hs. = Hxxsec < 9. Also, since the measurement results of the azimuth are reported by lighting back light or sound, it is not necessary to newly set a special method for reporting the measurement results, and the manufacturing cost of the radio-controlled timepiece 100 can be suppressed. ≪ Deformation Example > The flowchart shown in FIG. 11 shows the situation reported when the 12 o'clock direction is consistent with the north direction, but the following shows the action when the position shown in the 12 o'clock direction is notified. An example of this operation will be described with reference to the flowchart in FIG. 12 and the bearing measurement processing ② performed by the radio-controlled timepiece 1000. Since the azimuth measurement button 1 〇 2a is pressed, the azimuth measurement is instructed (step S 丨 丨; yes) when the azimuth sensor 1 1 2 is driven by the drive circuit 1 1. As a current flows through the bias coil C, a bias magnetic field is applied to the magnetic field. Detection elements X, γ (step s) Next, the x component of the magnetic field is detected by the magnetic field detection element X (step S 1 3), and the y component of the magnetic field is detected by the magnetic field detection element Y (step S 1 4), and then the azimuth calculation is performed The unit 1 〇1 a calculates the angle 0 〇 in the north direction based on the magnetic fields detected in steps S 1 3 and s 1 4 (step S 1 5). If the angle 0 〇 in the north direction is calculated, it is determined whether the angle 0 〇 Equal to Regulation-18- 200424545 値 / 2/2 (step S16). When step S16 is not 0 〇 = φ / 2 (step si6 • 'No') return to step S 1 3. Use of a radio-controlled timepiece 1 〇〇 In other words, the direction of the radio-controlled timepiece 100 is changed by changing the direction of the wrist or body, and the control section 101 repeats the processing from step S13 to step S16 in response to the direction of the radio-controlled timepiece 100. In step S16 Becomes 0 〇 = φ / 2, when the 12 o'clock direction is consistent with the north direction as shown in FIG. 13A (step Step S16; Yes), the backlight unit 103b is turned on (step S17). For example, 'At this time, when the observer's body is north, change the direction for the purpose and proceed with the next step. The backlight unit 10 After lighting in 3b, the position measurement is instructed by pressing the position measurement button 1202a 'again (step S 1 8; Yes), and the magnetic field detection element X detects the X component of the magnetic field (step S 1 9), and the magnetic field detection The element γ detects the y component of the magnetic field (step S20). Next, the azimuth calculation unit 101a calculates the angle 0 i in the north direction based on the magnetic fields detected in steps S 18 and S 19 (step S 2 1). After calculating the angle Θ i in the north direction, the application of the bias magnetic field is completed (step S 22). 'The angle 0 G (0 α = φ / 2) calculated from step S15 is different from the 0 1 calculated from step S 2. 0 0 !, Calculate the azimuth in the 12 o'clock direction (step S23). When the azimuth in the 12 o'clock direction is detected, the detected azimuth is displayed on the display unit 103a to notify (step S24), and the present azimuth measurement process is terminated. For example, as shown in Figure 13B, when 0〇-01 = φ / 2- 0ι = -7τ / 4, the azimuth at 12 o'clock is north. East. As shown in Fig. 13C, when 0 Q-0 1 = φ / ΐ-θ ^ + π / 4, the azimuth in the direction of 12 o'clock becomes northwest. As described above, the azimuth of the observer's direction is observed. -19- 200424545 In step S 2 4, the position in the direction of 12 o'clock is displayed on the display unit 10 3 a for notification, but the notification method is not limited to this. For example, a pointer may be used for notification. According to the azimuth measurement processing shown in Fig. 12, as the azimuth indicating the predetermined position of the radio-controlled timepiece 1000 (azimuth in the direction of 12 o'clock), the azimuth sensor can be notified because it can also notify the azimuth other than the north direction. Convenience. According to the present invention, two independent magnetic sensors can be arranged so that the crossing angle of the magnetic field detection direction is 90 degrees or more and 180 degrees or less, or 90 degrees more than 0 degrees, which can improve the magnetic sensitivity of the arrangement. Degree of freedom of the measuring device. Since the orientation is calculated based on the configuration of the magnetic sensor, the correct orientation can be raised. It should be noted that the content of the description in this embodiment can be changed as appropriate without departing from the spirit of the present invention. (5) Brief Description of Drawings Figure 1 is a schematic plan view of a radio-controlled timepiece 100 according to an embodiment of the present invention. Figure 2 is a cross-sectional view of the π-! 丨 part of Figure 1. FIG. 3 is a plan view of a radio-controlled timepiece 2000 according to a modification of the embodiment of the present invention. Fig. 4 is a sectional view of part iv_IV in Fig. 3. Fig. 5A is a diagram showing an example of an arrangement when the crossing angle of the magnetic field detection element X and the magnetic field detection element Y constituting the azimuth sensor 1 and 2 is 90 degrees or more and 180 degrees or less. Fig. 5B is a diagram showing the arrangement when the crossing angle of the magnetic field detection element X and the magnetic field detection element 构成 constituting the azimuth sensor 1 12 is greater than 0 ° and less than 90 ° -20-200424545. Fig. 6 is a block diagram showing an example of a circuit configuration of a radio-controlled timepiece 100. Fig. 7 is a block diagram showing an example of a circuit configuration of the orientation sensor 1 10 shown in Fig. 6. Fig. 8 is a graph showing the relationship between the geomagnetic field and the magnetic field detection direction. Fig. 9A is a diagram showing an example of the arrangement of the magnetic field detection element X, the magnetic field detection element Υ, and the bias coil C when the angle at which the magnetic field detection element X intersects the magnetic field detection element γ is 90 ° to 180 °. Fig. 9B is a diagram showing an example of the arrangement of the magnetic field detection element X, the magnetic field detection element Υ, and the bias coil C when the angle at which the magnetic field detection element X intersects the magnetic field detection element γ is greater than 0 to 90 degrees. Fig. 10 is a diagram showing the relationship between the direction in which the bias magnetic field B is applied and the direction in which the magnetic field is detected. Fig. 11 is a flowchart showing the azimuth measurement process ① performed by the radio-controlled timepiece 100. Fig. 12 is a flowchart showing a modified example of the present embodiment, and shows the azimuth measurement process ② performed by the radio-controlled timepiece 1000. Figure 13A is the azimuth measurement process in Figure 12 when the 12 o'clock direction coincides with the north direction, showing the relationship between the magnetic field detection direction and the north (geomagnetic direction) and 12 o'clock directions. Figure 1 3B is the azimuth measurement process ② in Figure 12 when the azimuth in the 12 o'clock direction becomes northeast, showing the relationship between the magnetic field detection direction and the north (geomagnetic direction) and 12 o'clock directions. Figure 1 3 C shows the azimuth measurement processing in Figure 12 ②. When the azimuth at 12 o'clock-21-242004545 becomes North West, it shows the relationship between the magnetic field detection direction and the north (geomagnetic direction) and 12 o'clock directions. Illustration. The representative symbols of the main part explain the magnitude of the bias magnetic field B, / 3 Bi bias magnetic field C; Cx, Cy bias coil Η Geomagnetic Ηχ Hy Lx, Ly X, YI θ 0〇, θ 10 1a 102a 1 03 103a 103b 106 1 07 108 110 111 Geomagnetic X-axis direction Geomagnetic y-axis direction y component Magnetic detection direction Magnetic field detection element (Magneto-sensing sensor) Angle where magnetic detection direction intersects Angle detected by geomagnetism Magnetic angle North direction azimuth calculation unit Azimuth measurement button display section Display section Backlight section Reception control section Time code conversion section Timing circuit section Azimuth sensor section drive circuit-22- 200424545 112 Azimuth sensor (azimuth measurement device) 1 1 3 Magnification section 114 A / D Conversion circuit-23-
Claims (1)
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2003074887A JP2004279363A (en) | 2003-03-19 | 2003-03-19 | Electronic device with direction sensor and program |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| TW200424545A true TW200424545A (en) | 2004-11-16 |
Family
ID=33027851
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| TW093107202A TW200424545A (en) | 2003-03-19 | 2004-03-18 | Azimuth measuring method and apparatus, and recording medium having stored the azimuth measuring method |
Country Status (3)
| Country | Link |
|---|---|
| JP (1) | JP2004279363A (en) |
| TW (1) | TW200424545A (en) |
| WO (1) | WO2004083780A1 (en) |
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|---|---|---|---|---|
| JP2017026370A (en) * | 2015-07-17 | 2017-02-02 | セイコーエプソン株式会社 | Electronics |
| EP3333646A1 (en) * | 2016-12-06 | 2018-06-13 | ETA SA Manufacture Horlogère Suisse | Portable object including a rotatable drive shaft, the actuation of which is detected by means of two inductive sensors |
| CN109557796B (en) * | 2017-09-25 | 2021-10-01 | 精工爱普生株式会社 | clock with magnetic sensor |
| JP2020134353A (en) * | 2019-02-21 | 2020-08-31 | セイコーエプソン株式会社 | Electronic clock |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2622637B2 (en) * | 1991-11-20 | 1997-06-18 | ユピテル工業株式会社 | Moving body direction measurement method and apparatus |
| CH687288B5 (en) * | 1994-11-21 | 1997-05-15 | Asulab Sa | Watch comprising a detection device of the northbound earth magnetic. |
| JP4006674B2 (en) * | 2001-05-22 | 2007-11-14 | 日立金属株式会社 | Compass |
-
2003
- 2003-03-19 JP JP2003074887A patent/JP2004279363A/en active Pending
-
2004
- 2004-03-18 TW TW093107202A patent/TW200424545A/en unknown
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| JP2004279363A (en) | 2004-10-07 |
| WO2004083780A1 (en) | 2004-09-30 |
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