TWI284682B - Electric discharge surface treating electrode, manufacture and evaluation methods thereof, electric discharge surface treating device, and electric discharge treating method - Google Patents
Electric discharge surface treating electrode, manufacture and evaluation methods thereof, electric discharge surface treating device, and electric discharge treating method Download PDFInfo
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Abstract
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1284682 玖、發明說明 [發明所屬之技術領域] 本發明有關以金屬、金屬化合物或陶瓷之粉末壓縮成 型之壓粉體所成放電表面處理用電極與加工物之間發生脈 衝狀之放電,並藉由該放電能量,而於加工物表面形成由 電極材料或電極材料因放電能量而反應的物質所成被膜的 放電表面處理中所使用之放電表面處理用電極、及其製造 方法與評價方法。又,亦有關使用該放電表面處理用電極 的放電表面處理裝置及放電表面處理方法。 [先前技術] 為航空飛機用燃氣渦輪引擎(gas turbine engine)之渦 輪機葉等之表面處理,由於需要將具有高溫環境下的強度 與〉間滑性的材料加以塗佈或加厚之故,向來採用焊接或火 焰噴塗(flame spray coating)等方法。藉由焊接或火焰喷塗 等方法,而將含有周知能在高溫環境下氧化而變成氧化 物’並發揮潤滑性的Cr(鉻)或Mo(鉬)作為基材的材料之被 膜,加厚於加工物(以下,稱為工件)上。在此,焊接,係 指藉由工件與焊接條之間的放電而使焊接條之材料熔融附 者於工件上的方法之意,而火焰喷塗,係指將金屬材料作 成炼融的狀態,並按喷霧狀方式喷塗於工件上,以形成被 膜的方法之意。 然而,由於此種焊接或火焰喷塗之任何一種方法均為 依靠人工的作業而需要熟練之故,作業之流程(line)化上有 困難’而有成本高張的問題。又,特別是焊接,係由於熱 315550 6 1284682 置集中而灌入工件中的方法之故,當處理厚度較薄的情 开'或處理如單結晶合金或單向凝固合金⑽W卜…化加丨 s〇lid=icating all〇y)等之方向控制合金等的易破裂材料 時谷易發生焊接裂開,而有收率差的問題。 作為解決此種問題的技術,提案有藉由液中放電,將 本身為工件的金屬材料表面加以塗層(coding)的方法。例 如’在第1種先前技術中揭示有,首先,作為i次加工, 使用含有將形成在工件的被膜成分的電極材料實施液中放 電後,作為2次加工係使用其他銅電極或石墨等不易消耗 的電極,對工件上所堆積#電極㈣實施再溶^放電加工 者(例如,參考專利文獻υ。如照此文獻,則對本身為工件 的鋼材可製得堅硬密接度良好的被覆層。然❿,對如超 硬合金等的燒結材料表面則難於形纟具有堅固^密接力的 被覆層。又,在此方法中,需要形成被膜的丨次加工、及 將被膜加以再熔融放電加工以使密接於工件的2次加工之 方式的2階段之步驟,以致有處理上變成複雜的問題。 在第2種先前技術中揭示有,依此種2階段之加工以 形成被膜的處理中,不改換電極之下僅靠放電電氣條件之 變更即能於金屬表面形成硬質之陶瓷被膜的技術(例如,參 考專利文獻2)。在此第2種先前技術中,係將成為構成電 極的陶瓷粉末,按能成為理論密度之5〇%至9〇%之方式, 以l〇t/cm2之極高壓力壓縮成型並經煅燒結者作為電極使 用。 在第3種先前技術中,則將形成Ti(鈦)等之硬質碳化 315550 7 1284682 物的材料作為電極,使在 身為卫件的金屬材料之間發 再= 經過在第1及第2種先前技術中所需要的 :::之過程’而於金屬表面形成堅固的硬質被膜(例如, :考專利文獻3)。此乃係利用因放電所消耗的電極材料盘 ^液中之成分的c(碳)起反應而生成Tic(碳化鈦)的現象 ^。又,ΤΐΗ2(氫化鈦)等,如藉由金屬之氫化物之壓粉體 電極,使與本身為工件的金屬材料之間發生放電,則可形 成較使用Ti等金屬材料時為快速且密接性良好的硬質被 膜。再者’如使用Tm2等之氫化物中混合有其他金屬或陶 竞的壓粉體電極,而使與本身為卫件的金屬材料之間發生 放電,則亦可迅速形成具有高硬度、耐磨耗性等種種性質 的硬質被膜。 、 又,在第4種先前技術中,將陶瓷粉末壓縮成型,並 藉由預備燒結以製造強度高的壓粉體電極,使用該電極並 藉由放電表面處理以形成Tic等之硬質材料之被膜(例 如,參考專利文獻4)。作為該第4種先前技術之一例,就 製造由經混合WC(碳化鎢)粉末與co(鈷)粉末的粉末所成 放電表面處理用電極(以下,簡稱電極)的情形加以說明。 此合WC粉末與Co粉末並壓縮成型所成壓粉體,可為僅 混合WC粉末與Co粉末並壓縮成型者,惟如摻入臘(wax) 後加以壓縮成型時即可改善壓粉體之成型性之故而更合 適。但,由於臘係絕緣性物質之故,如大量殘留在電極中 時,則由於電極之電阻會增大之故,放電性會惡化。於是, 需要將脱去除。此種腹’如將壓粉體放入真空爐内加熱, 8 315550 1284682 即可去除。此時,如加熱溫度過低時即不能去除臘、而溫 度過高時則臘即變成碳屑而劣化電極純度之故,需要保持 加熱溫度為能熔融臘的溫度以上且能分解臘而成為碳屑的 溫度以下。其次,使用高頻線圈將真空爐中之壓粉體加熱, 並燒成至賦與能耐機械加工的強度,且不致於過份硬化的 程度,例如粉筆程度之硬度。此種燒成,稱為預備燒結。 此時奴化物間之接觸部會有互相間之結合,惟因燒結溫 度較低而不會到達本燒結的溫度之故,其結合較弱。如使 用經此種預備燒結所燒成的強度高的電極實施放電表面處 理,即可於工件表面形成緻密且均質的被膜。 (專利文獻1) 曰本專利特開平5-148615號公報 (專利文獻2) 曰本專利特開平8-300227號公報 (專利文獻3 ) 曰本專利特開平9-192937號公報 (專利文獻4) 國際公開第99/58744號手冊 如第3及第4種先前技術所示,可藉由使用將壓粉體 所得電極的放電表面處理,而形成緻密的硬質被膜。但, 如藉由此種放電表面處理以形成厚膜時,即使依照第4種 先前技術所揭示方式製造電極,仍有電極之特性上呈現大 的差異的問題。又難於形成緻密的膜。 對於此種差異之原因之一,可能係因構成電極的素材 9 315550 1284682 之粉末粒徑之分佈不相同所引起。此乃如所製造的 有粉末上的粒徑之分佈之差異,則即使以同一加壓機 (press)壓力加壓以成型電極,由於各電極的結硬程 的關係,最後在電極強度上會發生差異之故。又二 =特:上所引起的差異之其他原因之一者,可能係因 形成在工件上的被膜材質之改變使所實施的電極材質(成 分)之變更。此乃如改變電極《材質時,因物性值之差显而 電極強度即與改變前之電極強度產生不同之故。" 又,如藉由放電表面處理以形成厚膜時,一般認為來 自電極側的材料之供給、及其所供給的材料在工件表面的 熔融及與工件材料的結合之方式對被膜性能最有影響。對 此種電極材料之供給上有影響的一個指標,即為電極之硬 度。例如,在第4種先前技術中,係將放電表面處理用電 極之硬度’作成能耐機械性加卫的強度且不過分硬化的程 度的硬度(例如粉筆程度之硬度)。藉由此種硬度之電極, 即可抑制因放電所引起的電極材料之供給,而所供給的材 料s充刀熔融之故,能在工件表面實現硬質陶竟被膜之形 成。 又,作為放電表面處理用電極之硬度指標的粉筆程度 之硬度’係非常含糊者。並且,亦有因此種電極之硬度等 的特性,而工件表面所形成的厚膜上產生差異的問題。如 Μ «極的粉末之材質或大小改變’則電極之成型條件會 不同。因此’有需要按各種電極之材質多次改變電極之成 型條件以實施被膜之形成試驗,藉以決定作為適合於其材 315550 10 1284682 質之放電表面處理用電極 屯從 < 便用的成型條件的過程的問 題。亦即’按構成電極的材質之種類 刊貝 < 裡頌需要求出為形成良 好被膜所需電極之成型侔件 又主俅仵,因而有耗費工夫的問題。豆 他’即使使用同樣材質之格太计# F1技& 〃 您杨末並依冋樣製造方法以製造電 極’由於因季節(溫度或渴产 又4廣度)之不同而粉末之體積會變化 之故’仍然與上述之材質變化時同樣,需要分別加以實際 加工以形成被膜,並將其電極評價,以致頗費勞力。、 又,此等先前之放電表面處理,係主要著重於硬質被 媒Α成’尤其疋接近常溫時的硬質被膜之形成,而現狀 。係以Φ成硬貝碳化物為主成分的被膜者。在此方法 中’僅能形成1G/zm程度之薄膜,而未能將被膜厚度為數 以上之厚度。以往,係多含有容易形成碳化物的材 料之比例’例如’電極中如含有Ti等材料,則因油中的放 電而起化學反應’被膜即成為如TiC(碳化鈦)的硬質碳化 物。隨著表面處理之進展,工件表面之材質即從鋼材(對鋼 材加以處理時)變成本身為陶瓷的Tic,係隨著熱傳導或熔 點等的特性變化之故。 :、、〈'而,如依本發明人等之實驗發現,如對電極材質之 成分中添加不會形成碳化物或難以形成碳化物的材料後, 則可增厚被膜之現象。此乃由於對電極添加不會碳化或難 、反化的材料,則不會成為碳化物而保持金屬狀態的材料 會增加所致者。並且發現,此種電極材料之選定,對被膜 之増加厚度上具有重要意義。於此同時,所形成被膜具有 硬度、緻密性及均一性。但,以往之放電表面處理,如上 315550 11 1284682 所述,係主要著重於Tie或WC(碳化鎢)等接近常溫時能發 揮硬質性的被膜之形成者,而關於如航空飛機用燃氣渦輪 引擎之渦輪機葉等的用途等在高溫環境下具有潤滑性之緻 密且較厚被膜(100 // m層級以上之厚膜)之形成,則並未加 以著重’而有不能形成如此厚度的被膜的問題。 另一方面,在第2之先前技術中,使用將成為構成電 極的材料的陶磁粉末按能成為理論密度之50%至90%之方 式,以如10t/cm2般之極高壓力壓縮成型並經锻燒結的電 極。此乃係因(1)以形成薄的硬質被膜為目的之故,電極堅 硬則可使形成的被膜愈強、(2)由於材質之主成分為陶竟之 故,可提高將構成電極的陶瓷粉末壓縮成型時之壓力,等 理由。但,如欲藉由放電表面處理以形成緻密的金屬之厚 膜時’則不能使用依第2之先前技術所示方法所製造之電 極。此乃因如將金屬粉末按第2先前技術所示以1 〇t/cm2 般的高壓力加壓時,則電極結硬,以致不能藉由放電表面 處理而形成被膜,如使用此種電極以實施放電表面處理, 則成為切削工件表面的彫型放電加工之故。亦即,由於在 第2之先前技術中使用陶瓷粉末之故,如以上述般的高壓 力加壓以製造放電表面處理用電極時並不會有問題,惟不 能將其條件直接適用於由金屬粉末所成放電表面處理用電 極上’對採用放電表面處理以形成緻密的金屬之厚膜用之 放電表面處理用電極之製造方法,則至今尚無人開發。 本發明係鑑於上述情形所開發者,以製得能藉由放電 表面處理方法,於加工物上容易地形成緻密的厚膜的放電 315550 12 1284682 表面處理用電極為目的。 又,以製得在放電表面處理時能在高溫環境下形成具 有潤滑性的厚被膜的放電表面處理用電極為目的。並且, 以獲得可正確評價其放電表面處理用電極能否冑用為被膜 形成的放電表面處理用電極之評價方法為目的。 再者,以製得將金屬粉末作為壓粉體電極使用的放電 表面處理時,减降低面粗糙度之下能實施安定的放電以 堆積厚被膜的放電表面處理用電極為目的。 再者,又以獲得使用此蓉姑φ主m 又竹丈w此寻孜電表面處理用電極的放電 表面處理裝置、及其方法為目的。 [發明内容] 為達成上述㈣’有關本發明之放電表面處理用電 極,係以金屬、金屬化合物或陶竞粉末壓縮成型的壓粉體 作為電極,在加工液中或氣體中’使前述電極與加工物之 :發生放電1由其放電能量’而於前述加工物表面形成 或電極材料因放電能量而反應的物質所成被膜 用為放電表面處理的放電表面處理用電極, 月'4末’具有5 i 10/zm之平均粒徑之同時,含 於加工物上形成被膜的成分,與4〇體積%以上之不合: :化物或難以形成碳化物的成分的混合物,並經成‘為依 ^用錯筆到痕試驗的硬度能成為Μ 8β範圍 係以金屬 ’在加工 其次,有關本發明之放電表面處理用電極, 或金屬化合物之粉末壓縮成型的壓粉體作為電極 315550 13 1284682 液中或氣體中,使前述電極與加工物之間發生放電,藉由 其放電能量,而於前述加工物表面形成由電極材料或電極 材料因放電能量而反應的物質所成被膜之用為放電表面處 理的放電表面處理用電極,其特徵為:前述電極之壓縮強 度,為160MPa以下者。 其次,有關本發明之放電表面處理用電極,係以本身 為金屬或金屬化合物之粉末的電極材料壓縮成型之壓粉體 作為電極,在加工液中或氣體中,使前述電極與加工物之 間發生放電’藉由其放電能量,而於前述加工物表面形成 由前述電極材料或前述電極材料因放電能量而反應的物質 所成被膜之用為放電表面處理的放電表面處理用電極,其 特徵為:前述電極材料對前述電極之體積所佔的體積比 例,為 25°/。至 65%。 其次,有關本發明之放電表面處理用電極,係以金屬 或金屬化合物之粉末壓縮成型的壓粉體作為電極,在加工 液中或氣體中,使前述電極與加工物之間發生放電,藉由 其放電能量,而於前述加卫物表面形成由電極材料或電極 材料因放電能量而反應的物質所成被膜之料纟電表面處 理的放電表面處理用電極,其特徵為:熱傳導率為刪恤 以下。 又,為達成上述目的起見,有關本發明之放電表面處 理用電極之製造方法夕4主. 表以乃沄之特徵為·包含以金屬、金屬化合物 或陶瓷之粉末粉碎的箆! + _ η & % 弟1 v驟、及為將經粉碎的前述粉末 凝聚所成塊分解為極間距齙 』此離以下之大小而過篩的第2步 315550 14 1284682 驟、以及將前述過筛之粉末作成既定之形狀,並以93至 278MPa之壓力壓縮成型的第3步驟。 再者,為達成上述目的起見,有關本發明之放電表面 處理用電極之製造方法,係以金屬、金屬化合物或陶竟之 粉末壓縮成型的壓粉體作為電極,在加工液中或氣體中, 使:述電極與加工物之間發生放電,藉由其放電能量,而 於前述加工物表面形成由電極材料或電極材料因放電能量 :反應的物質所成被膜的放電表面處理方法,其特徵為: :述粉末,具有…0/zm之平均粒徑之同時,含有為於 前述加工物上形成被膜的成分、與4g體積%以上之不會形 成碳化物或難以形成碳化物的成分的混合物,並使用依塗 膜用錯筆刮痕試驗的硬度能成為8Bm圍之方式所成 型的電極,以形成前述被膜。 其次’有關本發明之放電表面處理方法,係以金屬或 金屬^合物之粉末壓縮成型的壓粉體作為電極,在加工液 中或孔體中,使前述電極與加工物之間發生放電,藉由其 放電能量,而於前述加工物表面形成由電極材料或電極材 料因放電能的物質所成被膜的纟電表面處理方 法,其特徵為:使用具有160MPa以下之壓縮強度的電極, 以形成前述被膜。 其次’有關本發明之放電表面處理方法,係以本身為 金屬或金屬化合物之粉末的電極材料壓縮成型的壓粉體作 為電極,在加工液中或氣體中,使前述電極與加工液之間 毛生放電,藉由其放電能量,而於前述加工物表面形成由 315550 15 1284682 前述電極材料或前述電極材料因放電能量而反應的物質所 缝膜的放電表面處理方法,其特徵為:㈣電極材料對 前述電極之體積所佔的體積比例為25至65%的電極,以 形成前述被膜。 其次,有關本發明之放電表面處理方法,係以金屬或 金屬化合物之粉末壓縮成型的壓粉體作為電極,在加工液 中或氣體中,使前述電極與加工物之間發生脈衝狀之放 電’藉由其放電能量,而於前述加工物表面形成由電極材 料或電極材料因放電能量而反應的物質所成被膜的放電表 面處理方法’其特徵為:使用熱傳導率為i釋/故以下之 電極,以形成前述被膜。 又,達成上述目的起見,有關本發明之放電表面處理 裝置,係在加工液中或氣體中配置有以金屬、金屬化合物 或陶究之粉末壓縮成型的壓粉體所成電極、及將形成被膜 的加工物,而藉由與前述電極及前述加工物按電氣性連接 的電源裝置,而使前述電極與前述加工物之間發生脈衝狀 之放電,並藉由其放電能量,而於前述加工物表面形成由 電極材料或電極材料因放電能量而反應的物質所成被膜的 放電表面處理裝置,其特徵為:前述電極,係將含有用於 加工物上形成被膜的成分、與4〇體積%以上之不會形成碳 化物或難以形成碳化物的成分的混合物的平均粒徑5至1〇 之粉末,成型為依塗膜用鉛筆刮痕試驗的硬度能成為 B至8B範圍之硬度之方式。 其次’有關本發明之放電表面處理裝置,係在加工液 315550 16 1284682 中或氣體中配置有以金屬或金屬化合物之粉末壓縮成型的 壓粉體所成電極、及將形成被膜的加工物,而藉由與前述 電極及前述加工物按電氣性連接的電源裝置而使前述電極 與岫述加工物之間發生脈衝狀之放電,並藉由其放電能 量,而於前述加工物表面形成由電極材料或電極材料因放 電能量而反應的物質所成被膜的放電表面處理裝置,其特 徵為·前述電極,具有16 OMPa以下之壓縮強度。 其次,有關本發明之放電表面處理裝置,係在加工液 中或氣體中配置有时屬$金屬4匕合物之粉末壓縮成型的 壓粉體所成電極、及將形成被膜的加工物,而藉由與前述 電極及前述加工物按冑氣性連接㈣源裝置,岐前述電 =與前述^物之間發生脈衝狀之放電,並藉由其放電能 量::於前述加工物表面形成由電極材料或電極材料因放 電能量而反應的物質所成被膜的放電表面處理裝置,其特 徵為:前述電極’係作成對該電極之體積所佔前述電極材 料之體積比例,為25至65%。 面處理裝置,係在加工液 化合物之粉末壓縮成型的 的加工物,而藉由與前述 的電源裝置而使前述電極 放電,並藉由其放電能 電極材料或電極材料因放 放電表面處理裝置,其特 以下之熱傳導率。1284682 发明Invention Description [Technical Field] The present invention relates to a pulse-like discharge between an electrode for discharge surface treatment formed by compression molding of a powder of a metal, a metal compound or a ceramic, and a processed object. The discharge surface treatment electrode used in the discharge surface treatment of the film formed by the electrode material or the electrode material due to the discharge energy is formed on the surface of the workpiece by the discharge energy, a method for producing the same, and an evaluation method. Further, a discharge surface treatment apparatus and a discharge surface treatment method using the discharge surface treatment electrode are also known. [Prior Art] For the surface treatment of a turbine blade or the like of a gas turbine engine for an aircraft, since it is necessary to apply or thicken a material having a strength and a slip property in a high temperature environment, Conventionally, methods such as welding or flame spray coating have been used. A film containing a material such as Cr (chromium) or Mo (molybdenum) which is known to be oxidized in a high-temperature environment to become an oxide and exhibits lubricity as a substrate is thickened by a method such as welding or flame spraying. On the workpiece (hereinafter referred to as the workpiece). Here, the welding means that the material of the welding strip is fused to the workpiece by the discharge between the workpiece and the welding strip, and the flame spraying refers to the state in which the metal material is fused. It is sprayed onto the workpiece in a spray form to form a film. However, since any of such welding or flame spraying methods requires manual work and requires skill, there is a problem in the process of operation, and there is a problem of high cost. Moreover, in particular, welding is a method of pouring into the workpiece due to the concentration of heat 315550 6 1284682, when processing a thinner opening or processing such as a single crystal alloy or a unidirectional solidified alloy (10) When s〇lid=icating all〇y) or the like controls the easily breakable material such as an alloy, the valley is prone to weld cracking, and there is a problem of poor yield. As a technique for solving such a problem, there has been proposed a method of coating a surface of a metal material which is itself a workpiece by liquid discharge. For example, in the first prior art, first, it is difficult to use another electrode such as a copper electrode or graphite as a secondary processing system by using an electrode material containing a film component formed on a workpiece as a secondary process. The electrode to be consumed is subjected to re-dissolving and discharging the deposited electrode (4) on the workpiece (for example, refer to the patent document). According to this document, a coating layer having a good hardness and adhesion can be obtained for a steel material which is itself a workpiece. Then, it is difficult to form a coating layer having a strong adhesion to a surface of a sintered material such as a super-hard alloy. Further, in this method, it is necessary to form a coating process and re-melt discharge the film. The two-stage step of making the second processing in close contact with the workpiece has a problem that becomes complicated in processing. In the second prior art, it is disclosed that in the processing of forming the film according to the two-stage processing, A technique of forming a hard ceramic film on a metal surface by changing only the electrical conditions of the discharge under the change of the electrode (for example, refer to Patent Document 2). In the technique, the ceramic powder constituting the electrode is compression-molded at a very high pressure of 10 〇t/cm 2 and used as an electrode by a calcination at a theoretical density of 5 to 9 %. In the third prior art, a material of hard carbonized 315550 7 1284682 of Ti (titanium) or the like is formed as an electrode, so that the metal material which is a guard member is sent again = after the first and second types The process of::: is required in the art to form a strong hard film on the surface of the metal (for example, Patent Document 3). This is the use of the component (c) of the electrode material consumed by the discharge. Carbon) reacts to form Tic (titanium carbide). Further, ΤΐΗ2 (titanium hydride) or the like, such as a metal powder of a metal hydride, causes discharge to occur between a metal material that is itself a workpiece, It is possible to form a hard film which is fast and has good adhesion when using a metal material such as Ti. Further, if a metal powder such as Tm2 or the like is mixed with other metals or a ceramic powder electrode of Tao Jing, it is a Discharge between the metal materials of the piece, It is also possible to rapidly form a hard film having various properties such as high hardness and abrasion resistance. Further, in the fourth prior art, the ceramic powder is compression-molded and prepared by preliminary sintering to produce a high-pressure powder electrode. A film of a hard material such as Tic or the like is formed by the discharge surface treatment using the electrode (for example, refer to Patent Document 4). As an example of the fourth prior art, a mixed WC (tungsten carbide) powder is produced. The case where the powder of co (cobalt) powder is used as an electrode for discharge surface treatment (hereinafter referred to as an electrode) is described. The WC powder and the Co powder are compression-molded into a pressed powder, and only WC powder and Co powder can be mixed. And it is more suitable for compressing the molder, but it is better to improve the formability of the green compact if it is subjected to compression molding after being blended with wax. However, when a large amount of the wax-based insulating material remains in the electrode, the electrical resistance of the electrode is increased, so that the discharge property is deteriorated. Therefore, it needs to be removed. Such a belly can be removed by placing the pressed powder in a vacuum furnace and heating it at 8 315 550 1284682. At this time, if the heating temperature is too low, the wax cannot be removed, and when the temperature is too high, the wax becomes carbon dust and deteriorates the purity of the electrode. It is necessary to keep the heating temperature above the temperature at which the wax can be melted and to decompose the wax to become carbon. The temperature of the chips is below. Next, the green compact in the vacuum furnace is heated using a high frequency coil and fired to a degree that is resistant to mechanical processing and does not excessively harden, such as the hardness of chalk. Such baking is called preliminary sintering. At this time, the contact portions between the sulphides will be combined with each other, but the combination is weak because the sintering temperature is low and does not reach the temperature of the sintering. When the discharge surface treatment is performed using an electrode having high strength which is fired by such preliminary sintering, a dense and homogeneous film can be formed on the surface of the workpiece. (Patent Document 1) Japanese Laid-Open Patent Publication No. Hei. No. Hei. No. Hei. No. Hei. No. Hei 9-192937 (Patent Document 3). International Publication No. 99/58744, as shown in the third and fourth prior art, can form a dense hard film by treating the discharge surface of the electrode obtained by pressing the powder. However, when such a discharge surface is treated to form a thick film, even if the electrode is fabricated in the manner disclosed in the fourth prior art, there is a problem that the characteristics of the electrode are largely different. It is also difficult to form a dense film. One of the reasons for this difference may be caused by the difference in the particle size distribution of the material constituting the electrode 9 315550 1284682. If the difference in the distribution of the particle diameters on the powder is produced, even if the pressure is pressed by the same press pressure to form the electrode, the electrode strength will eventually be due to the junction hardening relationship of each electrode. There is a difference. Second, special: One of the other causes of the difference caused by the change may be the change in the material (component) of the electrode to be implemented due to the change in the material of the film formed on the workpiece. For example, when the electrode material is changed, the difference between the physical properties and the electrode strength is different from the electrode strength before the change. " Also, when a thick surface film is formed by discharge surface treatment, it is generally considered that the supply of the material from the electrode side, the melting of the material supplied thereto, and the bonding with the workpiece material have the most performance on the film. influences. An indicator that has an effect on the supply of such an electrode material is the hardness of the electrode. For example, in the fourth prior art, the hardness of the electrode for discharge surface treatment is made to be a hardness (for example, a hardness of chalk) which is resistant to mechanical strength and which is not excessively hardened. By the electrode of such hardness, the supply of the electrode material due to the discharge can be suppressed, and the supplied material s is melted by the knife, so that the hard ceramic film can be formed on the surface of the workpiece. Further, the hardness of the chalk degree as the hardness index of the electrode for discharge surface treatment is very ambiguous. Further, there are also problems such as the hardness of the electrodes and the like, and there is a problem that a thick film formed on the surface of the workpiece is different. For example, if the material or size of the powder is changed, the molding conditions of the electrode will be different. Therefore, it is necessary to change the molding conditions of the electrode a plurality of times according to the material of the various electrodes to carry out the film formation test, thereby determining the molding conditions for the discharge surface treatment electrode suitable for the material 315550 10 1284682. The problem with the process. In other words, the type of the material constituting the electrode is required. It is necessary to determine the shape of the electrode for forming a good film, and it takes a lot of trouble. Bean he's even using the same material of the grid too # F1 Technology & 〃 You Yang Yang and according to the manufacturing method to make the electrode 'because of the season (temperature or thirsty and 4 breadth) the volume of the powder will change The reason is that, as with the above-mentioned material change, it is necessary to separately process the actual film to form a film, and evaluate the electrode so that it is laborious. Moreover, these prior discharge surface treatments are mainly focused on the formation of a hard film which is hard-made by the media, especially when it is close to normal temperature. It is a film containing Φ into a hard shell carbide as a main component. In this method, only a film of the order of 1 G/zm can be formed, and the thickness of the film is not more than several. Conventionally, a ratio of a material which is likely to form a carbide is contained. For example, if a material such as Ti is contained in the electrode, a chemical reaction occurs due to discharge in the oil, and the film becomes a hard carbonaceous material such as TiC (titanium carbide). As the surface treatment progresses, the material of the surface of the workpiece changes from the steel material (when the steel material is treated) to the Tic which is itself ceramic, which changes with the characteristics of heat conduction or melting point. According to experiments by the inventors of the present invention, if a material which does not form carbides or is difficult to form carbides is added to the components of the electrode material, the phenomenon of the film can be increased. This is because the addition of a material that does not become carbonized or difficult or reversible to the electrode increases the amount of material that does not become a carbide and maintains the metal state. It has also been found that the selection of such an electrode material is important for the thickness of the film. At the same time, the formed film has hardness, compactness and uniformity. However, the conventional discharge surface treatment, as described in 315550 11 1284682, mainly focuses on the formation of a film that can exert a hard property close to normal temperature, such as Tie or WC (tungsten carbide), and relates to a gas turbine engine such as an aviation aircraft. The use of a turbine blade or the like, such as a dense and thick film (a thick film of 100 // m layer or more) having lubricity in a high-temperature environment, does not emphasize "there is a problem that a film having such a thickness cannot be formed" . On the other hand, in the prior art of the second aspect, the ceramic powder which will be the material constituting the electrode is compression-molded at a very high pressure such as 10 t/cm 2 in such a manner as to be 50% to 90% of the theoretical density. Forged sintered electrode. This is because (1) the purpose of forming a thin hard film, the harder the electrode is, the stronger the film can be formed, and (2) the ceramics constituting the electrode can be improved because the main component of the material is ceramic. The pressure during powder compression molding, and other reasons. However, if a thick film of a dense metal is to be formed by a discharge surface treatment, the electrode fabricated by the method of the prior art of the second embodiment cannot be used. This is because if the metal powder is pressurized at a high pressure of 1 〇t/cm 2 as shown in the second prior art, the electrode is hard so that the film cannot be formed by the discharge surface treatment, such as using such an electrode. When the discharge surface treatment is performed, it is an eagle discharge machining process for cutting the surface of the workpiece. That is, since the ceramic powder is used in the prior art of the second aspect, there is no problem in pressurizing the electrode for discharge surface treatment under the high pressure as described above, but the condition cannot be directly applied to the metal. The method for producing an electrode for discharge surface treatment for a thick film having a discharge surface treated with a discharge surface to form a discharge surface treatment electrode has not been developed. The present invention has been made in view of the above circumstances, and has been made in order to produce a discharge 315550 12 1284682 surface treatment electrode which can easily form a dense thick film on a workpiece by a discharge surface treatment method. Further, an electrode for discharge surface treatment capable of forming a thick film having lubricity in a high-temperature environment at the time of discharge surface treatment is obtained. Further, it is intended to obtain an evaluation method for accurately evaluating whether or not the electrode for discharge surface treatment can be used as a film for discharge surface treatment formed of a film. Further, in the case of producing a discharge surface treatment using a metal powder as a powder electrode, it is intended to reduce the surface roughness and to perform a stable discharge to deposit a discharge surface treatment electrode of a thick film. Furthermore, it is also an object of the present invention to obtain a discharge surface treatment apparatus and a method thereof for using the electrode of the surface treatment of the Ronggu φ main m and the bamboo stalk. SUMMARY OF THE INVENTION In order to achieve the above (4) 'electrode for discharge surface treatment according to the present invention, a metal powder, a metal compound or a powder compacted body of a ceramic powder is used as an electrode, and the electrode and the gas are made in a working fluid or a gas. The processed material is a discharge surface treatment electrode which is formed by discharging the energy from the surface of the workpiece or the electrode material is reacted by the discharge energy, and the discharge surface treatment electrode is a discharge surface treatment. 5 i 10 / zm of the average particle size, the composition of the film formed on the workpiece, and 4 vol% or more of the mixture: : or a mixture of components that are difficult to form carbide, and through the 'for ^ The hardness of the erroneous pen-to-mark test can be Μ 8β in the range of the metal 'in the processing, the electrode for discharge surface treatment of the present invention, or the powder compacted powder of the metal compound as the electrode 315550 13 1284682 liquid or In the gas, a discharge occurs between the electrode and the processed object, and by discharging energy, an electrode material or an electrode material is formed on the surface of the processed object. Substance discharge energy into the film and reaction with the discharge of the surface discharge surface treatment is treated with an electrode, wherein: the compression strength of the electrode, those of 160MPa or less. Next, the electrode for discharge surface treatment according to the present invention is an electrode formed by compressing an electrode material of a powder of a metal or a metal compound as an electrode, and between the electrode and the workpiece in a working fluid or a gas. A discharge surface treatment electrode for forming a discharge surface by forming a film formed by the discharge of the electrode material or the electrode material by the discharge energy on the surface of the workpiece by the discharge energy. The ratio of the volume of the electrode material to the volume of the electrode is 25°/. Up to 65%. Next, the electrode for discharge surface treatment according to the present invention is a powder compacted by a powder of a metal or a metal compound as an electrode, and discharge is generated between the electrode and the workpiece in a working fluid or a gas. The discharge surface energy is formed on the surface of the garnish, and the electrode surface material is formed by the electrode material or the electrode material, and the surface of the electrode material is treated by the discharge energy. the following. Further, in order to achieve the above object, the method for producing an electrode for electrical discharge surface treatment according to the present invention is characterized in that it comprises a crucible pulverized with a powder of a metal, a metal compound or a ceramic. + _ η & % 1 v 、 、 、 、 、 、 、 、 、 、 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 315 The powder of the sieve is formed into a predetermined shape and is subjected to a third step of compression molding at a pressure of 93 to 278 MPa. Further, in order to achieve the above object, a method for producing an electrode for electrical discharge surface treatment according to the present invention is a metal powder, a metal compound or a powder compacted powder of a ceramic powder, which is used as an electrode in a working fluid or a gas. a discharge surface treatment method in which a discharge occurs between the electrode and the workpiece, and a discharge surface is formed on the surface of the workpiece to form a film formed by the electrode material or the electrode material due to the discharge energy: the reaction material. It is: a powder having a mean particle diameter of 0/zm and containing a component which forms a film on the processed product, and a mixture of 4 g% by volume or more of a component which does not form a carbide or which is difficult to form a carbide. Further, an electrode formed by a method in which the hardness of the smear-scratch test was 8 8 m was used to form the film. Next, the discharge surface treatment method according to the present invention is a powder compacted by a powder of a metal or a metal compound as an electrode, and a discharge occurs between the electrode and the workpiece in the working fluid or in the pore body. A method of treating a surface of a film formed of a material of an electrode material or an electrode material by discharge energy by forming a discharge energy on the surface of the workpiece, wherein an electrode having a compressive strength of 160 MPa or less is used to form The aforementioned film. Next, the discharge surface treatment method according to the present invention is a powder compacted by using an electrode material of a powder of a metal or a metal compound as an electrode, and between the electrode and the processing liquid in a working fluid or a gas. a discharge surface treatment method in which a discharge film is formed on a surface of the workpiece by a reaction material of 315550 15 1284682 or an electrode material which is reacted by discharge energy, and is characterized by: (4) electrode material An electrode having a volume ratio of 25 to 65% by volume of the aforementioned electrode is formed to form the aforementioned film. Next, in the discharge surface treatment method of the present invention, a powder compacted by a powder of a metal or a metal compound is used as an electrode, and a pulse-like discharge occurs between the electrode and the workpiece in a working fluid or a gas. a discharge surface treatment method in which a material which is reacted by an electrode material or an electrode material due to discharge energy is formed on the surface of the workpiece by the discharge energy thereof, and is characterized in that an electrode having a thermal conductivity of i is used or less To form the aforementioned film. Further, in order to achieve the above object, the discharge surface treatment apparatus according to the present invention is characterized in that an electrode formed by compression molding of a metal, a metal compound or a ceramic powder is placed in a working fluid or a gas, and an electrode is formed. The processed object of the film is subjected to a pulse-like discharge between the electrode and the processed object by a power supply device electrically connected to the electrode and the processed object, and the discharge energy is used for the processing. A discharge surface treatment apparatus for forming a film formed by a material which reacts with an electrode material or an electrode material due to discharge energy, wherein the electrode contains a component for forming a film on a workpiece, and 4% by volume The powder having an average particle diameter of 5 to 1 Å which is a mixture of the above-mentioned components which do not form carbides or which are difficult to form carbides, is formed into a method in which the hardness of the coating film by the pencil scratch test can be a hardness in the range of B to 8B. Next, the discharge surface treatment apparatus according to the present invention is characterized in that an electrode formed by a powder compacted by a powder of a metal or a metal compound and a processed product which will form a film are disposed in the working fluid 315550 16 1284682 or in a gas. a pulse-like discharge is generated between the electrode and the processed workpiece by a power supply device electrically connected to the electrode and the processed object, and an electrode material is formed on the surface of the processed object by discharging energy thereof. Or a discharge surface treatment apparatus in which an electrode material is reacted by a discharge energy to form a film, and the electrode has a compressive strength of 16 OMPa or less. Next, the discharge surface treatment apparatus according to the present invention is characterized in that an electrode formed by a powder compression molding of a powder of a metal 4 chelate or a processed material which forms a film is placed in a working fluid or a gas. And (b) a source device is connected to the electrode and the workpiece according to the helium gas, and a pulse-like discharge occurs between the electric device and the device, and the discharge energy is formed by the electrode material on the surface of the workpiece. Or a discharge surface treatment apparatus in which an electrode material is reacted by a discharge energy to form a film, wherein the electrode ' is formed to have a volume ratio of the electrode material to the electrode material of 25 to 65%. The surface treatment device is a processed product in which a powder of a working fluid compound is compression-molded, and the electrode is discharged by the power supply device described above, and the discharge electrode material or the electrode material is discharged by the discharge surface treatment device. It has the following thermal conductivity.
其次’有關本發明之放電表 中或氣體中配置有以金屬或金屬 壓粉體所成電極、及將形成被膜 電極及前述加工物按電氣性連接 與前述加工物之間發生脈衝狀之 量’而於前述加工物表面形成由 電能量而反應的物質所成被膜的 徵為··前述電極,具有1〇W/mK 315550 17 1284682 又,為達成上述目的起成,有關本發明之放電表面處 理用電極之評價方法,係以金屬或金屬化合物之粉末壓縮 成型的壓粉體作為電極,在加工液中或氣體中,使前述電 極與加工物之間發生放電,藉由其放電能量,而於前述加 工物表面形成由電極材料或電極材料因放電能量而反應的 物負所成被膜之用為放電表面處理用之放電表面處理電極 之評價方法,其特徵為:對前述電極徐徐加壓既定負荷, 根據前述電極表面即將產生龜裂時之壓縮強度,以評價能 否將既定之被膜形成於前述被加工物表面之電極。 [實施方式] 以下參考所附圖*,就彳關本發明之放電表面處理 用電極、放電表面處理用電極之製造方法與評價方法、放 電表面處理裝置以及放電表面處理之合適的實施形態,加 以詳細說明。 實施形態1 首先,就本發明所用之放電表面處理與其裝置之概 要’加以說明。第lgI,係表示在放電表面處理用裝置中 的放電表面處理之概略圖。放電表面處理裝置丨係具備: 欲形成被m 14的加工物(以了,簡稱工件)u、&為於工件 11表面形成被膜14之用的放電表面處理用電極12、以及 經按電氣性連接於卫件u及放電表面處理用電極η,而 為使兩者間發生電狐(叫放電而對兩者供給電壓的放電 表面處理用電源13 %接# ^ ^ _ π u所構成。如在液中實施放電表面處理 時按工件11及放電表面處理用電極12之與工件11相對 315550 18 1284682 向的部分能以油等之加工液15所裝滿之方式,再設置加工 槽16。又,如在氣體中實施放電表面處理時,則工件u 與放電表面處理用電極12,係置於處理氣氛中。在此,第 !圖及以下之說”,將例示加工液中實施放電表面處理 之情形。X,在下述中,有時將放電表面處理用電極簡稱 電極。再者,在下述中’將放電表面處理用電極匕與工件 11相對向的面之間的距離,稱為極間距離。 就此種構成之放電表面處理裝置i中的放電表 方法’加以說明。例如,以欲形成被膜14的卫件U作為 陽極’以成型有成為被膜14之供給源的金屬或陶究等之^ 均粒徑!〇nm至數…粉末的放電表面處理用電極12作 為陰極,將此等電極藉由未圖示的控制機構在加工液Η 2兩者不致於接觸之方式控制極間距離之下,使兩 發生放電,以實施。 如在放電表面處理用電極12與工件u之間發生放 ::則由於此種放電之熱而工件u及電極12之一部分即 、引1㈣此電極12之粒子間結合力弱時,則因放電所 、暴風或靜電力而所熔融的電極12之_部分 , =電子)21,即從電極12疏遠,而朝向工件η表面 移動。然後,電極粒子21到達工件η表面,則再行凝固, 並成為被膜14。又,疏遠的電極粒子 ^ , c , ^ 1之一部分在加工 、’乱體中之成7刀22起反應者23,亦將在工件η 膜/4。如此方式,即在工件11表面形成被膜 但’如電極12之粉末間之結合力強時,則僅靠因放電 315550 19 1284682 的爆風或靜電力尚不能剝取電極u τ 11 ^ Λ致不旎供給電極;^ 枓於.工件11。亦即’能否依放電表面處理开,…材 =,::來自電極12側的材料供給與其所供給材料::件 的炼融及與工件11材料的結合方式H在此 會對此電極材料之供給上有影響者,即為電極 度,亦即硬度。 之、m硬程 在此’就用為放電表面處理的放電 :製造方法之-例,加以說明。第2圖,係表示放電::2 ^用電極之製造過程的流程圖。首先,將具有欲於工件 1上形成被膜14之成分的金屬或陶变等的粉末,加以於 驟S1)。如由複數種成分所成時,則按能成為所希刀望 例之方式將各種成分之粉末混合並加讀碎1如 用球磨(Ban mill)裝置等粉碎機,將市面上流通的平均粒和 數十心之金屬或㈣等球形粉末加以粉碎為平均粒炉3 p以下。粉碎可在液體中實施,惟此時,則蒸發液體以 乾燥粉末(步驟S2p由於乾燥後之粉末,係粉末與粉末互 相凝聚而形成大塊之故,為將此大塊解碎之同時,為能使 下過程所使用的臘與粉末充分混合起見,加以過篩(步:驟 S3)。例如,於殘留有經凝聚的粉末之篩網上放置陶瓷球或 金屬球,並加以振動時,則經凝聚所成塊即因振動之能量 或與球之踫衝而解散,並通過網篩。通過網筛的粉末,始 能使用於下述步驟中。 在此,就經步驟3所粉碎的粉末過篩的工作,加以說 明。放電表面處理中,為使發生放電而施加於放電表面處 315550 20 1284682 理用電極12與工件U之間的電壓,通常係在8〇v至4〇〇v 之範圍如將此範圍之電壓施加於電極1 2與工件1 1之間, 則放電表面處理中之電極12與工件U之間的距離將成為 0.3mm程度。如上述,纟電表面處理中,可能因兩極間所 產生的電弧放電,而構成電極12的經凝聚所成塊,亦有照 原樣大小從電;^ 12㈤離的情形。在此,如成塊之大小在極 間距離以下(0.3mm以下)時,則即使在極間存在有成塊 時’仍可使下一個放電發生。又,由於放電係在距離近之 處毛生之故,存在有成塊之處發生放電,以致可能因放電 之熱能量或爆發力而可將其成塊細碎。 但,如構成電極12的成塊之大小在極間距離以上 (0.3mm以上)時,則因放電而其成塊照原樣大小從電極η 離脫,以致堆積於工件u上,或漂游在電極12與工件Η 間之加工液15所充滿的極間。如前者之方式大塊堆積時, 則由於放電係於電極工件u之距離最近之處發生之故,在 此部分集中放電而不會在其他處所發生放電,以致不能將 被膜U均勾堆積於工件n表面。又,此種大塊,由於過 大之故,放電之熱不能宗令、校%。m 个月b兀王熔融。因此,所形成的被膜μ 非常脆弱,可以手指所剝削之程度。又,如後者之方式, 大塊漂游在極間時,則引起電極12與工件丨丨間之短路, 以致不能發生放電。換言之,如欲獲得均勾形成被膜14 且安定的放電時’則構成電極的粉末中不可存在有因粉末 凝聚所形成之較極間距離以上為大的成塊。此種粉末之凝 聚容易發生在金屬粉末或導電性陶-亮之情形,而非導電性 315550 21 1284682 之情形則不容易發生。又,粉末之平均粒徑愈小,粉末之 凝聚愈容易發生。因此,為防止因此種粉末之凝聚所生成 之成塊所引起的放電表面處理中之缺點起見,需要有將步 驟S3中所凝聚的粉末加以過篩的步驟。從以上之結論可 知,如實施過篩時,則需要使用較極間距離為小的尺寸之 筛目。 其後’如欲改善在之後步驟中之加壓時對粉末内部的 加壓壓力傳遞時,視需要,對粉末摻入石臘(paraffin)等臘 按重置比1%至10%程度(步驟S4)。如將粉末與臘混合時, 雖然可改善成型性,惟由於粉末周圍再度為液體所包覆之 故,因其分子間力或靜電力之作用而凝聚,以致形成大塊。 於疋再度為了將所凝聚的成塊解散起見,加以過筛(步驟 S5)。在此之過篩之方法係與上述的步驟的方法相同。 接著,將所得粉末使用壓縮加壓成型(步驟S6)。第3 圖,係依模式性表示將粉末成型時之成型器之狀態的剖面 圖。將下衝床104從形成在金屬模具(die,鍈)1〇5的孔下 邛插入,並對此等下衝床1〇4與金屬模具(鍈口 〇5所形成的 二間中填充經上述步驟S5所過篩的粉末(由複數種成分所 成時,則為粉末之混合物)丨〇丨。然後,將上衝床i 〇3從形 成在金屬模具(鎮)1 〇5的孔上部插入。然後,使用加壓器等 從填充有此種粉末101的成型器之上衝床103及下衝床 104之兩側施加壓力,並將粉末1〇1壓縮成型。以下,將 經壓縮成型的粉末101簡稱壓粉體。此時,如增高加壓壓 力時,則電極102變硬,如降低加壓壓力時,則電極1〇2 315550 22 1284682 變軟。又,如電極材料之扒 电往材枓之叔末1〇1之粒徑 變硬,如粉末1〇1之赦赖士 # 貝1電隹12 之拉徑大時,則電極12變軟。 然後’從成型器取出壓粉體,使用真 爐加熱(步驟S7)。在加熱時,如 次風就矾之 提间加熱 >皿度,則雷搞1 2 變硬,如降低加熱溫度彳 、 j奄極12變軟。又,由W ‘航, 亦可降低電極12之電阻。因此,即使 =: 臘而廢縮成型時,加熱 4中不心入 φ ΛΛ ^ ^ ^ 负八心義由此,將進行壓粉體 中的叔末間之結合,而可製得具有導電性士 用電極12。 -有涂電I生之放電表面處理 另外’如’略上述之步驟Μ之粉碎步驟的情形,亦 即直接使用平均教;| + S3之過締牛:…粉末的情形,或省略步驟 b j之過師步驟而混扃古 ^ . · mm以上之大塊的情形,仍然 月匕成1放電表面處理用雷士 有如表面硬度稍:而Γ 其電極12’仍然存在 更度賴同而中心部之硬度低等硬度不均的問題。 又,由於難氧化的C05t Ni(鎳),此等合金 物以及陶竟之平均粒徑3…下之粉末多在市面上流通 =Γ用此種粉末時,可省略上述步驟si之粉碎步 驟與步驟S2之乾燥步驟。 且_=’就依上述方法所製造的放電表面處理用電極之 ==態:加以說明。實施形態1中,就構成電極 .\ :粒仫在5至10"m時,不會形成碳化物或難 於形成礙化物的铋极a , ^ m ;斗之比例、與電極之硬度、與由复 所形成的«厚度之間的關係,加以說明。 - 在本貫施形態1中,就改變不會形成碳化物的材料或 315550 23 1284682 難於形成碳化物的材料之成分的放電表面處理用電極,將 試驗其電極硬度、及依放電表面處理方法形成於加工物上 的被膜厚度之變化的結果,表示如下。用為試驗的放電表 面處理用電極之基材的材質,係CrsC2(碳化鉻)粉末,而對 此,作為不會形成碳化物或難於形成碳化物的材料而添加 C0粉末。所添加的Co係按體積在〇至8〇0/。之間改變,所 試驗的放電表面處理用電極之硬度則作成後述的既定硬 度。在此,電極係從粒徑在5//111之CrsC2粉末與粒徑在5 # m之Co粉末並按照第2圖之流程圖所製造者,惟在步 驟S1之粉末之粉碎步驟中,係依能製得粒徑為㈤之粉 末的條件下進行粉碎,在步驟84之與臘的混合步驟中, 混合2至3重量%之臘,在步驟S6之加壓步驟中,以約 lOOMPa之加壓壓力將粉末壓縮成型,而在步驟s7之加熱 步驟中,則以40(TC至80(rc之範圍改變加熱溫度。在此, 加熱溫度,係Che,粉末之比例愈高,作成溫度愈高,c〇 粉末之比例愈高則作成溫度愈低。此乃因Cr3C2粉末之比 例多時所製造的電極容易變脆,如以較低溫度加熱時則立 即崩潰,相對於此,如Co粉末之比例多時,即使加熱溫 度低’電極之強度仍然容易變強之故。 在此,本說明書中所用的體積比(體積0/〇),係指將所混 合的材料分別以其材料之密度相除的值之比例之意。具體 而言,如將材料複數種混合時,為各別之體積之比例本身, 而如材料係合金時,將合金中所含之各材料(金屬元素), 以各密度(比重)相除的值之比例作為體積%。換言之,體積 315550 24 1284682 比(體積%),係指將以作為目的成分之重量❶/g除以其成分之 密度的值’除以放電表面處理用電極所使用的各成分之重 量%分別除以其成分之密度所相除的值加以合計的值之 意。例如’本例之Cr3C2粉末與Co粉末之混合物中的Co 粉末之體積比(體積%),可以下式表示。Next, in the discharge meter according to the present invention, an electrode formed of a metal or a metal powder is disposed in the gas, and an amount of a pulse between the formed electrode and the processed material and the workpiece is electrically connected to the processed product. On the other hand, the electrode formed by the electric energy on the surface of the workpiece is formed into a film, and the electrode has 1 〇W/mK 315550 17 1284682. In order to achieve the above object, the discharge surface treatment of the present invention is concerned. In the evaluation method of the electrode, a powder compacted by a powder of a metal or a metal compound is used as an electrode, and a discharge occurs between the electrode and the workpiece in a working fluid or a gas, and the discharge energy thereof is used. The surface of the processed object is formed by a negative reaction of the electrode material or the electrode material due to the discharge energy, and is used as a coating surface for the discharge surface treatment electrode for the discharge surface treatment. The method is characterized in that the electrode is gradually pressurized with a predetermined load. According to the compressive strength when the surface of the electrode is about to be cracked, it is evaluated whether a predetermined film can be formed in the aforementioned processed The electrode on the surface of the object. [Embodiment] Hereinafter, an appropriate embodiment of a method for producing a discharge surface treatment, a method for producing a discharge surface treatment electrode, a discharge surface treatment device, and a discharge surface treatment according to the present invention will be described with reference to the accompanying drawings. Detailed description. Embodiment 1 First, the outline of the discharge surface treatment and the apparatus used in the present invention will be described. The first lgI is a schematic view showing the discharge surface treatment in the discharge surface treatment apparatus. The discharge surface treatment apparatus includes: a discharge surface treatment electrode 12 for forming a film 14 on the surface of the workpiece 11 to form a workpiece of m 14 (abbreviated as a workpiece), and an electrical property It is connected to the guard u and the discharge surface treatment electrode η, and is configured to generate an electric fox between the two, which is a discharge surface treatment power source that supplies a voltage to the discharge surface of the power supply 13 %# ^ ^ _ π u. When the discharge surface treatment is performed in the liquid, the machining chamber 16 can be further provided so that the portion of the workpiece 11 and the discharge surface treatment electrode 12 facing the workpiece 11 at 315550 18 1284682 can be filled with the machining liquid 15 such as oil. When the discharge surface treatment is performed in a gas, the workpiece u and the discharge surface treatment electrode 12 are placed in a processing atmosphere. Here, in the drawings and the following, "discharge surface treatment in the working fluid will be exemplified. In the following, the electrode for discharge surface treatment is abbreviated as an electrode. In addition, the distance between the surface of the electrode for discharge surface treatment and the surface of the workpiece 11 is hereinafter referred to as the inter-electrode. distance The discharge table method 'in the discharge surface treatment apparatus i having such a configuration' will be described. For example, the metal U or the ceramic material which is the supply source of the coating film 14 is formed by using the guard U to form the coating film 14 as the anode '. The discharge surface treatment electrode 12 having a particle diameter of 〇 nm to several is used as a cathode, and the electrodes are controlled by a control mechanism (not shown) so that the processing liquid Η 2 is not in contact with each other to control the interelectrode distance. The discharge occurs between the discharge surface treatment electrode 12 and the workpiece u.: Due to the heat of the discharge, the workpiece u and a portion of the electrode 12, that is, the lead (1) between the particles of the electrode 12 When the bonding force is weak, the portion of the electrode 12 that is melted by the discharge, the storm or the electrostatic force, = electrons 21, is alienated from the electrode 12, and moves toward the surface of the workpiece η. Then, the electrode particles 21 reach the workpiece η. The surface is solidified again and becomes the film 14. Further, one part of the alienated electrode particles ^, c, ^ 1 is processed in the 'disorderly body, 7 knives 22 as a reaction 23, and will also be in the workpiece η film / 4. In this way, that is, at work 11 The surface forms a film but if the bonding force between the powders of the electrode 12 is strong, the electrode u τ 11 ^ can not be stripped by the explosion or electrostatic force of the discharge 315550 19 1284682; Workpiece 11. That is, 'can be processed according to the discharge surface, ... material =,:: material supply from the electrode 12 side and the material supplied thereto:: the smelting of the piece and the combination with the material of the workpiece 11 H will be The influence on the supply of the electrode material is the electrode degree, that is, the hardness. The m hard path is used here as the discharge of the discharge surface treatment: the manufacturing method - an example, which is explained. Indicates the discharge:: 2 ^ Flow chart of the manufacturing process of the electrode. First, a powder having a metal or a ceramic or the like which is intended to form a component of the film 14 on the workpiece 1 is applied to step S1). When it is made up of a plurality of components, the powders of the various components are mixed and read and crushed in such a manner as to be a case of a knife. For example, a granulator such as a ball mill device is used to circulate the average particles on the market. And tens of heart metal or (four) spherical powder is pulverized to an average grain furnace of 3 p or less. The pulverization can be carried out in a liquid, but in this case, the liquid is evaporated to dry the powder (step S2p is a powder after drying, and the powder and the powder are agglomerated to each other to form a large mass, and the large mass is simultaneously broken. When the wax used in the next process is sufficiently mixed with the powder, it is sieved (step S3). For example, when a ceramic ball or a metal ball is placed on a sieve on which the coagulated powder remains, and vibrated, Then, the agglomerated piece is disintegrated by the energy of the vibration or the impact of the ball, and passes through the mesh screen. The powder passing through the mesh can be used in the following steps. Here, it is pulverized by the step 3. The operation of powder sieving is explained. In the surface treatment of discharge, the voltage applied between the electrode 12 and the workpiece U is applied to the discharge surface for discharge to occur, usually between 8 〇v and 4 〇〇v. If the range is such that a voltage of this range is applied between the electrode 12 and the workpiece 11, the distance between the electrode 12 and the workpiece U in the discharge surface treatment will be about 0.3 mm. As described above, in the surface treatment, May be caused by the two poles The arc discharge, and the agglomerated blocks constituting the electrode 12 are also separated from the original size by the electric power; ^ 12 (five). Here, if the size of the block is less than the distance between the poles (0.3 mm or less), even if When there is a block between the poles, the next discharge can still occur. Moreover, since the discharge system is in a close proximity, there is a discharge in the block, so that the thermal energy or explosive force may be caused by the discharge. However, if the size of the block constituting the electrode 12 is greater than or equal to the distance between the electrodes (0.3 mm or more), the block is separated from the electrode η by the discharge due to the discharge, so that it is deposited in the block. The workpiece u is floated between the electrodes 12 and the workpieces 15 between the electrodes 12 and the workpieces. When the bulk is stacked as in the former, the discharge is caused by the closest distance to the electrode workpiece u. This part is concentrated in discharge and does not discharge in other places, so that the film U cannot be stacked on the surface of the workpiece n. Moreover, due to the large size, the heat of discharge cannot be ordered or corrected. The moon b 兀 熔融 melting. Therefore, the The formed film μ is very fragile and can be exploited by the fingers. Moreover, in the latter way, when the bulk floats between the poles, a short circuit between the electrode 12 and the workpiece is caused, so that discharge cannot occur. In other words, if desired When a discharge is formed in which the film 14 is formed and stabilized, the powder constituting the electrode is not likely to have a large agglomerate formed by the agglomeration of the powder, and the agglomeration of the powder is likely to occur in the metal powder or the conductive material. In the case of sex ceramics - bright, but not conductive 315550 21 1284682, the smaller the average particle size of the powder, the more easily the aggregation of the powder occurs. Therefore, in order to prevent the aggregation of the powder For the disadvantages of the discharge surface treatment caused by the agglomeration, a step of sieving the powder agglomerated in the step S3 is required. From the above conclusions, it is known that when sieving is carried out, it is necessary to use a mesh having a smaller distance between the electrodes. Thereafter, if it is desired to improve the pressure transfer to the inside of the powder during pressurization in the subsequent step, if necessary, the powder is blended with paraffin or the like by a reset ratio of 1% to 10% (steps) S4). When the powder is mixed with the wax, although the moldability can be improved, since the powder is coated with a liquid again, it is agglomerated by the action of its intermolecular force or electrostatic force, so that a large mass is formed. Yu Yu once again screened for the dissolution of the agglomerated pieces (step S5). The method of sieving here is the same as the method of the above steps. Next, the obtained powder is subjected to compression press molding (step S6). Fig. 3 is a cross-sectional view schematically showing the state of the former when the powder is molded. The lower punch 104 is inserted from the hole formed in the die 1 〇 5, and the lower punch 1 〇 4 and the metal mold (the two compartments formed by the 〇 〇 5 are filled in the above steps The powder sieved by S5 (when a plurality of components are formed, it is a mixture of powders). Then, the upper punch i 〇 3 is inserted from the upper portion of the hole formed in the metal mold (town) 1 〇 5. Then Pressure is applied from both sides of the punch 103 and the lower punch 104 on the former filled with the powder 101 using a pressurizer or the like, and the powder 1〇1 is compression-molded. Hereinafter, the compression-molded powder 101 is referred to as a press. At this time, if the pressure is increased, the electrode 102 becomes hard. If the pressure is lowered, the electrode 1 〇 2 315550 22 1284682 becomes soft. The particle size of the final 1 〇 1 becomes hard, such as the powder 1 〇 1 赦 赖 士 # 贝 1 隹 隹 之 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 12 Heating (step S7). When heating, such as the secondary wind, the heating of the room is increased, and the degree of the dish is 1 2 Hardening, such as lowering the heating temperature 彳, j 奄 12 softening. Also, by W 'voyage, can also reduce the resistance of the electrode 12. Therefore, even if =: wax and shrink molding, heating 4 is not φ ΛΛ ^ ^ ^ Negative Eight Hearts Thus, the combination of the tertiary and the final ends in the pressed powder can be obtained, and the conductive electrode 12 can be obtained. Slightly the above steps Μ the pulverization step, that is, directly using the average teaching; | + S3 through the cattle: ... powder situation, or omitting step bj through the division steps and mixing the ancient ^. · mm or more In the case of a block, it is still a month of discharge. The surface of the discharge is similar to that of the NVC: and the electrode 12' still has a problem of uneven hardness such as a lower hardness and a lower hardness at the center. C05t Ni (nickel), such alloys and ceramics under the average particle size of 3...the powder is mostly in the market. If the powder is used, the pulverization step of the above step si and the drying step of step S2 may be omitted. And _=' electrode for discharge surface treatment manufactured by the above method == state: To be explained, in the first embodiment, the electrode is formed. When the particle is at 5 to 10"m, no carbide or a bungee a, which is difficult to form a barrier, is formed; The relationship between the hardness of the electrode and the thickness formed by the complex is explained. - In the present embodiment 1, the material which does not form carbide is changed or the material which is difficult to form carbide is 315550 23 1284682 The results of the change in the electrode hardness of the component and the thickness of the film formed on the workpiece by the discharge surface treatment method are shown below. The material of the substrate used for the electrode for discharge surface treatment to be tested was CrsC2 (chromium carbide) powder, and thus C0 powder was added as a material which does not form carbides or is difficult to form carbides. The added Co is in the range of 〇 to 8〇0/. The hardness of the electrode for discharge surface treatment to be tested was changed to a predetermined hardness as described later. Here, the electrode is produced from a CrsC2 powder having a particle diameter of 5//111 and a Co powder having a particle diameter of 5 #m and manufactured according to the flow chart of Fig. 2, except in the pulverization step of the powder in the step S1. The pulverization is carried out under the condition that the powder having the particle diameter of (5) is obtained, and in the mixing step with the wax in the step 84, 2 to 3 wt% of the wax is mixed, and in the pressurizing step of the step S6, the addition is performed at about 100 MPa. The pressure is compressed to form the powder, and in the heating step of step s7, the heating temperature is changed by 40 (TC to 80 (the range of rc. Here, the heating temperature is Che, the higher the proportion of the powder, the higher the temperature is. The higher the ratio of c〇 powder, the lower the temperature is. This is because the electrode made by the ratio of Cr3C2 powder is easy to become brittle, and if it is heated at a lower temperature, it immediately collapses. In contrast, such as Co powder When the ratio is large, even if the heating temperature is low, the strength of the electrode is still easily increased. Here, the volume ratio (volume 0/〇) used in the present specification means that the materials to be mixed are respectively in the density of the material thereof. The meaning of the ratio of the value to be divided. Specifically, if the material is complex In the case of a plurality of types of mixing, the ratio of the respective volumes is itself, and in the case of a material-based alloy, the ratio of the values of the respective materials (metal elements) contained in the alloy divided by the respective densities (specific gravity) is taken as the volume %. In other words, the volume ratio of 315550 24 1284682 (% by volume) is defined by dividing the value ❶/g as the target component by the density of the component's by the weight % of each component used for the electrode for discharge surface treatment. The value obtained by dividing the density of the components is a total of values. For example, the volume ratio (% by volume) of the Co powder in the mixture of the Cr3C2 powder and the Co powder of the present example can be expressed by the following formula.
Co之重量%Co% by weight
Co之體積% _TCo之密度_Co% of volume _TCo density_
Cr3C2之重量% + Co之重量%、 ι*3〇:2之密度+7。之密度) 從此式可知,如作為合金混合的材料之原來之密度係 相接近的材料,則當然與重量%略為相同的值。 在此’就本實施形態1的放電表面處理時之放電脈衝 條件’加以說明。第4A圖及第4B圖,表示放電表面處理 時之放電脈衝條件之一例的圖,第4a圖表示放電時施加 於放電表面處理用電極與工件之間的電壓波形,而第4b 圖表示放電時對放電表面處理裝置所流動的電流之電流波 形。如第4A圖所示,在時刻t〇對兩極間施加無負荷電壓 ui ’惟在放電滯後時間(time lag)td經過後之時刻^,對兩 極間開始流動電流,而開始放電。此時之電壓為放電電壓 ue ’而此時所流動的電流為峰值(peak)電流值ie。然後, 如在時刻q對兩極間的電壓之供給停止時,電流即不會流 動。亦即,放電即停止。在此,稱為脈衝寬度te。將 此時刻tG至q的電壓波形,隔著靜止時間%反複施加於兩 極間。亦即,如第4A圖所示,在放電表面處理用電極η 25 315550 1284682 與工件11之間,施加脈衝狀之電壓。在本例中,在放電表 面處理時所使用的放電脈衝條件,係作成峰值電流值 ^=10Α、放電持續時間(放電脈衝寬度)te = 64// s,靜止時間 t〇 128 // s。又,在試驗時,使用1 5mmx 1 5mm之面積之電 極’對工件11實施放電表面處理1 5分鐘。 第5圖,係表示對本身為碳化物的Cr3C2粉末中使難 以形成碳化物的c〇粉末量改變以製造的放電表面用電極 中的因C〇量之變化所引起的被膜厚度之關係圖。在第5 圖中,橫軸表示放電表面處理用電極中所含之體積%, 縱軸係以對數刻度表示形成於加工物的被膜之厚度(# m)。 “依據上述之放電脈衝條件以形成被膜時,因所製造的 電極内所含有的c〇之體積%而形成於工件上的被膜之厚 度不相同。在第5圖中,表示如Co含量在10體積%以下 時被膜厚度在1G"m程度者,從C。含量30體積%程度起 逐漸增厚,從Co含量超過4()體積_近起會增厚至1〇_ # m的情形。 ’ 關於此點,再詳細加以探討。如依據上 料,如電極内之C。含量在0體積%時,亦即 3 末為1〇〇體積%時’能形成被膜之厚度係程 度為/、界限’而不能再增加其厚度。 碳化係表示放電表面處理用電極中未含不會形成 被膜形成之二或難以形成碳化物的材料情形對處理時間的 料成之情況圖。在第6圖中,橫轴表示對每單位面積 315550 26 1284682 之實施放電表面處理的處理時間(分鐘/cm2)、縱軸表示以 實施放電表面加工處理前之工件表面之位置作為基準時之 被膜厚度(工件之表面位置)(em)。如第6圖所示,在放電 表面處理之初期階段,被膜將隨著時間一起成長而增厚, 惟在某處(約5分鐘/cm2)即飽和。其後被膜厚度暫時不會 成長,惟如某時間(約20分鐘/cm2;)以上繼續放電處理時, 則被膜厚度開始減少,最後被膜厚度即成為負I,而變成 挖深亦即去除加工。但’即使變成去除加工的狀態下,實 際上仍然存在有工件上之被帛’而具有10// m程度之厚 度。亦即,被膜之厚度幾乎與以適當時間(處理時間為5至 刀4里/cm之間)處理的狀態相同。從此種結果來看,$ 至20分鐘之間的處理時間較為適當。 回頭看第5圖可知,電極内隨著增加難以形成碳化物 的材料之C。量即可開始增厚被膜,而如電極中的Co含量 超過3〇體積%即所形成的被膜厚度開始增厚,並超過40 :㈣即可安定並容易形成厚膜。第6圖中,雖記載為c〇 3置從30體積%程度開始順利增厚膜厚,惟 行複數以試驗的平均值,而實際上,^。含量在 %程度時’有被膜不會增厚的情形,或即被 膜強度仍然脆弱,亦即容易以今屬以“/的Β被 情形,以致不能安定。田 專強力摩擦而去除的 以上。 而,杈佳為Co含量在40體積〇/〇 此方式i曰加被膜中作為金屬殘留 含有未成為碳化物的全屬^…睹 即可形成 扪至屬成刀的被膜,而容易安定地形成 315550 27 1284682 厚膜。 弟7圖表示使用Co含量在π ± ^ 里隹/υ體積。〆〇之電極實施放電 表面處理時所形成的被膜照片。 乃°亥恥片係例示厚膜之形成 者’而顯示形成有2mm程度之厚膜的情形。該被膜係經 分鐘之處理時間所形成者,惟如增長處理時間,則可形 成更厚的被膜。 如此方式,如使用電極内含有c〇等之難以形成碳化 物的材料或不會形成碳化物的材料4〇體積%以上的電 極,即可依放電表面處理而在工件上安定地形成厚的被 膜。 上述之例,係就作為難以形成碳化物的材料而使用c〇 的情形加以說明者,惟如使用Ni、Fe(鐵)、AI(鋁)、Cu(銅广Weight % of Cr3C2 + % by weight of Co, ι * 3 〇: density of 2 + 7. Density) From this formula, it is understood that the material having the same density as the material to be alloyed is of course slightly the same as the weight %. Here, the "discharge pulse condition" at the time of discharge surface treatment in the first embodiment will be described. 4A and 4B are views showing an example of discharge pulse conditions at the time of discharge surface treatment, and FIG. 4a shows a voltage waveform applied between the discharge surface treatment electrode and the workpiece during discharge, and FIG. 4b shows discharge. A current waveform of a current flowing to the discharge surface treatment device. As shown in Fig. 4A, the no-load voltage ui ’ is applied between the two electrodes at time t 惟, but at the time after the discharge lag time td elapses, a current flows between the two electrodes, and discharge starts. The voltage at this time is the discharge voltage ue ', and the current flowing at this time is the peak current value ie. Then, if the supply of the voltage between the two poles is stopped at time q, the current does not flow. That is, the discharge is stopped. Here, it is called a pulse width te. The voltage waveform at this time tG to q is repeatedly applied between the two electrodes with a rest time %. That is, as shown in Fig. 4A, a pulse-like voltage is applied between the discharge surface treatment electrode η 25 315550 1284682 and the workpiece 11. In this example, the discharge pulse conditions used in the discharge surface treatment were set to a peak current value of ^=10 Α, a discharge duration (discharge pulse width) te = 64//s, and a rest time t〇 128 // s. Further, at the time of the test, the workpiece 11 was subjected to discharge surface treatment for 15 minutes using an electrode of an area of 15 mm x 15 mm. Fig. 5 is a graph showing the relationship between the thickness of the film due to the change in the amount of C〇 in the electrode for a discharge surface produced by changing the amount of the c〇 powder which is difficult to form a carbide in the Cr3C2 powder which is itself a carbide. In Fig. 5, the horizontal axis represents the volume % contained in the electrode for discharge surface treatment, and the vertical axis represents the thickness (# m) of the film formed on the workpiece in a logarithmic scale. "When the film is formed according to the discharge pulse conditions described above, the thickness of the film formed on the workpiece due to the volume % of c〇 contained in the electrode to be produced is different. In Fig. 5, the content of Co is 10 When the film thickness is less than or equal to 5% by volume, the thickness is gradually increased from the C content of 30% by volume, and the Co content is increased by more than 4 () volume _ close to 1 〇 _ # m. In this regard, we will discuss it in detail. For example, according to the feeding, such as C in the electrode, when the content is 0% by volume, that is, when the end of 3 is 1% by volume, the thickness of the film can be formed as /, the limit 'The thickness can't be increased. The carbonization system shows a case where the electrode for discharge surface treatment does not contain a material which does not form a film formation or a material which is difficult to form a carbide, and the processing time is shown. In Fig. 6, The horizontal axis represents the processing time (minutes/cm 2 ) of the discharge surface treatment per unit area of 315550 26 1284682, and the vertical axis represents the film thickness when the position of the workpiece surface before the discharge surface processing is performed as a reference (table of the workpiece) Position) (em). As shown in Fig. 6, in the initial stage of discharge surface treatment, the film will grow thicker with time, but it will be saturated somewhere (about 5 minutes/cm2). If it does not grow for a while, if the discharge process continues at a certain time (about 20 minutes/cm2;), the thickness of the film begins to decrease, and finally the film thickness becomes negative I, and the depth of the hole is removed, that is, even if it becomes In the state where the processing is removed, there is actually a bedding on the workpiece, and the thickness is about 10/m. That is, the thickness of the film is almost equal to the appropriate time (the processing time is 5 to 4 liters/cm). The processing state is the same. From this result, the processing time between $ and 20 minutes is more appropriate. Looking back at Figure 5, it can be seen that the amount of C in the electrode is increased with the increase of carbides. Thickening the film, and if the Co content in the electrode exceeds 3% by volume, the thickness of the formed film begins to increase, and if it exceeds 40: (4), it can be stabilized and a thick film is easily formed. In Fig. 6, although it is described as c〇 3 set to open from 30% by volume The thickness of the film is increased smoothly, but the average value of the test is performed. In fact, when the content is at a level of %, there is a case where the film is not thickened, or the film strength is still weak, that is, it is easy to be With the situation of "/, it is impossible to settle. Tian special strong friction and removed above. On the other hand, the Co content is 40 volume 〇 / 〇 in this way, as a metal residue containing all the non-carbides, it is possible to form a film which is a knives, and it is easy to form stably. 315550 27 1284682 Thick film. Figure 7 shows the use of the Co content in π ± ^ 隹 / υ volume. The electrode of the crucible is subjected to a photo of the film formed during the discharge surface treatment. In the case where the formation of a thick film is exemplified as a thick film, a thick film of about 2 mm is formed. The film is formed by a processing time of a minute, but if the treatment time is increased, a thicker film can be formed. In such a manner, if a material containing a carbide which is difficult to form a carbide such as c 或 or an electrode which does not form a carbide is used, it is possible to form a thick film on the workpiece by discharge surface treatment. . The above examples are described using c〇 as a material that is difficult to form carbides, but using Ni, Fe (iron), AI (aluminum), and Cu (copper).
Zn(鋅)等時,亦獲得同樣結果。 另外,在此所稱厚膜,係指組織内部(因脈衝狀之放電 所形成的被膜之故,最外表面之面粗糙度不佳,外觀似乎 不具有光澤)能具有金屬光澤的緻密的被膜之意。例如,如 C〇等難於形成碳化物的材料之含量較少的情形,如減弱電 極強度(硬度)’有時工件上之附著物能增厚。但此種附著 物並非緻密的被膜,而如以金屬片等摩擦時即會容易去除 者,此種被膜不屬於本發明所稱之厚膜。同樣,由於上述 之專利文獻1等所記載的堆積層實係並非緻密的被膜,容 易以金屬片等之摩擦所去除者之故,此種被膜亦不屬於本 發明所稱的厚膜。 又’在上述說明中,係就經Cr3C2粉末壓縮成型後加 28 315550 1284682 說明者’惟有時直接將經壓縮成 。但’為形成緻密的厚膜時,則 不宜’而需要適當硬度之故,一 熱以製造電極的情形加以 型的壓粉體作為電極使用 電極之硬度過硬或過軟均 般需要加熱處理。壓粉體之‘办士 & 、 !物篮之加熱直接對成型之維持或固形 化有益。 該電極之硬度,係與電極材料之粉末之結合強度有 關,關係到因放電所引起的電極材料對工件側的供給量。 如電極硬度高時,由於電極材料之結合強之故,即使發生 放電仍然僅能釋出少量電極材料,以致不能實施充分^被 膜形成。相反地’如電極強度低時,由於電極材料之結合 弱之故,如發生放電時則供給大量材料,而如此量過多時: 此等材料不能充分由放電脈衝之能量所熔融,以致不能形 成緻密的被膜。 如使用同樣原料而同樣粒徑之粉末時,對電極硬度, 亦即電極材料之結合狀態有影響的參數(parameter),係加 壓壓力與加熱溫度。在本實施形態! 係作為加壓壓力 之例而使用約1 OOMPa者,惟如將此加壓壓力增高,則即 使降低加熱溫度仍能獲得同樣硬度。相反地,如降低加壓 壓力’則需要設定加熱溫度為較高之方式。 又,在本實施形態1中,係作為放電表面處理時之放 電脈衝條件之例而表示以i種條件下的試驗結果者,惟被 膜之厚度雖會有所不同,在其他條件下,當然亦可獲得同 樣結果。 如上所述,可知在厚膜形成上,材料方面的條件甚為 315550 29 1284682 重要’惟亦已知在放電表面處理、特別是厚膜形成時,其 他條件亦屬極為重要者。通常,纟電表面處理用電極,係 遵循上述的第2圖之流程圖,將粉末材料壓縮成型、加熱 以製造電極。其時,—般多以壓縮成型時之加壓壓力與加 熱處理時之加熱溫度以決定電極之狀態。亦即,先前之電 極狀4之管理係使用以加壓壓力與加熱溫度等% ^條件所 成型的電極以進行被膜形成,並依其狀態而加以判斷者。 但’此種方法係為電減態之管理起見需要形成被膜,而 頗費工夫。於是’本發明人等為作為管理電極狀態,就⑴ 電極之電阻、(2)電極之彎曲試驗,以及⑺電極之硬度試驗 方法,加以檢討。 〜百先,(1)之電阻,係將放電表面處理用電極裁切為既 ^形狀,以測定電阻之方法。電阻具有如放電表面處理用 電極愈堅固結硬則會愈小的傾向,故雖然可成為放電表面 處理用之強度之良好指標,惟由於測定上容易有偏差,受 材料之物性值影響之故,不同材料時會有不同值,需要按 每種不同材料掌握最適狀態時之值等,有諸多問題。 其次’(2)之彎曲試驗,係將放電表面處理用電極按既 疋之形狀裁切並實施三點彎曲試驗,以測定對彎曲的阻力 的方法。本方法有測定上容易有偏差,測定上耗費較大, 荨問題。 而’最後之(3)之硬度試驗,有對放電表面處理用電極 按住壓頭(indenter),依其壓痕之形狀測定硬度的方法,或 使用錯筆等之量具抓傷放電表面處理用電極並由有否傷痕 30 315550 !284682 以判斷的方法等。 此等3種方法係互相具有強相關者,惟由測定之簡易 性等之理由,發現採用(3)之鉛筆等量具的硬度試驗以判斷 放電表面處理用電極之狀態的方法最為合適。於是,就電 極之硬度與由該電極所形成的被膜之性質之關係,加以說 明如下。在此,下述之作為電極之硬度之基準所使用的指 標,如係構成電極的粉末之粒徑大且電極軟時,採用jis K5 600-5.4中的塗媒用船筆抓傷試驗,如係構成電極的粉 末之粒徑小且電極硬時,則採用洛式硬度(R〇ckweii hardness)。上述之JIS K56〇〇_5_4之規格,本來係塗被膜 之評價上所使用者,惟硬度低的材料之評價上很合適。當 然’其他硬度評價方法之結果與此種塗膜用錯筆抓傷試驗 :結果係可互為換算者’當然,可將其他硬度評價方法作 為指標使用。 如上述,為形成厚膜 丄 材料方面的條件甚為重要, 視實驗的情形’如係厚膜形成的情形時其他條件,特別是 硬度亦極為重要。就藉由放電表面處理的厚膜之形 ^放電表面處理用電極之硬度之間的關係、,作為例而將 r3 2 3 0%至Cg7G%之體積比所製造的放電表 =之情形,加以舉例說明。第8圖,係表示改變叫3二 〇 70%之體積比之放電表面處理用電極之 膜形成之狀態圖。在第8圖中,橫 予 用的塗膜用鉛筆之硬度所測定的放電表:平價所 度’愈往…,愈往…軟。= 315550 31 1284682 :用電極所形成的被膜之厚度之評價狀態。當實施此種 試驗時之放電表面處理時所使用的放電之脈衝條件, 放電持續時間(放電脈衝時間)㈣4 A S、靜止時間t ;= 1 ) r 〇 28# s。又’在評價試驗中,係使用15mm X 15mm之面積之電極,形成被膜。 如第8圖所示,放電表面處理用電極之硬度在4B至 ^程度之硬度之情形下被膜之狀態非常良好,而形成有緻 在、予膜。又’放電表面處理用電極之硬度在B至化之 亦可形成良好的厚膜在此範圍下,隨著結硬, 被膜之形成速度有緩慢的傾向,B程度之硬度下1厚膜 之形成將相當困難。如再較B為硬時,則不可能形成厚膜, 以致隨著放電表面處理用電極之硬度結硬,即將一邊去除 工件(work),一邊進行加工之方式。 ’ 另一方面’即使放電表面處理用電極之硬度在⑽程 2之硬度,仍然能形成良好的厚膜,惟如分析組織 發現被膜中有逐漸增加μ的傾向。再者,如放電表^ 理用電極之硬度較9Β程度為軟,則有電極成分不能充广 熔融而直接附著於工件上的頦參 日丨a 乃 仵上的現象,則破膜即成為非緻密之 夕孔性(P_US)者。在此,上述之放電表面處理用電極之 硬f與被膜之狀態間的關係’係視所使用的放電脈衝條件 而:少會變化’而如使用適當的放電脈衝條件時,則可擴 大能形成某些程度良好的被膜的範圍。本發明人 ’、 上述傾向,並W構成電極之材料,而從平均隸5:’ β m大小之粉末所製造的電極所具有。 315550 32 !284682 如採用本實施形態i,而使用粒徑在5至l〇//m之粉 末,對構成放電表面處理用電極的材料中添加c〇、Ni、Fe、 Cu、Zn等不會形成碳化物的材料或難以形成碳化物的 二枓40體積%以上,按能成為依塗膜用錯筆刮痕試驗的硬 在B至8B之間,杈佳為能成為4B至7B之間的硬度之 方式製造放電表面處理用電極,並使用此種放電表面處理 用電極以實施放電表面處理,即可具有在工件上安定地形 成厚膜的效果。如使用此種放電表面處理用電極,即能替 代焊接或火焰噴塗法之作堂, , 、 業並此將先前依靠焊接或火焰 T塗法所作的作業加以製程化。 放電表面處理上,能否因放電而從電極釋出電極材 =’端視構成電極的粉末之結合強度。亦即,如結合強度 則容=難於因放電之能量所釋出,惟如結合強度弱, :又’此種結合強度係因構成電極的粉末之大 在常i :不同f列如’構成電極的粉末之粒徑大時,由於 末互相結合的點之數目減少之故,電極強度 冓成電極的粉末之粒徑小時,由於在電極中的 : ^ 口的點之數目增多之故,電極強度會增強。因 二能否從電極釋出電極材料,係因粉末之 ΐ下至Γ呈度之粉末時,依塗膜用錯筆到痕試驗的硬 度下在Β至8Β之硬度者成 中,則就粒徑在1JL 5”時之…:在本貫施形態2 #時之電極硬度與被膜厚度加以 315550 33 1284682 說明。 在此’例舉按既定比例含有Co、Cr、Ni等成分的合 金粉末,例如使用霧化(atomize)法或磨子(^⑴等(按粉粒 能成為3 // m程度之方式)加以粉碎、混合,依照實施形態 1之第2圖之流程圖以製造放電表面處理用電極的情形。 但,在步驟S4之與臘的混合步驟中,係將2至3重量%之 臘混合,在步驟S6之加壓步驟中,依約i〇〇Mpai加壓壓 力將製作電極時之粉末壓縮成型,在步驟S7之加熱步驟 中,係使加熱溫度在60(TC至8〇〇t之範圍變化。另外,在 =種電極之製造中,可省略步驟S7之加熱步驟,而將混 合粉末壓縮成型並將所得壓粉體作為電極使用。又,上述 之合金粉末之組成,係Cr20重量%、Ni 1〇重量%、w(鎢)15 重量。/〇、Co 55重量%,而此時之c〇體積%為4〇%以上。 使用所製造的電極實施放電表面處理時之放電脈衝條 件,係在第4A圖及第4B圖中,作成峰值電流值ie=i〇A、 放電持續時間(放電脈衝寬度)te = 64 # s、靜止時間 8 。,使用15mm之面積之電極,形成被膜。 其結果,雖然電極材料係由粉末所構成者,惟由於使用合 金粉末化者而材質均一無偏差之故,能形成於成分上益偏 差的良質被膜。 、當然,&能成為既定之組成之方式所冑量的各材料之 粉末(在此為Cr粉末、Ni粉末、w粉末、c。粉末)混合以 ^造電極時’亦能製造同樣的電極。纟,由於會有粉末之 混合偏差等問題之故,不能避免性能會若干降低。 315550 34 1284682 上述說明中,係使用使Cr 20重量%、犯i 〇重量。 W 15重量%、其餘為c〇之比例之粉末化的材料者里^、 粉末化之合金組成並不限定於此,而可為例如& 25重: %、Ni10重量%、W7重量%、其餘為c〇之比例之合金量 或M〇28重量%、Cr 17重量%、Si(石夕)3重量%、其餘、 C 〇之比例之合金、或C r i 5重量%、F e 8重量% /其餘為 '之比例之合金、或Cr21重量%、M〇9重量m⑷* 重量%、其餘為Ni之比例之合金、或CM9重量%、妬Μ 重量❶/pM〇3重量%、(Cd(鎬)+ Ta)5重量%、Ti〇 8重量%、 A10.6重量%、其餘為Fe之比例之合金等按體積% 屬於難以形成碳化物的元素之C〇、Ni、卜、八卜Cu、〜 為40%以上者即可。 n 仁,由於合金比例不相同,則材料之硬度等之性質會 不相同之故,電極之成型性或被膜之狀態上多少會產^ 異。例如,電極材料之硬度硬時,則使用加壓的粉末之成 型將有困難。X ’如藉由加熱處理以增加電極之強度時, 則需要設法將加熱溫度增高-些。舉例而言,Cr 25重量 °/〇、Ni 10重量%、w 7重量%、其餘為c。之比例之合金得 較軟,而M。28重量%、Cr 17重量%、& 3重量%、其餘 為之比例之合金係較硬的材料,但在為給與電極所需 要的電極之加熱處理中,需要將後者之溫度較前者為平均 約高100°c前後之方式設定溫度。 又,厚膜之形成之容易度,係如實施形態丨所示,隨 之量增高而更為容易。電極成分之合金粉 35 315550 1284682 末所3材料而言,屬於難以形成碳化物的材料之Co、Ni、The same result was obtained also when Zn (zinc) or the like. In addition, the term "thick film" as used herein refers to a dense film which can have a metallic luster inside a tissue (a film formed by a discharge of a pulsed shape, a surface roughness of the outermost surface is not good, and the appearance does not appear to be glossy). The meaning. For example, in the case where the content of a material which is difficult to form a carbide such as C 较少 is small, such as attenuating the electrode strength (hardness), the deposit on the workpiece may be thickened. However, such an adherent is not a dense film, and if it is rubbed with a metal sheet or the like, it is easily removed. Such a film is not a thick film as referred to in the present invention. In the same manner, the deposited layer described in the above-mentioned Patent Document 1 or the like is not a dense film, and it is easy to remove the friction by a metal piece or the like, and such a film is not a thick film as referred to in the present invention. Further, in the above description, it is described that after compression molding of Cr3C2 powder, 28 315 550 1284682 is added, but it is sometimes directly compressed. However, in order to form a dense thick film, it is not preferable to require a proper hardness, and a powder compacted body is used as an electrode in the case of manufacturing an electrode. The hardness of the electrode is too hard or too soft, and heat treatment is required. The heating of the ‘ 士士 & 、 basket of the powder compact is directly beneficial to the maintenance or solidification of the forming. The hardness of the electrode is related to the bonding strength of the powder of the electrode material, and is related to the supply amount of the electrode material to the workpiece side due to the discharge. When the hardness of the electrode is high, since the bonding of the electrode material is strong, even if the discharge occurs, only a small amount of the electrode material can be released, so that sufficient film formation cannot be performed. Conversely, if the electrode strength is low, due to the weak combination of the electrode materials, a large amount of material is supplied when the discharge occurs, and when the amount is too large: these materials cannot be sufficiently melted by the energy of the discharge pulse, so that denseness cannot be formed. The film. When a powder having the same particle diameter and the same particle diameter is used, a parameter which affects the electrode hardness, that is, the bonding state of the electrode material, is a pressing pressure and a heating temperature. In this embodiment! As an example of the pressurizing pressure, about 100 MPa is used, but if the pressurizing pressure is increased, the same hardness can be obtained even if the heating temperature is lowered. Conversely, if the pressure is lowered, it is necessary to set the heating temperature to be higher. Further, in the first embodiment, the test result under the conditions of i is shown as an example of the discharge pulse condition at the time of discharge surface treatment, but the thickness of the film may vary, and under other conditions, of course The same result can be obtained. As described above, it is known that the material condition is very high in the formation of a thick film. 315550 29 1284682 Important It is also known that other conditions are also extremely important in the treatment of discharge surfaces, particularly thick film formation. Usually, the electrode for electric surface treatment is subjected to compression and molding and heating of the powder material in accordance with the flow chart of Fig. 2 described above to produce an electrode. At this time, the state of the electrode is determined by the pressurization pressure at the time of compression molding and the heating temperature at the time of heat treatment. That is, the management of the prior electrode 4 uses an electrode formed by a pressure and a heating temperature, etc., to form a film, and judges according to the state. However, this method requires the formation of a film for the management of electrical subtraction, and it takes a lot of work. Then, the inventors of the present invention reviewed the resistance of (1) the resistance of the electrode, (2) the bending test of the electrode, and (7) the hardness test method of the electrode as the state of the management electrode. ~100 first, (1) The resistance is a method of cutting the surface of the discharge surface treatment into a shape to measure the resistance. The electric resistance has a tendency to become smaller as the electrode for discharge surface treatment becomes stronger and stronger. Therefore, although it is a good indicator of the strength of the discharge surface treatment, it is easily affected by the measurement, and is affected by the physical property value of the material. Different materials have different values, and it is necessary to grasp the value of the optimum state for each different material, and there are many problems. Next, the bending test of (2) is a method in which the electrode for discharge surface treatment is cut in a shape of a crucible and a three-point bending test is performed to measure the resistance to bending. This method has a tendency to be biased in measurement, and the measurement is expensive and has a problem. In the final (3) hardness test, there is a method of measuring the hardness according to the shape of the indenter by pressing the electrode for the discharge surface treatment, or using a measuring instrument such as a wrong pen. The electrode is determined by the method of judging whether there is a scratch 30 315550 !284682. These three methods are strongly related to each other, and it is found that the method of determining the state of the electrode for discharge surface treatment by the hardness test of the pencil of (3) is the most suitable for the reason of the simplicity of measurement and the like. Thus, the relationship between the hardness of the electrode and the properties of the film formed by the electrode will be described below. Here, as an index used as a reference for the hardness of the electrode, if the particle diameter of the powder constituting the electrode is large and the electrode is soft, the scratch test of the paint pen in the jis K5 600-5.4 is used, for example, When the particle size of the powder constituting the electrode is small and the electrode is hard, Röckweili hardness is used. The above-mentioned JIS K56〇〇_5_4 specification is originally applied to the evaluation of the coated film, but the evaluation of the material having a low hardness is suitable. Of course, the results of other hardness evaluation methods and the scratch test of the coating film are the same: the results can be mutually converted. Of course, other hardness evaluation methods can be used as indicators. As described above, the conditions for forming the thick film ruthenium material are very important, and depending on the case of the experiment, other conditions, particularly hardness, are extremely important as in the case of thick film formation. The relationship between the hardness of the electrode for discharge surface treatment by the surface of the thick film treated by the discharge surface, and the case where the volume ratio of r3 2 3 0% to Cg7G% is made as an example, for example. Fig. 8 is a view showing a state in which a film of a discharge surface treatment electrode having a volume ratio of 3 〇 70% is changed. In Fig. 8, the discharge film used for the transverse coating is measured by the hardness of the pencil: the price is more... = 315550 31 1284682 : Evaluation state of the thickness of the film formed by the electrode. The pulse condition of the discharge used in the discharge surface treatment when performing such a test, the discharge duration (discharge pulse time) (4) 4 A S, rest time t; = 1) r 〇 28# s. Further, in the evaluation test, an electrode of an area of 15 mm X 15 mm was used to form a film. As shown in Fig. 8, in the case where the hardness of the electrode for discharge surface treatment is 4B to φ, the state of the film is very good, and the film is formed and formed. Further, the hardness of the electrode for discharge surface treatment can form a good thick film at the B-formation. Under this range, as the junction is hard, the formation speed of the film tends to be slow, and the formation of a thick film at a hardness of B degree It will be quite difficult. If B is harder than B, it is impossible to form a thick film, so that the hardness of the electrode for discharge surface treatment is hard, that is, the work is performed while removing the work. On the other hand, even if the hardness of the electrode for discharge surface treatment is at a hardness of (10) 2, a good thick film can be formed, but the analysis of the structure reveals a tendency to gradually increase μ in the film. In addition, if the hardness of the electrode for the discharge meter is softer than 9 Β, the phenomenon that the electrode component cannot be melted and melted and directly adheres to the workpiece on the workpiece is a phenomenon that the membrane is broken. Density of the hole (P_US). Here, the relationship between the hard f of the electrode for discharge surface treatment and the state of the film 'is dependent on the discharge pulse condition to be used: it is less likely to change', and when an appropriate discharge pulse condition is used, it can be expanded. The extent of the film is somewhat good. The present inventors', the above-described tendency, constitute a material of an electrode, and are provided by an electrode made of a powder having an average size of 5:' β m. 315550 32 !284682 When the powder having a particle diameter of 5 to 10 Å/m is used in the present embodiment i, c 〇, Ni, Fe, Cu, Zn, etc. are not added to the material constituting the electrode for discharge surface treatment. The carbide-forming material or the carbide which is difficult to form carbides is 40% by volume or more, and the hardness of the coating film may be between B and 8B, and preferably between 4B and 7B. By manufacturing the electrode for discharge surface treatment in a manner of hardness, and using the electrode for discharge surface treatment to perform discharge surface treatment, it is possible to form a thick film on the workpiece stably. If such an electrode for discharge surface treatment is used, it can replace the welding or flame spraying method, and the work previously performed by welding or flame T coating is also processed. In the discharge surface treatment, whether the electrode material can be released from the electrode due to discharge =' end is the bonding strength of the powder constituting the electrode. That is, if the bonding strength is difficult, it is difficult to be released by the energy of the discharge, but if the bonding strength is weak, the 'binding strength is due to the large powder of the electrode constituting the electrode i: different f columns such as 'constituting the electrode When the particle size of the powder is large, since the number of points at which the ends are bonded to each other is reduced, the particle diameter of the electrode which is formed into the electrode is small, and the electrode strength is increased due to the number of points in the electrode: Will be enhanced. Because the second can release the electrode material from the electrode, because the powder is smashed to the thickness of the powder, the film is used in the hardness of the Β to 8 依 according to the hardness of the erroneous pen to the mark test. When the diameter is 1 JL 5"...: The electrode hardness and the film thickness in the case of the present embodiment are 315550 33 1284682. Here, an alloy powder containing Co, Cr, Ni, etc. in a predetermined ratio is exemplified, for example It is pulverized and mixed by an atomize method or a grindstone (^(1) or the like (in a manner that the particle size can be about 3 // m), and the discharge surface treatment is performed according to the flowchart of Fig. 2 of the first embodiment. In the case of the electrode, however, in the mixing step with the wax in step S4, 2 to 3 wt% of the wax is mixed, and in the pressurizing step of step S6, the electrode is prepared at a pressure of about i〇〇Mpai. Powder compression molding, in the heating step of step S7, the heating temperature is varied within a range of 60 (TC to 8 〇〇t. In addition, in the manufacture of the electrode, the heating step of step S7 may be omitted, and The mixed powder was compression-molded and the obtained compact was used as an electrode. The composition of the alloy powder described above is 20% by weight of Cr, 1% by weight of Ni, and 15% by weight of w (tungsten). / 〇, Co is 55 % by weight, and at this time, c vol% is 4% by weight or more. The discharge pulse condition when the manufactured electrode is subjected to the discharge surface treatment is in the 4A and 4B drawings, and the peak current value ie=i〇A, the discharge duration (discharge pulse width) te = 64 # s, the rest time 8. The electrode is formed by using an electrode having an area of 15 mm. As a result, although the electrode material is composed of powder, the material can be formed without any deviation due to the use of the alloy powder. The film, and of course, can be produced by mixing the powder of each material (here, Cr powder, Ni powder, w powder, c powder) in a manner that is a predetermined composition. The electrode, 纟, may have some performance degradation due to problems such as mixing variation of the powder. 315550 34 1284682 In the above description, the weight of Cr is 20% by weight, the weight of i is 。, W 15% by weight, the rest For c The composition of the powdered material is not limited thereto, and may be, for example, an alloy of <25 weight: %, Ni 10 weight%, W7 weight%, and the balance of c〇. Amount or M〇28% by weight, Cr 17% by weight, Si (Shi Xi) 3% by weight, the balance of the remaining, C 比例 ratio, or C ri 5 wt%, F e 8 wt% / the balance of ' Alloy, or Cr 21% by weight, M〇9 by weight m (4)*% by weight, the balance of the alloy of Ni, or CM9 wt%, 妒Μ weight ❶/pM 〇 3 wt%, (Cd(镐)+ Ta) 5 wt. %, Ti 8% by weight, A 10.6% by weight, and the balance of Fe and other alloys, such as C 〇, Ni, Bu, Ba Bu Cu, ~ 40% or more of the elements which are difficult to form carbides by volume% Just fine. n The kernel, because the alloy ratio is not the same, the hardness of the material and the like will be different, so the moldability of the electrode or the state of the film will be different. For example, when the hardness of the electrode material is hard, it may be difficult to form a powder using pressurized powder. When X' is heated to increase the strength of the electrode, it is necessary to try to increase the heating temperature. For example, Cr 25 wt/〇, Ni 10 wt%, w 7 wt%, and the balance c. The proportion of the alloy is softer, and M. 28% by weight, Cr 17% by weight, & 3% by weight, the balance of the alloy is a harder material, but in the heat treatment of the electrode required for the electrode, the temperature of the latter needs to be The temperature is set in an average manner about 100 ° C or higher. Further, the ease of formation of the thick film is as shown in the embodiment, and it is easier to increase the amount. Alloy powder of electrode composition 35 315550 1284682 For the last 3 materials, it is Co, Ni, which is a material that is difficult to form carbides.
Fe、A1、Cu、7 乂 办 ^Fe, A1, Cu, 7 乂
Zn愈多,愈容易形成緻密的厚膜。 一使用種種合金粉末實施試驗之結果發現,與實施形態 ^ 如電極中的難以形成碳化物的材料或不會形成碳 化物的材料夕人士 t ^ 叶之s有率超過4〇體積%,則能容易安定地形成 旱、並且發現,如電極中的Co之含量超過50體積%, 因月b形成足夠厚度之厚膜之故較佳。 又即使難以形成碳化物的材料的Co、Ni、Fe、A1、 、、X外作為合金之成分所混合的材料係會形成碳化物 “科^在其所含材料中成為相對地難以形成碳化物的 =時’被膜中將含有c〇、Ni、Fe、A卜Cu、Zn以外之 、屬成分,而 Co、Ni、Fe、A1、P ύ Λ. Μ A1、Cu、Zn之比例,至少再 月匕形成緻密的厚膜。 由Cl*與C〇之2元素所成合金的情形,發現如電 的Co之含量將超過20體積%起時,開始容易形成厚 比:C:係會形成碳化物的材料,惟如與”等活性的材料 車又時,則係較為難以形成碳化物的材料。亦即,在& 之情形,雖然係屬於容易碳化的 勿反化的材枓,惟如與丁i等材料比 夺’其谷易碳化的程度較低 不及罕乂低而如電極中含有Cr時,則 其一部分將成為碳化物,而一部分 、 成A妯赠, 丨刀將保持金屬之Cr之狀態 m m Λ j <為,在形成緻密的 ;膜時,需要被膜中作為金屬所留 穑斗十如 蜀所邊存的材料之比例為按體 積计,存在30%程度以上。 將調查使用從粒徑丨至5 β 之知末所製造的電極以 315550 36 !284682 形成被膜時之電極硬度與被膜之厚度的關係之結果,表示 如下。在此,如使用粒徑在6 # m程度大小之粉末以製造 電極時,可採用上述的JIS K5600_5_4所規定的塗膜用錯 筆到痕試驗,惟如使用粒徑較此為小的粉末製造電極時, 則不此適用此種試驗。於是,本例中,係採用從將i 吋 之鋼球按15kgf之壓力按壓時之壓痕距離h(//m)所求得硬 度Η=1〇〇_ι〇0〇χ1ι之硬度之指標。 其結果,電極硬度在25至35程度之硬度時之被膜之 狀態最佳,而能形成緻密的厚度。但,即使多少偏離其範 圍,仍然有能形成厚膜的範圍,硬的方向係至5〇程度之硬 度為止尚能形成厚膜,而軟的方向則至2〇程度之硬度為止 尚能形成厚膜。但,隨著硬度增高,則有被膜之形成速度 會緩慢下來的傾向,惟在50程度之硬度,則厚膜之形成會 相當困難。如再增加硬度則不能形成厚膜,而隨著硬度之 增加,會開始工件側之去除加工。又,在軟的方向,至2〇 程度為止的硬度下,雖能形成厚膜,惟有未熔融之材料會 增加之傾向,如電極較20程度為軟時,則可發現電極成= 尚未十分熔融之下直接附著於工件侧的現象。在此,此種 電極硬度與被膜之狀態之關係,會因所使用的放電脈衝條 件而多少變化,如使用適當的放電脈衝條件時,則亦可某 些程度擴大能形成良好的被膜的範圍。 另外,如本實施形態2之粉末粒徑成為3Am程度(ι "m至5/zm程度)’則放電表面處理上適當的電極之硬度 亦會增高,以實施形態1所示的JIS K56〇〇_5_4之塗膜用 315550 37 1284682 紐筆到痕試㈣難m因此,在此,則制洛式硬度 成驗。洛氏硬度試驗,係將球按既定荷重按壓,而從壓痕 之形狀求得硬度者。如荷重過重時,則會引起電極之破損 之故,需要作成適當的強度。硬度試驗,其他尚有維氏硬 度試驗(Vieker,shardnesstest)等’當然可用為電極硬度之 敎,惟在此情形财壓痕之端部會帛潰轉於觀察的問 題’故壓頭形狀仍然以球狀者較佳。 如採用本實施形態2,而從含有不會形成碳化物的材 #或難以形成碳化物的材料4()體積%以上並作成構成電 :的叙末之平均粒瓜為i至5" m的粉末,按將硬度能成 為20至5G之方式製造放電表面處理用電極,並使用此電 極以實施放電表面處理’即可於工件表面形成緻密且厚的 被膜。 實施形熊3 將與實施形態2同樣材料之粉末作成平均一以製 造電極。雖然係同-種材料,由於將粉末粒徑改小,即可 更增加為放電表面處理上所適當的電極硬度。在此情形 下:如亦含有不會形成碳化物的材料或難於形成碳化物的 材料40體積%以上,則能容易形成厚膜。 在此情形下,電極硬度在3〇至5〇程度之硬度時被膜 =狀恶最佳,而能形成緻密的厚膜。❻,即使多少偏離其 靶圍’仍然有能形成厚膜的範圍,硬的方向係至的程度之 硬度為止尚能形成厚腔;, 珉与膜而軟的方向則至25程度之硬度為 止尚能形成厚膜。自,隨著硬度增高,則有被膜之形成速 315550 38 1284682 度會緩慢下來的傾向,惟在6G程度之硬度,則厚膜之形成 會相當困難。如再增加硬度則不能形成厚膜,而隨著硬度 之增加,會成為去除工件側的去除加工。又,在軟的方向, 係在25程度為止的硬度下,雖能形成厚膜,惟有未熔融之 材料會增加之傾向,如電極較25程度為軟時,則可發現電 極成分尚未十分熔融之下直接附著於工件側的現象。在 此,此種電極硬度與被膜狀態之關係,會因所使用的放電 脈衝條件而多少變化,如使用適當的放電脈衝條件時,則 亦可某些程度擴大能形成良好的被膜的範圍。又,關於從 平均粒徑在1 // m以下之粉末所製造的電極,獲得同樣之 結果。 如採用本實施形態3,而從含有不會形成碳化物的材 料或難以形成碳化物的材料40體積%以上,並作成構成電 極的粉末之平均粒徑為丨# m以下之粉末,按將硬度能成 為25至60之方式製造放電表面處理用電極,並使用此電 極以實施放電表面處理’即可於工件表面形成緻密且厚的 被膜。 實施形Μ 4 本實施形態4中,就藉由放電表面處理方法而能將工 件上所形成的被膜增厚的放電表面處理用電極加以說明。 首先’就因構成放電表面處理用電極的粒徑大小所引 起的硬度之變化加以說明。在第2圖之流程圖之步驟S6 之加壓步驟中,將粉末加壓成型時,壓力將從與加壓面或 金屬模具面相接的粉末往電極内部傳遞,其時,粉末會微 39 315550 1284682 :移::、此時,如粉末之平均粒徑為數十"m程度的大小 或全二末與粉末之間所形成的空間將增大,而與加壓面 或金屬核具面相接的(電極 表面之)粉末,即按能填充其空 "移動’存在於電極表面的粒子密度將增高,而丈 刀之摩擦將增大。亦即, ’、 彳重此罪電極表面即可保持對加 、反作用力,以致壓力不會傳遞至電極内部。此乃 電極中形成有硬度之分佈的原因。 〃如使用此種具有硬度分佈的放電表面處理用電極以實 施處理時,則會成為下述^種中之任—種狀態。第1種, 係電極之外周部為最適當的硬度,而内部為過軟的情形。 在此種情形下,在電極之外周部即可在工件上堆積被膜, 惟在其内部則不能在工件上形成被膜或形成鬆懈不堪的被 膜。第2種,係電極之外周部為過硬,而㈣為軟的情形。 在此情形下,在外周部由於放電表面處理中不會消耗電極 之故,會成為去除加工’惟在其内部則在工件上形成鬆懈 不堪的被膜。X,在電極外周部過硬以致成為工件表面之 去除加工的情形下,則由於電極内部雖㈣耗,但外周部 不會消耗之故,電極放電側之面,將成為外周部突出的形 狀,而在外周部將發生多數之放電。如發生此種情況,則 容易引起放電集中而放電會成為不安定。此等情況均在放 電表面處理上甚為不宜。 於是,就使用粒徑小的粉末所製造的放電表面處理用 電極之硬度與被膜之形成,進行試驗。在此,僅使用平均 粒徑1.2#m之合金粉末,依照第2圖所示步驟製造 315550 40 1284682 χ 1 lmmx 5.5mm之形狀之放電表面處理用電極。此時所使 用的的合金粉末,係Cr 25wt%、Ni l〇wt%、W 7wt%、C 〇.5wt%、其餘為c〇之比例之合金。又,此種組成之合金 粉末之外’亦可使用Mo 28wt%、Cr 17wt%、Si 3wt%、其 餘為Co之比例之合金、或者Cr 28wt%、Ni 5wt%、W 1 9wt%、其餘為c〇之比例之合金等。在此,在第2圖之步 驟S6之加壓步驟中,以67MPa之壓力將粉末壓縮成型, 又’為製得具有不同的硬度的電極起見,在步驟S7之加 熱步驟中,以73(TC及75(TC之各溫度,使用真空爐將壓粉 體加熱一小時。 首先,就改變加熱溫度所製造的各種電極之硬度加以 研究。在此,在本實施形態4中,採用電極之壓縮強度作 為電極之硬度。第9圖,係表示測定電極之壓縮強度的實 驗裝置之概要的照片。在第9圖之實驗裝置,係按每秒m 之比例增加對電極施加負荷的力量,並藉由電極上部之測 力傳感器(load cell)以測定對電極(Electr〇de)所施加負荷 之力里。如到達某種力量時,則由於電極表面會發生龜裂 而所負何的力量會釋放之故,從即將發生龜裂時之力量, 算出電極之壓縮強度。其結果…3代下所加熱的電極 之壓縮強度為麵Pa,在75吖下所加熱的電極之麼縮強 度為 180MPa。 其次,就從合金粉末所製造的電極之壓縮強度與被膜 厚度的關係’加以說明。此時之放電表面處理條件,係將 峰值電流值作成1〇A’將放電持續時間(放電脈衝寬度)作 315550 41 1284682 成 4 # S 0 第11圖,係表示依上述條件實施放電表面處理時之電 極之Μ縮強度與被膜厚度的關係的圖。在第u圖中,橫轴 表示放電表面處理用電極之壓縮強度(Mpa),縱袖表示使 用具有橫轴所示的壓縮強度的放電表面處理用電極 放電表面處理時,在工侔矣而私上 貫細1 在件表面所形成的被膜厚度(mm)。 又,較縱轴之被膜厚度〇随為小的值,係表示 膜而切削工件表面的去除加 v成破 云陈加工。如亦在該圖中所示,如放 電表面處理用電極之壓縮強度在1嶋Pa_,可在工件表 面上實施堆積加工’惟如壓縮強度在18幅Pa_,則會成 為工件表面之絲加工。特別是,在工件上形成厚度02_ 以上之厚被膜時,電極之壓縮強度需要在議Pa以下。 另外,如電流之峰值或放雷 戎裒冤時間增大時,由於僅增大從電 極所供給的電極粉末量,而從電極剝取電極粉末的力量不 八加之故,在其他加工條件下仍然與第i i圖同樣的社 果。 。 將粉末壓縮成型所製造的放電表面處理用電極之壓縮 強度,可由每單位體積中所含的粒子與粒子之結合數目所 決定。如平均粒徑增大時,由於單位體積中所含的粒子與 粒子之、.”數目會減少之故,壓縮強度會下降。亦即,表 示祇要是平均粒徑相同’如將壓縮強度作成能形成厚被膜 的某值以下’則無論任何材質均可形成厚被膜之意。例如, 關於此種電極硬度加以考察時,發現使用平均粒徑約1 # m 之口金私末之壓粉體電極的放電表面處理中,作為適當的 315550 42 1284682 被膜形成的電極評價之一指針,需要管理壓縮強度為 lOOMPa以下之方式,惟此種能形成厚被膜的電極評價之 一指針的壓縮強度,祇要是平均粒徑相同,則即使材質改 變仍然不會改變。但,改變材質時,則需要改變電極製造 上的加熱溫度或加壓壓力等成型條件。 如上所說明,經確認能決定可否藉由放電表面處理而 形成厚的被膜的主要因素之一,在於電極之硬度。亦即, 如使用平均粒徑在約丨# m之粉末時,改變壓縮成型時之 壓力或加熱溫度’並使用壓縮強度能成為1 〇〇Mpa以下之 方式所製造的放電表面處理用電極實施放電表面處理,則 可在工件上形成厚被膜。因放電所發生的力量,會按拉開 電極粉末之方式作用,而此種力量所及範圍,係0數+ " m 至0數mm。亦即,需要能以此種層級之大小而測知電極 之強度’為此,能掌握電極之整體的硬度之壓縮強度最為 合適。 ” 再者如電極之粉末之粒徑較小時,則即使以同樣加 壓壓力,同樣加熱溫度下製造電極,由於每單位體積之粒 子數增加,雖然一個粒子與其周圍之粒子結合的面之數目 不會改變’惟單位體積中所含總結合面數會增加之故,電 極會變硬。 近年來’由於粉末之成型技術之進步,已能製造具有 至1 〇〇nm之平均粒徑的金屬粒末或陶瓷粉末。於是, 就使用平均粒徑5〇nm之別粉末以製造放電表面處理用電 極時之壓縮強度與被臈厚度的關係,加以實驗。另外,如 43 315550 1284682 使用平均粒徑在奈米層級之粉末以製造電極時,由於僅靠 加壓即可製得具有充夠強度的電極之故,可省略第2圖之 步驟S7之加熱步驟,在本例中省略加熱步驟。又,使用 所製造的電極下的放電表面處理的放電之脈衝條件,係依 知與上述第1 〇圖所示者同樣條件下實施者。實驗之結果, 、、二確5忍如壓縮強度較i 6〇MPa為低時,雖然在工件表面實 施堆積加工,惟較此壓縮強度以上時,則會變成工件表面 之去除加工之情況。 在此’如關於平均粒徑50nm之Ni粉末之電極強度加 以考察時,發現在使用Ni粉末之壓粉體電極的放電表面處 理上,作為適當的被膜形成用的電極評價之一指針,需要 苔理壓縮強度為能成為1 60MPa以下之方式。 如上所述’將粉末壓縮成型所製造的電極之壓縮強 度,係由每單位體積中所含粒子與粒子之結合之數目所決 定。如平均粒徑變小時,由於單位體積中所含粒子與粒子 之結合之數目會增加之故,壓縮強度會增高。又,如上述, 發現在使用平均粒徑5〇nm之犯粉末之壓粉體電極的放電 表面處理上,作為適當的被膜形成用的電極評價之一指 針,需要管理壓縮強度為16〇MPa以下之方式。此種發現, 如與平均粒徑為1·2// m之情形之結果合併考察時,係表 示隨著平均粒徑之不同,而能形成厚被膜的電極之壓縮強 度亦不同之意。又,作為適當的被膜形成用之電極評價之 -指針的壓縮強度之值,祇要是平均粒徑相同,係不會因 電極材料之材質而有所不同。因&,如判斷由平均粒徑小 315550 44 1284682 的粉末所成放電表面處理用電極,能否堆積厚被膜時,則 可將其壓縮強度增大。 再者’作為其他電極材料,而使用平均粒徑3 # m之 Co粉末’貫施同樣實驗之結果,經確認能堆積被膜的界限 之電極之壓縮強度,為50MPa程度。在此情形下,亦經確 涊旎決定可否藉由放電表面處理而形成厚的被膜的主要因 素之一,在於電極之硬度。亦即,經確認如使用平均粒徑 3 // m之粉末,改變壓縮成型時之壓力或加熱溫度以製造壓 縮強度成為50MPa以下的電極,並使用其電極以實施放電 表面處理時,則能在工件表面形成厚的被膜。 在此情形下,由於將粉末壓縮成型所製造的電極之壓 縮強度,係由每單位體積中所含粒子與粒子之結合之數目 所決定之故,作為適當的被膜形成用之電極評價之一指針 的壓縮強度之值,祇要是平均粒徑相同,係不會因電極材 料之材質而有所不同。因此,如判斷由平均粒徑大的粉末 所成放電表面處理用電極,能否堆積厚被膜時,則有需要 將其壓縮強度作成偏低些。 第11圖,係表示平均粒徑與能堆積厚被膜的電極之壓 縮強度的關係圖。在第11圖中,橫軸係以對數刻度表示構 成放電表面處理用電極的粉末之平均粒徑Um),而縱軸表 示能在工件表面形成被膜的電極之壓縮強度之堆積界限壓 縮強度(MPa)。如此圖所示,平均粒徑愈小,愈增加堆積 界限壓縮強度。 如採用本實施形態4,而將平均粒徑為丨“爪之粉末作 315550 45 1284682 為原料,使用壓縮強度能成為100MPa以下之方式所製造 的放電表面處理用電極以實施放電表面處理,即能在工件 上形成在高溫環境下具有潤滑性的緻密的厚膜。又,平均 粒徑為50nm之粉末時,按壓縮強度能成為ΐ6〇Μρ&以下 之方式而,平均粒徑為3#m之粉末時,按壓縮強度能 成為50MPa以下之方式製造放電表面處理用電極,並使用 其放電表面處理用電極以實施放電表面處理,即能在工件 上形成高溫環境下具有潤滑性的緻密的厚膜。 再者,如採用本實施形態4,而將所製造的放電表面 ^理用電極用於放電表面處理時,可使用其壓縮強度以評 仏此否在工件上堆積厚被膜。藉此,亦能適用於放電表面 處理用電極在同樣條件下一次大量製造時之電極之評價 上。具體而t,係將從同一料下一次大量製造的電極之 中所抽出的一個或複數個電極之壓縮強度之測定結果,作 為同時所製造的電極之評價者。由此,在電極之大量生產 時,亦能管理所有電之品質。 實施形態5 本實施形態5中,就將金屬粉末作為壓粉體電極使用 的放電表面處理上,不致降低表面粗糙度下能進行安定的 放電,並能堆積厚被膜的放電表面處理用電極,加以說明。 如實施形態1至3所說明者,如藉由放電表面處理而 在工件表面上形成厚模時,需要將不會形成碳化物的材料 或難以形成碳化物的碳化物的材料添加於電極材質之成分 上等的材料上的條件。自’僅添加不會形成碳化物的材料 315550 46 1284682 或難以形成碳化物的材料於電極中年 T牙有工件上表面所形 ,中厚膜中將殘留n以致難以形成緻密的被膜的問 題。於是,在本實施形態5中,即就盘At γ >广 、 T 丨就為旎形成厚膜且緻密 的被膜上所需要的技術,加以說明。 在此,舉含有 Cr 3〇%、Ni 3%、M〇 2%、w 5%、以 3% 專以Co為基材之合金(以下,簡稱c〇合金)為例,加以說 明。此種Co合金粉末,係使用市售品。另外,c〇合金而 言’含有^^紹㈣^^等以“為基材之合金、 =含有〇難%、们%等以〇〇為基材的合金、或 3有。20%,10%,15%等的以。。為基材之合金等; 祇要是含有以Co為基材者即可。 從平均粒徑3" m程度之c。合金粉末,依照上述第2 圖之步驟以製造放電表面處理用電極。此時之步驟S" 的加壓步射之加壓壓力最好在93至·奶程度。如較 =力為高時’則電極之硬度上會產生偏差,或在加壓時 電極上會發生氣裂(air crack)。 如使用依上述方式所製造之co合金粉末所成放電表 面處八理用電極以實施放電表面處理時,將在工件表面形成 ^金之被膜。但,從發明人等的實驗,發現被膜之性能 =電極中所伯電極材料之粉末之比例之影響很大。由於 =係將f末材料加以”成型所製作之故’成為存有空 曰夕的狀恶。如此種空間過多時, + 于則電極強度會降低以致 ::猎由放電之脈衝而正常進行電極材料之供給。例如, 曰表生因放電之衝擊而電極即在廣泛範圍崩壞等現象。另 315550 47 1284682 一方面,如空間過少時,電極太過堅固地密接,而發生藉 由放電脈衝的電極材料之供給減少的現象,以致不能形成 厚膜。 在此所使用的粒徑3 // m程度之粉末,係將粒徑數十 // m之粒徑之粉末粉碎所製造,而粒徑之粒度分佈為具有 以3// m為峰值的分佈的粉末。如將此種相當程度均勻的 粒徑之粉末壓縮成型以製造電極時,根據本發明人等之實 驗,電極材料在能形成良好被膜的電極之電極體積中所佔 的體積比例(其餘為空間),係在25%至5〇%之範圍。但, 如。電極材料之體積之比例(以下,簡稱電極材料之比例)在 25〇/〇時,料電極而言,為相#柔軟且有強度不足夠的感 覺。相反地,如電極材料之比例在5〇%時,作為電極而言, 為相當堅硬且部分有產生氣裂的情形。將此種情形之;電 極材料體積之比例所引起的被膜之狀態之概略情況,列示 於表1中。但,此種比例,t因粉末粒徑之分佈等而多少 會變化,例如,使用粒徑分佈較廣的粉末時,則有電極之 空間率(=(100-電極材料體積之比例)%)會降低的傾向。相 反地,如使用粒徑分佈較狹窄的粉末時,則有電極之空 率會增大的傾向。 I曰 315550 48 1284682 表1 電極材料體積之比例 被膜之狀態 15% 電極崩潰而不能使用 20% 雖能形成被膜,惟鬆懈不堪之狀態 25% 雖屬多孔性,惟尚能形成厚膜 30% 能形成緻密的厚膜 40% 能形成緻密的厚膜 50% 雖能形成緻密的厚膜,惟膜之形成緩慢。 55% 進行工件之去除加工,以致不能形成厚膜。 另一方面,如將粒徑不同的粉末混合時,例如,於上 述例中所使用的粒徑3 // m程度中混合粒徑6 /z m程度之粉 末時,電極材料體積在能形成良好被膜的電極之電極體積 所佔之比例係在40至65%之範圍。但,電極材料體積之 比例在40%時,作為電極而言,為相當柔軟且有強度不足 夠的感覺。相反地,如電極材料體積之比例在6 5 %時,作 為電極而言,為相當堅硬者。將此種情形之因電極材料體 積之比例所引起的被膜之狀態之概略情況,例示於表2 中 〇 表2 電極材料體積之比例 被膜之狀態 30% 電極崩潰而不能使用 35% 雖能形成被膜,惟鬆懈不堪之狀態 40% 雖屬多孔性,惟尚能形成厚膜 50% 能形成緻密的厚膜 60% 能形成緻密的厚膜 65% 雖能形成緻密的厚膜,惟膜之形成緩慢。 70% 進行工件之去除加工,以致不能形成厚膜。 如採用本實施形態5,由於作成使用經考慮電極材料 在電極體積所佔之體積比例之放電表面處理用電極以實施 49 315550 1284682 放電表面處理之方式之故,即使以金屬粉末作為原料所製 造的放電表面處理用電極,亦能在工件上形成無空穴的緻 密的被膜。 另外’在上述專利文獻2中,在能以極高的壓力形成 的陶瓷電極方面,有使用經壓縮成型為理論密度之5〇%至 90%之方式的電極的記錄,惟並非係如本實施形態5之形 成緻密的金屬之厚膜者,故其技術範圍、用途、效果亦不 相同。 實施形態6 本實施形態6中,在採用將金屬粉末壓缩成型所製造 的放電表面處理用電極方面,就能堆積厚的被膜的放電表 面處理,加以說明。 在由第2圖所示過程所製造的放電表面處理用電極方 面,如粉末與粉末之結合強時,粉末間之熱之傳遞順利進 行,亦即熱傳導率增大,相反地,如其結合弱時,則粉末 間之熱之傳遞不會順利進行,以熱傳導率降低。如提高加 熱溫度,則粉末與粉末之金屬結合進展,而電極之熱傳率 增大。相反地,如降低加熱溫度,則粉末與粉末之金屬結 合不甚進展,而電極之熱傳導率降低。 如電極之熱傳導率(對每單位長度、單位溫度之 較低時,由於局部性地成為高溫之故,可藉用放電之執量 而使電極材料一瞬間即氣化。藉由此爆發力而剝取電極之 熔融部或固體部,從電極所脫離者即堆積在工件表面 一方面’如電極之熱傳率較高時,由於熱容易擴散之故難 315550 50 1284682 以產生熱斑點(heat spot),以致電極材料殆不會氣化。因 此,不會發生爆發力,以致不能供給電極材料。由此可知, 欲在工件表面形成厚被膜時,需要在工件上堆積較構成工 件的材料之去除量為多的量之電極材料,因此,放電表面 處理用電極之熱傳導率需要較低者。 以下,就降低放電表面處理用電極之熱傳導率之作法 加以說明。依照第2圖之過程,僅使用平均粒徑1 · 2 #瓜 之合金粉末,以製造50mmx 11 mmx 5.5mm之形狀之放電 表面理用電極。此時所用的合金粉末,係Cr 25wt%、Ni 10wt%、W 7wt%、C 0.5wt%,其餘為Co之比例的合金。 除此種組成之合金粉末之外,尚可使用M〇 28¾、Cr 17wt%、Si 3wt%,其餘為Co之比例之合金,或Cr 28% wt%、Ni 5wt%、W 19wt%其餘為Co之比例之合金。再者, 在第2圖之步驟S6之加壓步驟中,以67]V[pa之壓力將粉 末壓縮成型,又,為製得具有不同硬度的電極起見,在步 驟S7之加熱步驟中,在73〇它及750^之各溫度下,在真 空爐内加熱壓粉體1小時。又,放電表面處理,係以與實 施形態4同樣之放電脈衝條件實施者。 首先’就改變加熱溫度所製造之各電極之熱傳導率依 雷射閃爍(Laser flash)法加以調查。其結果,在73〇°C下所 加熱的電極之熱傳導率為l〇W/mK,而在750°C下所加熱 的電極之熱傳導率為Kw/mK。 第12圖’係表示使用熱傳導率不相同的放電表面處理 用電極實施放電表面處理5分鐘時,於工件表面所形成的 51 315550 1284682The more Zn, the easier it is to form a dense thick film. As a result of performing tests using various alloy powders, it has been found that, in the case of a material such as an electrode which is difficult to form a carbide in an electrode or a material which does not form a carbide, the probability of a t ^ leaf is more than 4 vol%, It is easy to form a drought, and it has been found that if the content of Co in the electrode exceeds 50% by volume, it is preferable since the month b forms a thick film having a sufficient thickness. Further, even if Co, Ni, Fe, A1, and X, which are difficult to form a carbide material, are mixed as a component of the alloy, a carbide is formed, and it is relatively difficult to form a carbide in the material contained therein. The = when the film will contain c〇, Ni, Fe, A, Cu, Zn, other components, and Co, Ni, Fe, A1, P ύ Μ. Μ A1, Cu, Zn ratio, at least A dense thick film is formed in the lunar calendar. When the alloy of Cl* and C is alloyed, it is found that if the content of Co exceeds 20% by volume, the thickness ratio begins to form: C: carbonization is formed. The material of the material is only a material that is more difficult to form carbides when it is used with a material such as an active material. That is to say, in the case of &, although it is a material that is easy to carbonize, it is a material that is not decarburized, but if it is compared with a material such as Ding, the degree of carbonization is not as low as that of the grain, and the electrode contains Cr. At the time, a part of it will become a carbide, and a part will be given as a gift. The file will maintain the state of the metal Cr. mm lt j < In order to form a dense film, it is necessary to leave the film as a metal. The ratio of the materials stored in the bucket is as high as 30% or more. The results of the relationship between the electrode hardness and the thickness of the film when the film was formed using 315550 36 !284682 from the electrode made of the particle size 丨 to 5 β were examined as follows. Here, when a powder having a particle size of about 6 #m is used to produce an electrode, the erroneous pen-to-mark test of the coating film specified in the above-mentioned JIS K5600_5_4 can be used, but a powder having a smaller particle diameter is used. For electrodes, this test is not applicable. Therefore, in this example, the hardness of the hardness Η=1〇〇_ι〇0〇χ1ι is obtained from the indentation distance h (//m) when the steel ball of i 吋 is pressed at a pressure of 15 kgf. . As a result, the state of the film at the hardness of the electrode hardness of 25 to 35 is optimum, and a dense thickness can be formed. However, even if it deviates somewhat from its range, there is still a range in which a thick film can be formed. A hard film can form a thick film until the hardness is 5 〇, and a soft direction can be formed to a thickness of 2 硬度. membrane. However, as the hardness increases, the rate at which the film is formed tends to slow down, but at a hardness of 50 degrees, the formation of a thick film is quite difficult. If the hardness is increased again, a thick film cannot be formed, and as the hardness increases, the removal of the workpiece side is started. Further, in the soft direction, to a hardness of about 2 ,, a thick film can be formed, but the unmelted material tends to increase. If the electrode is softer than 20, the electrode can be found to be not yet melted. The phenomenon of directly attaching to the side of the workpiece. Here, the relationship between the hardness of the electrode and the state of the film varies somewhat depending on the discharge pulse conditions to be used. When an appropriate discharge pulse condition is used, the range in which a good film can be formed can be expanded to some extent. In addition, as the powder particle size of the second embodiment is about 3 Am (i<m to 5/zm), the hardness of an appropriate electrode on the discharge surface treatment is also increased, and the JIS K56 shown in the first embodiment is used. 〇_5_4 coating film with 315550 37 1284682 New pen to the trace test (four) difficult m Therefore, here, the Luo type hardness test. The Rockwell hardness test is a method in which the ball is pressed against a predetermined load and the hardness is obtained from the shape of the indentation. If the load is too heavy, it will cause damage to the electrode and it is necessary to make an appropriate strength. Hardness test, other Vickers hardness test (Vieker, shardnesstest), etc. 'Of course can be used as the electrode hardness, but in this case, the end of the financial indentation will collapse to the problem of observation', so the shape of the indenter is still A spherical shape is preferred. According to the second embodiment, the average melon which is composed of a material which does not form a carbide or a material which is difficult to form a carbide 4 (% by volume) and which constitutes electricity is i to 5 " m In the powder, an electrode for discharge surface treatment is produced in such a manner that the hardness can be 20 to 5 G, and the electrode can be subjected to discharge surface treatment to form a dense and thick film on the surface of the workpiece. The bear 3 was formed by averaging the powder of the same material as in the second embodiment to produce an electrode. Although the same material is used, since the particle size of the powder is made smaller, the electrode hardness suitable for the discharge surface treatment can be further increased. In this case, if a material which does not form a carbide or a material which is difficult to form a carbide is contained in an amount of 40% by volume or more, a thick film can be easily formed. In this case, when the hardness of the electrode is from 3 Torr to 5 Torr, the film is in the best shape, and a dense thick film can be formed. ❻, even if it deviates from its target circumference, there is still a range in which a thick film can be formed, and the hardness of the hard direction can still form a thick cavity; the soft direction of the enamel and the film is as high as 25 degrees. Can form a thick film. Since the hardness increases, there is a tendency that the formation speed of the film 315550 38 1284682 will slow down, but the hardness of 6G will make the formation of a thick film quite difficult. If the hardness is increased again, a thick film cannot be formed, and as the hardness increases, the removal process on the side of the workpiece is removed. Further, in the soft direction, a thick film can be formed at a hardness of 25 degrees, but the unmelted material tends to increase. If the electrode is softer than 25, the electrode component is not yet melted. The phenomenon of directly attaching to the side of the workpiece. Here, the relationship between the hardness of the electrode and the state of the film varies depending on the discharge pulse condition to be used. If an appropriate discharge pulse condition is used, the range in which a good film can be formed can be expanded to some extent. Further, the same results were obtained for an electrode produced from a powder having an average particle diameter of 1 // m or less. According to the third embodiment, the powder having a carbide-free material or a material which is difficult to form a carbide is contained in an amount of 40% by volume or more, and the powder having the average particle diameter of the electrode is 丨# m or less. The electrode for discharge surface treatment can be manufactured in a manner of 25 to 60, and the electrode can be subjected to discharge surface treatment to form a dense and thick film on the surface of the workpiece. (Fourth Embodiment) In the fourth embodiment, an electrode for discharge surface treatment in which a film formed on a workpiece can be thickened by a discharge surface treatment method will be described. First, the change in hardness caused by the particle size of the electrode for discharge surface treatment will be described. In the pressurizing step of step S6 of the flowchart of Fig. 2, when the powder is press-formed, the pressure is transferred from the powder which is in contact with the pressing surface or the surface of the metal mold to the inside of the electrode, and the powder is slightly 39. 315550 1284682 : Shift:: At this time, if the average particle size of the powder is tens of degrees, the size of the powder or the space formed between the powder and the powder will increase, and with the pressing surface or metal core The surface of the powder (of the surface of the electrode), that is, the density of the particles present on the surface of the electrode will increase as the space can be filled, and the friction of the blade will increase. That is, ', 彳 此 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极 电极This is the reason why the distribution of hardness is formed in the electrode. For example, when such an electrode for discharge surface treatment having a hardness distribution is used for the treatment, it may be in any of the following categories. In the first type, the outer peripheral portion of the electrode is the most suitable hardness, and the inside is too soft. In this case, the film can be deposited on the workpiece at the outer periphery of the electrode, but the inside of the electrode cannot form a film on the workpiece or form a loose film. In the second type, the outer peripheral portion of the electrode is too hard, and (iv) is soft. In this case, in the outer peripheral portion, since the electrode is not consumed in the discharge surface treatment, the removal process is performed, but the inside of the workpiece is formed into a slack film on the workpiece. X, when the outer peripheral portion of the electrode is too hard to be removed from the surface of the workpiece, the inside of the electrode is consumed (4), but the outer peripheral portion is not consumed, and the surface on the discharge side of the electrode becomes a shape in which the outer peripheral portion protrudes. Most of the discharge will occur in the outer peripheral portion. If this happens, it is easy to cause the discharge to concentrate and the discharge will become unstable. These conditions are not suitable for discharge surface treatment. Then, the hardness of the electrode for discharge surface treatment produced by using the powder having a small particle size and the formation of the film were tested. Here, only the alloy powder having an average particle diameter of 1.2 #m was used, and an electrode for discharge surface treatment having a shape of 315550 40 1284682 χ 1 lmm x 5.5 mm was produced in accordance with the procedure shown in Fig. 2 . The alloy powder used at this time is an alloy of Cr 25 wt%, Ni l〇 wt%, W 7 wt%, C 〇 5 wt%, and the balance of c〇. Further, in addition to the alloy powder of such composition, it is also possible to use an alloy of Mo 28 wt%, Cr 17 wt%, Si 3 wt%, and the balance of Co, or Cr 28 wt%, Ni 5 wt%, W 19 wt%, and the rest. An alloy such as c比例. Here, in the pressurizing step of step S6 of FIG. 2, the powder is compression-molded at a pressure of 67 MPa, and 'for the purpose of producing electrodes having different hardnesses, in the heating step of step S7, 73 ( TC and 75 (the temperature of TC, the powder compact was heated for one hour using a vacuum furnace. First, the hardness of various electrodes produced by changing the heating temperature was investigated. Here, in the fourth embodiment, the compression of the electrodes was employed. The intensity is taken as the hardness of the electrode. Fig. 9 is a photograph showing an outline of an experimental apparatus for measuring the compressive strength of the electrode. In the experimental apparatus of Fig. 9, the force applied to the electrode is increased by a ratio of m per second, and The load cell on the upper part of the electrode is used to measure the force applied to the counter electrode. If a certain force is reached, the force will be released due to cracking on the electrode surface. Therefore, the compressive strength of the electrode is calculated from the force at the time of cracking. The result is that the compressive strength of the electrode heated in the third generation is the surface Pa, and the strength of the electrode heated at 75 为 is 180 MPa. Next, the relationship between the compressive strength of the electrode made of the alloy powder and the thickness of the film will be described. The discharge surface treatment condition at this time is to make the peak current value 1 〇 A' and the discharge duration (discharge pulse width). 315550 41 1284682 into 4 # S 0 Fig. 11 is a view showing the relationship between the collapsing strength of the electrode and the thickness of the film when the discharge surface treatment is performed under the above conditions. In Fig. 5, the horizontal axis indicates the surface treatment for discharge. The compressive strength (Mpa) of the electrode, and the longitudinal sleeve indicates the thickness of the film formed on the surface of the member by the surface of the discharge surface treated by the discharge surface treatment using the compressive strength indicated by the horizontal axis ( Mm). Further, the thickness 〇 of the film on the vertical axis is a small value, which means that the film is removed and the surface of the workpiece is removed to form a cloud. As shown in the figure, an electrode for discharge surface treatment is also shown. The compressive strength is 1嶋Pa_, and the stacking process can be performed on the surface of the workpiece. However, if the compressive strength is 18 Pa_, it will become the wire processing of the workpiece surface. In particular, the thickness is formed on the workpiece. When the thickness of the film is 2_ or more, the compressive strength of the electrode needs to be below the Pa. In addition, if the peak value of the current or the time of the thunder is increased, the amount of the electrode powder supplied from the electrode is increased, and the electrode is increased from the electrode. The strength of stripping the electrode powder is not the same as that of Figure ii under other processing conditions. The compressive strength of the electrode for discharge surface treatment produced by compression molding of powder can be contained in each unit volume. The number of particles combined with the particle is determined. If the average particle size is increased, the compressive strength will decrease as the number of particles and particles contained in the unit volume will decrease. That is, as long as it is average The same particle size 'if the compressive strength is formed to a value below the thickness of the thick film', the thickness of the film can be formed regardless of any material. For example, when examining the hardness of such an electrode, it has been found that in the discharge surface treatment of a powdered powder electrode having an average particle diameter of about 1 # m, as an electrode of the appropriate 315550 42 1284682 film formation, It is necessary to manage a method in which the compressive strength is 100 MPa or less, but the compressive strength of one of the electrodes for forming a thick film is not changed as long as the average particle diameter is the same. However, when changing the material, it is necessary to change the molding conditions such as the heating temperature or the pressing pressure on the electrode manufacturing. As described above, it is confirmed that one of the main factors that can determine whether or not a thick film can be formed by the discharge surface treatment is the hardness of the electrode. In other words, when a powder having an average particle diameter of about m# m is used, the pressure at the time of compression molding or the heating temperature is changed, and discharge is performed using an electrode for discharge surface treatment in which the compressive strength can be 1 〇〇Mpa or less. Surface treatment can form a thick film on the workpiece. The force generated by the discharge will act in the manner of pulling off the electrode powder, and the range of this force is 0 + " m to 0 mm. That is, it is necessary to be able to measure the strength of the electrode by the size of such a layer. For this reason, it is most suitable to grasp the compressive strength of the hardness of the entire electrode. Furthermore, if the particle size of the powder of the electrode is small, even if the electrode is produced at the same heating temperature under the same pressing pressure, the number of faces of one particle combined with the surrounding particles is increased due to the increase in the number of particles per unit volume. Will not change 'only the total number of joints contained in the unit volume will increase, the electrode will become hard. In recent years, due to advances in powder molding technology, it has been possible to manufacture metals with an average particle size of up to 1 〇〇nm. A powder or a ceramic powder is used. Thus, the relationship between the compressive strength of the electrode for discharge surface treatment and the thickness of the bedding is measured using a powder having an average particle diameter of 5 〇 nm. Further, an average particle diameter of 43 315 550 1284682 is used. When the powder of the nano layer is used to produce an electrode, since the electrode having sufficient strength can be obtained only by pressurization, the heating step of step S7 of Fig. 2 can be omitted, and the heating step is omitted in this example. The pulse condition of the discharge treated by the discharge surface under the electrode produced is carried out under the same conditions as those shown in the above first figure. The result of the experiment, If the compressive strength is lower than i 6〇MPa, the stacking process is performed on the surface of the workpiece, but when it is more than the compressive strength, it will become the removal process of the workpiece surface. When the electrode strength of the Ni powder having a particle diameter of 50 nm was examined, it was found that the surface of the electrode for the formation of an appropriate film for the discharge surface treatment using the powder of Ni powder requires one of the evaluations of the electrode for the formation of the film. 1 A method of 60 MPa or less. As described above, the compressive strength of an electrode produced by compression molding of a powder is determined by the number of combinations of particles and particles contained per unit volume. The number of combinations of particles and particles contained in the particles is increased, and the compressive strength is increased. Further, as described above, it is found that the discharge surface treatment of the powdered powder electrode using the powder having an average particle diameter of 5 〇 nm is appropriate. One of the evaluations of the electrode for film formation requires management of a compressive strength of 16 MPa or less. Such a finding, as with an average particle size of 1·2// When the results of the case of m are combined, it is indicated that the compressive strength of the electrode capable of forming a thick film differs depending on the average particle diameter. Further, as an appropriate electrode for film formation, the compression of the pointer The value of the strength is not the same as the material of the electrode material as long as the average particle diameter is the same. For example, if the electrode for discharge surface treatment is formed from a powder having an average particle diameter of 315,550, 44,128,468, When a thick film is deposited, the compressive strength can be increased. Further, as another electrode material, a Co powder having an average particle diameter of 3 # m is used, and the result of the same experiment is observed. The compressive strength is about 50 MPa. In this case, one of the main factors determining whether or not a thick film can be formed by the discharge surface treatment is the hardness of the electrode. In other words, it has been confirmed that when a powder having an average particle diameter of 3 // m is used, the pressure at the time of compression molding or the heating temperature is changed to produce an electrode having a compressive strength of 50 MPa or less, and the electrode is used to perform discharge surface treatment, A thick film is formed on the surface of the workpiece. In this case, since the compressive strength of the electrode produced by compression molding of the powder is determined by the number of combinations of particles and particles contained per unit volume, it is one of the electrode evaluation indexes for forming an appropriate film. The value of the compressive strength is not the same as the material of the electrode material as long as the average particle diameter is the same. Therefore, if it is judged whether or not the electrode for discharge surface treatment is formed of a powder having a large average particle diameter, whether or not a thick film can be deposited, it is necessary to lower the compressive strength. Fig. 11 is a graph showing the relationship between the average particle diameter and the compressive strength of an electrode capable of depositing a thick film. In Fig. 11, the horizontal axis represents the average particle diameter Um of the powder constituting the electrode for discharge surface treatment on a logarithmic scale, and the vertical axis represents the cumulative limit compressive strength of the compressive strength of the electrode capable of forming a film on the surface of the workpiece (MPa). ). As shown in the figure, the smaller the average particle size, the more the packing limit compressive strength is increased. According to the fourth embodiment, the discharge surface treatment electrode which is produced by using the electrode having the average particle diameter of 丨 "paw powder" as 315550 45 1284682 and having a compressive strength of 100 MPa or less is subjected to discharge surface treatment. A dense thick film having lubricity in a high-temperature environment is formed on the workpiece. Further, when the powder having an average particle diameter of 50 nm, the compressive strength can be ΐ6〇Μρ& or less, and the average particle diameter is 3#m. In the case of powder, the electrode for discharge surface treatment is produced so that the compressive strength can be 50 MPa or less, and the electrode for discharge surface treatment is used to perform discharge surface treatment, that is, a dense thick film having lubricity in a high temperature environment can be formed on the workpiece. Further, according to the fourth embodiment, when the electrode for discharge surface treatment is used for the discharge surface treatment, the compressive strength can be used to evaluate whether or not the thick film is deposited on the workpiece. It can be applied to the evaluation of the electrode when the electrode for discharge surface treatment is mass-produced under the same conditions. Specifically, t will be the next large amount from the same material. The measurement results of the compressive strength of one or a plurality of electrodes extracted from the produced electrodes are used as evaluators of the simultaneously fabricated electrodes, whereby the quality of all the electrodes can be managed even when the electrodes are mass-produced. In the fifth embodiment, the discharge surface treatment for the metal powder is used as the powder surface electrode, and the electrode for discharge surface treatment in which the discharge can be stabilized without reducing the surface roughness and the thick film can be deposited can be described. As described in the first to third embodiments, when a thick mold is formed on the surface of the workpiece by the discharge surface treatment, it is necessary to add a material which does not form a carbide or a material which is difficult to form carbides to the electrode material. The condition of the material with the highest composition. From the 'addition only to the material that does not form carbides 315550 46 1284682 or the material that is difficult to form carbides in the electrode. The middle T tooth has the upper surface of the workpiece, and the medium thick film will remain in the middle. Therefore, it is difficult to form a dense film. Therefore, in the fifth embodiment, the disk At γ > The technique required for the dense film is described here. Here, an alloy containing Cr 3〇%, Ni 3%, M〇2%, w 5%, and 3% Co as a base material is used (hereinafter, referred to as C〇 alloy) is described as an example. A commercially available product is used for such a Co alloy powder. In addition, in the case of a c〇 alloy, "the alloy is contained in the alloy, and the alloy is contained in the alloy. %, %%, etc., or alloys based on ruthenium. 20%, 10%, 15%, etc. . It is an alloy of a base material, etc., as long as it is a base containing Co. From the average particle size 3 " m degree c. The alloy powder was subjected to the steps of the above Fig. 2 to manufacture an electrode for discharge surface treatment. At this time, the pressurization pressure of the step S" is preferably from 93 to the degree of milk. If the force is high, the electrode will have a deviation in hardness, or an air crack will occur on the electrode during pressurization. When the eight-purpose electrode at the discharge surface is formed by using the co alloy powder produced in the above manner to perform the discharge surface treatment, a film of gold is formed on the surface of the workpiece. However, from the experiments of the inventors and the like, it was found that the performance of the film = the ratio of the powder of the primary electrode material in the electrode has a large influence. Because the = system is made by forming the material at the end of the f-forming material, it becomes a emptiness. If there is too much space, the electrode strength will decrease so that: the hunting is performed by the pulse of the discharge. The supply of materials, for example, the phenomenon that the electrode is collapsed in a wide range due to the impact of the discharge. Another 315550 47 1284682 On the one hand, if the space is too small, the electrode is too tightly bonded, and the discharge pulse occurs. The supply of the electrode material is reduced, so that a thick film cannot be formed. The powder having a particle size of about 3 // m is used to pulverize a powder having a particle diameter of several tens/m, and the particle diameter is The particle size distribution is a powder having a distribution with a peak of 3//m. When such a relatively uniform particle size powder is compression-molded to produce an electrode, the electrode material can be formed well according to experiments by the present inventors. The proportion of the volume occupied by the electrode volume of the electrode of the film (the rest is space) is in the range of 25% to 5%. However, for example, the ratio of the volume of the electrode material (hereinafter, referred to as the ratio of the electrode material) At 25 〇/〇, the electrode is soft and has insufficient feeling of strength. Conversely, if the ratio of the electrode material is 5〇%, it is quite hard and partially produced as an electrode. In the case of air cracking, the outline of the state of the film caused by the ratio of the volume of the electrode material is shown in Table 1. However, such a ratio, t is somewhat due to the distribution of the particle size of the powder, etc. For example, when a powder having a broad particle size distribution is used, there is a tendency that the space ratio of the electrode (= (100% of the electrode material volume)) is lowered. Conversely, if a powder having a narrow particle size distribution is used, When there is a tendency for the space of the electrode to increase. I曰315550 48 1284682 Table 1 The ratio of the volume of the electrode material is 15% of the state of the film. The electrode collapses and cannot be used 20%. Although the film can be formed, the state is 25%. Although it is porous, it can form a thick film 30% to form a dense thick film 40% to form a dense thick film 50%. Although a dense thick film can be formed, the formation of the film is slow. 55% removal of the workpiece So that can't On the other hand, when a powder having a different particle diameter is mixed, for example, when a powder having a particle diameter of 6 /zm is mixed in a particle size of 3 // m used in the above examples, the volume of the electrode material is The ratio of the electrode volume of the electrode capable of forming a good film is in the range of 40 to 65%. However, when the ratio of the volume of the electrode material is 40%, the electrode is relatively soft and has insufficient feeling of strength. On the other hand, if the ratio of the volume of the electrode material is 65 %, it is quite hard as an electrode. The outline of the state of the film caused by the ratio of the volume of the electrode material in this case is shown in Table 2. Table 2 The ratio of the volume of the electrode material is 30% of the state of the film. The electrode collapses and cannot be used. 35% can form a film, but the state of laxity is 40%. Although it is porous, it can form a thick film 50% to form a dense Thick film 60% can form a dense thick film of 65%. Although it can form a dense thick film, the formation of the film is slow. 70% of the workpiece is removed so that a thick film cannot be formed. According to the fifth embodiment, the discharge surface treatment electrode having a volume ratio of the electrode material in consideration of the volume of the electrode is used to carry out the discharge surface treatment of 49 315 550 1284682, even if the metal powder is used as a raw material. The electrode for discharge surface treatment can also form a dense film having no voids on the workpiece. Further, in the above Patent Document 2, in the case of a ceramic electrode which can be formed at an extremely high pressure, there is a recording using an electrode which is compression-molded to a theoretical density of 5 to 90%, but it is not the present embodiment. Form 5 forms a thick film of dense metal, so its technical range, use, and effect are also different. (Embodiment 6) In the sixth embodiment, a discharge surface treatment for depositing a thick film can be carried out by using a discharge surface treatment electrode produced by compression molding of a metal powder. In the electrode for discharge surface treatment manufactured by the process shown in Fig. 2, if the combination of the powder and the powder is strong, the heat transfer between the powder proceeds smoothly, that is, the thermal conductivity increases, and conversely, if the combination is weak The heat transfer between the powders does not proceed smoothly, and the thermal conductivity is lowered. If the heating temperature is increased, the combination of the powder and the metal of the powder progresses, and the heat transfer rate of the electrode increases. Conversely, if the heating temperature is lowered, the powder does not progress to the metal of the powder, and the thermal conductivity of the electrode is lowered. For example, the thermal conductivity of the electrode (for each unit length and unit temperature is low, due to the local high temperature, the electrode material can be vaporized instantaneously by the discharge of the discharge. Taking the molten portion or the solid portion of the electrode, which is separated from the electrode, is deposited on the surface of the workpiece. On the one hand, if the heat transfer rate of the electrode is high, it is difficult to diffuse due to heat, and 315550 50 1284682 is generated to generate a heat spot. Therefore, the electrode material is not vaporized. Therefore, the explosive force does not occur, so that the electrode material cannot be supplied. Therefore, when a thick film is to be formed on the surface of the workpiece, it is necessary to deposit a material on the workpiece which is larger than the constituent material. Since the amount of the electrode material is large, the thermal conductivity of the electrode for discharge surface treatment needs to be lower. Hereinafter, the method of reducing the thermal conductivity of the electrode for discharge surface treatment will be described. According to the process of Fig. 2, only the average particle is used. Diameter 1 · 2 # alloy alloy powder to make a 50mm x 11 mm x 5.5mm shape discharge surface treatment electrode. The alloy powder used at this time is Cr 25wt %, Ni 10wt%, W 7wt%, C 0.5wt%, and the balance is the ratio of Co. In addition to the alloy powder of this composition, M〇283⁄4, Cr 17wt%, Si 3wt% can be used, and the rest is The alloy of the proportion of Co, or the alloy of Cr 28% wt%, Ni 5 wt%, W 19 wt%, and the balance of Co. Further, in the pressurization step of step S6 of Fig. 2, 67] V [pa The pressure compresses the powder, and, in order to obtain an electrode having a different hardness, in the heating step of step S7, the powder compact is heated in a vacuum furnace at each temperature of 73 Torr and 750 ° for 1 hour. Further, the discharge surface treatment was carried out under the same discharge pulse conditions as in the fourth embodiment. First, the thermal conductivity of each electrode produced by changing the heating temperature was investigated by a laser flash method. The thermal conductivity of the electrode heated at 73 ° C is 10 〇 W / mK, and the thermal conductivity of the electrode heated at 750 ° C is Kw / mK. Figure 12 ' shows the use of thermal conductivity is not the same When the discharge surface treatment electrode is subjected to discharge surface treatment for 5 minutes, the surface formed on the surface of the workpiece is 51 315550 1 284682
被膜厚度與放電表面處理用電極之熱傳導率之關係圖。在 第12圖中,橫轴表示放電表面處理用電極之熱傳導率 (W/mK),縱轴表示使用具有橫軸所示之熱傳導率的放電表 面處理用電極實施放電表面處理時在工件表面所形成的被 膜厚度(mm)。在此,如縱軸之被膜厚度值為負時,則表示 去除加工之意。如此圖所示,加工時間相同時,熱傳導率 愈低被膜厚度會愈厚。又,電極之熱傳導率約u.8w/mK 11 時 以上時,則會成為去除工件表面之去除加工。由此,從實 驗發現,如欲形成厚被膜時,電極之熱傳導率需要在 如欲形成0.2mm以上之厚被膜 • 8W/mK以下。特別是 ,則需要電極之熱傳導率為1〇w/mK以下 ^在放電表面處理後,如觀察熱傳導率為12w/mK之放 電表面處理用電極之經發生放電的面時,可確認電極之粉 末熔融,並經再凝固的結果之金屬光澤。亦即,經發生放 電之面並非係粉末互相稱微結合的壓粉體,而係成為金屬 粉末熔融後互相毒占接所形成的再凝固體。另_方面,敎傳 導率為麵mK之放電表面處理用電極之經發生放電的'面 之狀態,係未能觀察到光澤。 ,如此,熱傳導率為10w/mK以上時,則由於電極上不 會形成熱斑點,並電極與電弧㈣柱相接的部分殆不氣化 ^故’爆發力變小以致不能完全去除電極上所形成的溶融 ^而殘留在電極表面。並且,由於放電之反覆進行而其 炫融域蓄積,電極表面上形成經熔融、再凝固的金屬層。 如形成有此種金屬層,則不再有從電極移行到工件的電極 315550 52 1284682 卷而成為去除工件表面的去除加工。 另外’在本實施形態6 +,係就具有如上述組成的合 、/、末之It I加以說明者’惟在C。合金粉末、犯合金粉A graph showing the relationship between the film thickness and the thermal conductivity of the electrode for discharge surface treatment. In Fig. 12, the horizontal axis represents the thermal conductivity (W/mK) of the electrode for discharge surface treatment, and the vertical axis represents the surface of the workpiece when the discharge surface treatment is performed using the electrode for discharge surface treatment having the thermal conductivity indicated by the horizontal axis. The film thickness (mm) formed. Here, if the film thickness value of the vertical axis is negative, it means that the processing is removed. As shown in the figure, the lower the thermal conductivity, the thicker the film thickness will be when the processing time is the same. Further, when the thermal conductivity of the electrode is about u.8 w/mK 11 or more, the removal of the surface of the workpiece is removed. Therefore, it has been found from experiments that if a thick film is to be formed, the thermal conductivity of the electrode needs to be formed to a thickness of 0.2 mm or more and 8 W/mK or less. In particular, the thermal conductivity of the electrode is required to be 1 〇 w/mK or less. ^ After the discharge surface treatment, if the surface of the discharge surface treatment electrode having a thermal conductivity of 12 w/mK is observed, the powder of the electrode can be confirmed. The metallic luster that melts and resolidifies. That is, the surface on which the discharge occurs is not a compact which is micro-bonded to each other, but is a re-solidified body formed by the mutual toxic occupation of the metal powder after melting. On the other hand, the 敎 conductivity is a state in which the surface of the discharge surface treatment electrode of the surface mK is discharged, and no gloss is observed. Therefore, when the thermal conductivity is 10 w/mK or more, since hot spots are not formed on the electrodes, and the portion where the electrodes are in contact with the arc (four) column is not vaporized, the explosive force is so small that the electrode cannot be completely removed. The solution melts and remains on the surface of the electrode. Further, since the discharge is repeated, the fused domain is accumulated, and a molten, resolidified metal layer is formed on the surface of the electrode. If such a metal layer is formed, there is no longer a roll of electrode 315550 52 1284682 that travels from the electrode to the workpiece to remove the workpiece surface. In addition, in the present embodiment, the expression "6" has the composition of the above-mentioned composition, and the final It I is described as "only". Alloy powder, alloy powder
或a金粕末之情形,如同樣製造熱傳導率丨〇 W/mK 乂下的電極,並使用該電極以實施放電表面處理,則亦能 形成厚被膜。 電極係將粉末壓縮成型的壓粉體,而決定(影響)電極 之熱傳=率者,並非電極粉末之材質,而係粉末與粉末之 、’η &狀心因此,對所有材料,如按熱傳導率(1 〇 W/mK) 以下之方式製造電極,則能在卫件上形成厚被膜。例如, 即使使用熱傳導率良好的Cu(約300W/mK)或 Al(200W/mK),祇要是從其粉末所製造的電極之熱傳導率 能符合上述之熱傳導率(1〇w/mK)者,則能在工件表面上形 成厚被膜,惟如其熱傳導率為上述之熱傳導率以上時,則 不能在工件上形成被膜。 從本實施形態6,由實驗可證明如使用熱傳導率在 10W/mK以下之電極,則可形成厚被膜,亦經證明將其值 用為形成厚被膜上之電極所需要的指標時之有用性。如 此,如作為電極之指標而使用熱傳導率,則有可簡單評估 能形成厚被膜的電極之好處(merit)。 另外,關於放電加工用之電極之熱傳導率方面,曰本 專利特開昭54-124806號公報中記載有將電極之熱傳導率 作成0.5Kcal/cm · sec · °C以下的作法。但,該曰本專利特 開昭54-124806號所記載之發明,係以避免電極之消耗, 315550 53 1284682 並將電極形狀抄錄 者,而非如本發明 理用電極者。 加工於工件上為目的之有關放電加 之有關在工件上形成被膜的放電表 工 面處 又,日本專利特開昭54_124806號公報中,雖然並無 …、傳導率之下限值之記載,惟很明顯可瞭解,如降低電極 之熱傳導率(例如,卿/mK)時,則不能達成電極上形成熱 斑點、消耗電極、並抄錄加工形狀等的放電加工之目的。 亦p與如本實知幵》態6般之積極消耗電極而在工件上形 成被膜的放電表面處^ 电衣®慝理之方式,其目的與手法截然有所不 同者再者,该 〇.5Kcal/cm· _ · 〇c(=2〇93〇3w/mK)之值 過大’較先d忍為熱傳導率最高之純銅之值398〇w/mK高 出甚多。 如依照本實施形態6,由於使用熱傳導率在1 OW/mK 以下之放電表面處理用電極以實施放電表面處理之方式, 故即使以金屬粉末作為原料所製造的放電表面處理用電 極’仍然能在工件上形成原被膜。 如上所說明,如依照本發明,由於按照粉末之粒徑, 將放電表面處理用電極之硬度、其壓縮強度、電極材料體 積在其體積所佔之比例、以及其熱傳導率等能符合既定之 範圍内之方式製造,並使用其電極以實施放電表面處理之 方式之故,能於工件上形成緻密的厚被膜。 實施形態7 在本實施形態7中,作為電極之評價方法,就依既定 條件實際使放電連續發生,從電極之消耗量、處理時間、 54 315550 1284682 所形成的被膜厚度評價電極之優劣之方法,加以說明。 將貝鉍形恶4所示合金粉末(經粉碎為平均粒徑1 ·2 # m者)壓縮成型,以製造5〇mmx Ummx 5 形狀之放電 表面處理用電極。本電極製造之過程,係與實施形態4者 相同。如此所製造的電極係在管理粉末粒徑、製造條件之 下所製造者,惟有時會因製造時之氣溫或濕度之不同、粉 末之粉碎狀態、臘與粉末之混合狀態等而產生偏差。在上 述中’係就藉由電極硬度等以管理此等偏差的方法,加以 說明,惟除此種方法之外,亦可使用電極直接實施被膜之 形成以調查。 乐圖至第 一 ·〜、π % %褙田风腺試驗以判定 電極之優劣的方法之概要用的圖。在此等圖中,對與實施 形態1之第i圖所使用者之同樣之構成要件則附以同樣符 號。在此’此等圖係為說明有關判定方法之概略用的圖之 故’電源或驅動軸等之構成要件則加以省略而未圖示。 本實施形態7之電極之評價方法中,係使用如上述方 式所製造的電極並藉由既定量搜 里 < 孜電表面處理以實施被膜 =成。在上述電極之情形,從處理之簡便性來看,最好 言凡5.5mm之面能成為放電面之方式設置,惟亦可 叹置為其他面能成為放電 -^ 式1先,如第13A圖所 不,實施電池12盥工件n „ + a , nOr in the case of a gold crucible, if an electrode having a thermal conductivity 丨〇 W/mK 同样 is also produced, and the electrode is used to perform discharge surface treatment, a thick film can also be formed. The electrode is a powder compacted into a powder, and the heat transfer rate of the electrode is determined (influenced), not the material of the electrode powder, but the powder and the powder, 'η & heart shape, therefore, for all materials, such as When the electrode is fabricated in a thermal conductivity (1 〇W/mK) or less, a thick film can be formed on the guard. For example, even if Cu (about 300 W/mK) or Al (200 W/mK) having good thermal conductivity is used, as long as the thermal conductivity of the electrode made from the powder can satisfy the above thermal conductivity (1 〇 w/mK), A thick film can be formed on the surface of the workpiece. However, if the thermal conductivity is equal to or higher than the above thermal conductivity, the film cannot be formed on the workpiece. From the sixth embodiment, it has been experimentally confirmed that if an electrode having a thermal conductivity of 10 W/mK or less is used, a thick film can be formed, and the value is also proved to be useful as an index required for forming an electrode on a thick film. . Thus, if the thermal conductivity is used as an index of the electrode, there is a merit that the electrode capable of forming a thick film can be easily evaluated. In the case of the thermal conductivity of the electrode for electric discharge machining, the thermal conductivity of the electrode is set to 0.5 Kcal/cm · sec · ° C or less, as described in Japanese Laid-Open Patent Publication No. SHO 54-124806. However, the invention described in Japanese Laid-Open Patent Publication No. SHO 54-124806 is to avoid the consumption of electrodes, 315550 53 1284682 and to rip the electrode shape instead of the electrode of the present invention. In the case of the discharge related to the workpiece, the discharge table is formed on the workpiece, and in the Japanese Patent Laid-Open Publication No. 54-124806, although there is no record of the lower limit of the conductivity, it is obvious. It can be understood that, for example, when the thermal conductivity of the electrode is lowered (for example, qing/mK), the purpose of forming an electric spot on the electrode, consuming the electrode, and copying the processed shape or the like cannot be achieved. Also, the method of actively consuming the electrode and forming the film on the workpiece at the discharge surface of the film as shown in Fig. 6 is the same as the method of the electric clothing®, and the purpose and method are completely different. 5Kcal/cm· _ · 〇c(=2〇93〇3w/mK) is too large. The value of pure copper, which is the highest thermal conductivity, is 398〇w/mK. According to the sixth embodiment, the electrode for discharge surface treatment having a thermal conductivity of 1 OW/mK or less is used for the discharge surface treatment, so that the electrode for discharge surface treatment made of metal powder as a raw material can still The original film is formed on the workpiece. As described above, according to the present invention, the hardness of the electrode for discharge surface treatment, the compressive strength thereof, the proportion of the volume of the electrode material in its volume, and the thermal conductivity thereof can conform to the predetermined range in accordance with the particle diameter of the powder. A dense thick film can be formed on the workpiece by manufacturing it in the manner of using the electrode to perform the discharge surface treatment. (Embodiment 7) In the seventh embodiment, as a method for evaluating an electrode, a method in which the discharge is continuously generated according to a predetermined condition, and the electrode is used to evaluate the thickness of the electrode from the consumption amount of the electrode, the processing time, and the thickness of the film formed by 54 315 550 1284682, Explain. An alloy powder of the shellfish type 4 (which was pulverized to have an average particle diameter of 1 · 2 # m) was compression-molded to produce a 5 〇 mm x Umm x 5 shaped electrode for discharge surface treatment. The process for producing the electrode is the same as that of the fourth embodiment. The electrode produced in this manner is manufactured under the management of the powder particle size and the production conditions, but may vary depending on the temperature or humidity at the time of production, the state of pulverization of the powder, the state of mixing of the wax and the powder, and the like. In the above description, the method of managing the deviation by the electrode hardness or the like is described. However, in addition to this method, the formation of the film may be directly performed using an electrode to investigate. The figure used for the outline of the method of determining the merits of the electrodes in the first to the first, ~, π % %. In the figures, the same components as those of the user of the first embodiment of the first embodiment are given the same symbols. Here, the drawings are diagrams for explaining the outline of the determination method. The components of the power source, the drive shaft, and the like are omitted and are not shown. In the method for evaluating an electrode according to the seventh embodiment, the electrode manufactured by the above method is used, and the film is formed by quantitatively searching for < In the case of the above-mentioned electrode, from the viewpoint of the simplicity of the treatment, it is preferable that the surface of 5.5 mm can be set as the discharge surface, but it can be set as the other surface to become the discharge-^ type 1 first, such as the 13A. Figure No, implement the battery 12 盥 workpiece n „ + a , n
,、件11間之定位工作。接著,如第13B 圖所不,開始放電,以進行 皮膜形成。然後,如第13C圖 不,工件11上將形成被膜14。 中,符號p表示放電之電弧& / 圖及第130圖 冤之電弧柱。在此,將電極12往圖之 315550 55 1284682 z軸之朝下方向驅動的距離保持在既定之值,以測定成膜 形成時間及所形成的被膜厚度。在此,z軸方向之推送量 係作成2mm。由於將電極朝z軸方向推送2mm之故,被 膜形成後之電極消耗量(長度)為2mm+(所形成的被膜厚 度)+ (放電間隙(gap))。放電間隙為數1〇至1〇〇#m程度。 又,放電表面處理條件,係作成峰值電流值ie=i〇A、放電 持續時間(放電脈料間)te =…。將實際實施成膜試驗的 結果’表不表3中。 表3 電極號碼 ~N^T No.2 No.3' "N^T4 No.5 (分鐘)16 20 被膜厚度(mm) ^35""οΤϊΤ 抗張強度(MPa) 35 25 # ^ , ^--—--20 " ,電極號碼係對實施試驗的電極所附以的號 =被膜形成時間表示放電表面處理時間,被膜厚度表示 ::膜形成時間内所形成的被膜之厚度,而抗張強度表示 吏用黏接劑將試驗片黏接於工件u上所形成的被膜上 吏用抗張強度試驗機將黏接於工件與被膜上的試驗 片貫施抗張試驗而被膜破裂的壓力。 、電極號No」之電極係被膜形成時間為16分鐘,當時 之被膜厚度為〇.35mm,而電極號碼如.3、4亦略為相同。 電極波碼Νο.2電極如與電極號碼Ν。 被 時間為較長之20八扭私子破膜形成 之雷$ 刀、里,惟被膜厚度較薄。電極號碼No.5 之電極,相反地,被膜形成時間為較短之13分鐘,而被膜 315550 56 1284682 厚度則成為G.3〇mm。從此等電極所形成的被膜強度,不拘 处里夺間&通常(1 6分鐘)為長或短,均有降低的傾向,可 ^處理時間或能形成的被膜厚度方面存在有最適值。此種 最適值’會因電極材質、電極形狀、處理條件等而異,惟 可從依既定條件下所實施的被膜形成時之被膜形成時間或 被膜厚度,判斷電極之優劣。此種判斷之基準可設定為例 如1平均處理時間之正負丨成者作為優判斷,而將脫離 該範圍者作成劣等之方式。 又,被膜之厚度方面亦可作成同樣方式。例如,在上 述試驗中係將電極之推送量作成既定之值而實施試驗者, 惟亦可作成將處理時間作成既定時間並將當時之被膜 作為判斷基準並將平均值之正負丨成者作為優判斷,而^ 脫離該範圍者作為劣之方式設定。 如採用本實施形態7,則可使用藉由電極而在工件上 依既定之條件形成被膜時之被膜形成時間或被膜厚度,以 判定電極之優劣。 (產業上之利用可能性) 如上所述,本發明適合於能使工件表面上形成厚被膜 的處理自動化的放電表面處理裝置。 [圖式簡單說明] 第1圖係表示在放電表面處理裴置中的放電表面處理 之概略的圖, 第2圖係表示放電表面處理用電極之製遂過程的流程 圖, 315550 57 1284682 第3圖係依模式性表示將粉末成型時之成型器之狀態 的剖面圖, 第4A圖係表示放電時施加於放電表面處理用電極與 工件間之電壓波形的圖, 第4B圖係表示放電時對放電表面處理裝置流動的電 流之電流波形, 第5圖係表示改變對Cr2、C2粉末混合的c〇粉末量所 製造的放電表面處理用電極上因C〇量之變化所引起的被 膜尽度的關係的圖, 第6圖係表示放電表面處理用電極中未含有不會形成 碳化物的材料或難以形成碳化物的材料時對處理時間的被 膜形成之情況圖, 第7圖.使用c〇含量為70體積%之電極以實施放電 表面處理時所形成的被膜之照片, “第8圖係表示改變Cr/2 30。/。至Co 70。/。之體積比之放 電表面處理用電極之硬度時之厚膜形成之狀態的圖, 第9圖係表示測定電極之壓縮測定的實驗裝置之概 的照片, 第1〇圖係表示電極之壓縮強度與被模厚度的關係 第11圖係表示平均粒徑與能實施被膜之堆積的電極 之壓縮強度之間的關係圖, 第^圖係表示使用熱傳導率不同的放電表面處理用 電極以貫施放電處理時於株 才於件表面所形成的被膜厚度與方 315550 58 1284682 電表面處理甩電極之熱傳導率之間的關係圖, 第13A圖係表示依成膜試驗以判定電極優劣的方法之 概要圖, 第13B圖係表示依成膜試驗以判定電極優劣的方法之 概要圖, 第1 3 C圖係表示依成膜試驗以判定電極優劣的方法之 概要圖。 (元件符號之說明) 11 工件 12 放電表面處理用電極 13 放電表面處理用電源 14 被膜 15 加工液 16 加工槽 21 電極粒子 22 氣體中之成分 24 與氣體中之成分反應者 101 粉末 103 上衝床 104 下衝床 105 金屬模具(鎮) 315550 59, and the positioning of the 11 pieces of work. Next, as shown in Fig. 13B, discharge is started to form a film. Then, as shown in Fig. 13C, the film 14 will be formed on the workpiece 11. In the middle, the symbol p denotes the arc of the discharge & / Fig. and the arc of the figure of Fig. 130. Here, the distance at which the electrode 12 is driven in the downward direction of the 315550 55 1284682 z-axis of the figure is maintained at a predetermined value to determine the film formation time and the film thickness formed. Here, the pushing amount in the z-axis direction is made 2 mm. Since the electrode was pushed 2 mm in the z-axis direction, the electrode consumption (length) after the formation of the film was 2 mm + (the thickness of the formed film) + (discharge gap). The discharge gap is from 1 〇 to 1 〇〇 #m. Further, the discharge surface treatment conditions were made into a peak current value ie = i 〇 A, and a discharge duration (between discharge pulsations) te = .... The results of actual implementation of the film formation test are shown in Table 3. Table 3 Electrode number ~N^T No.2 No.3' "N^T4 No.5 (minutes) 16 20 Film thickness (mm) ^35""οΤϊΤ Tensile strength (MPa) 35 25 # ^ , ^-----20 " , the electrode number is the number attached to the electrode to be tested = the film formation time indicates the discharge surface treatment time, and the film thickness indicates: the thickness of the film formed during the film formation time, and Tensile strength means that the test piece is adhered to the film formed on the workpiece u by an adhesive, and the test piece adhered to the workpiece and the film is subjected to a tensile test by a tensile strength tester to break the film. pressure. The electrode formation time of the electrode No. was "16 minutes, and the film thickness at that time was 〇.35 mm, and the electrode numbers such as .3 and 4 were slightly the same. The electrode wave code Νο.2 electrode is like the electrode number Ν. The time is longer than the 20-eight twisted smashed film formed by the thunder, the knife, but the film thickness is thin. The electrode of the electrode No. 5, on the contrary, the film formation time was 13 minutes shorter, and the thickness of the film 315550 56 1284682 was G.3 〇 mm. The strength of the film formed from these electrodes is not limited to the length of the film, and usually (16 minutes) is long or short, and there is a tendency to decrease, and there is an optimum value in the treatment time or the thickness of the film which can be formed. Such an optimum value varies depending on the electrode material, the electrode shape, the processing conditions, and the like, and the merits of the electrode can be judged from the film formation time or the film thickness at the time of formation of the film under the predetermined conditions. The basis for such judgment can be set as, for example, a positive or negative average of the average processing time as an excellent judgment, and a person who is out of the range is made inferior. Further, the thickness of the film can also be made in the same manner. For example, in the above test, the test is carried out by setting the amount of push of the electrode to a predetermined value, but it is also possible to make the treatment time a predetermined time and use the film at that time as a criterion for judgment and to calculate the positive and negative values of the average value. Judging, and ^ is out of the range as a bad way to set. According to the seventh embodiment, the film formation time or the film thickness when the film is formed on the workpiece under predetermined conditions by the electrode can be used to determine the merit of the electrode. (Industrial Applicability) As described above, the present invention is suitable for a discharge surface treatment apparatus which can automate the process of forming a thick film on the surface of a workpiece. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a schematic view showing a discharge surface treatment in a discharge surface treatment device, and Fig. 2 is a flow chart showing a process for preparing a discharge surface treatment electrode, 315550 57 1284682 3 The figure is a cross-sectional view showing the state of the former when the powder is molded, and FIG. 4A is a view showing a voltage waveform applied between the electrode for discharge surface treatment and the workpiece during discharge, and FIG. 4B is a view showing a state of discharge during discharge. The current waveform of the current flowing through the discharge surface treatment device, and Fig. 5 is a graph showing the film endurance due to the change in the amount of C〇 on the electrode for discharge surface treatment produced by changing the amount of c〇 powder mixed with the Cr2 and C2 powders. Fig. 6 is a view showing a state of formation of a film at a processing time when a material for a discharge surface treatment does not contain a material which does not form a carbide or a material which is difficult to form a carbide, and Fig. 7 shows a content of c〇 A photo of a film formed by performing a discharge surface treatment on a 70% by volume electrode, "Fig. 8 shows a change in the volume ratio of Cr/2 30% to Co 70. FIG. 9 is a view showing a state in which a thick film is formed in the hardness of the electrode for processing, and FIG. 9 is a photograph showing an experimental apparatus for measuring the compression of the electrode, and the first drawing shows the relationship between the compressive strength of the electrode and the thickness of the mold. Fig. 11 is a graph showing the relationship between the average particle diameter and the compressive strength of the electrode capable of performing deposition of the film, and Fig. 4 is a view showing the use of the electrode for discharge surface treatment having different thermal conductivity to perform the discharge treatment. The relationship between the thickness of the film formed on the surface and the thermal conductivity of the electrode surface treated with 315550 58 1284682, and Fig. 13A shows the outline of the method for determining the quality of the electrode according to the film formation test, and Fig. 13B shows the A schematic diagram of a method for determining the merits of an electrode by a film formation test, and a schematic diagram of a method for determining the merits of an electrode according to a film formation test. (Description of component symbols) 11 Workpiece 12 Discharge of electrode 13 for discharge surface treatment Surface treatment power supply 14 Film 15 Processing fluid 16 Processing tank 21 Electrode particles 22 Component in gas 24 Reactant with gas components 101 Powder 103 Upper punch 104 Lower punch 105 Metal mold (town) 315550 59
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JP2002304730A JP3847697B2 (en) | 2002-10-18 | 2002-10-18 | Electrode for discharge surface treatment |
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JP2003166010 | 2003-06-11 | ||
PCT/JP2004/000848 WO2004108990A1 (en) | 2003-06-05 | 2004-01-29 | Discharge surface treating electrode, production method and evaluation method for discharge surface treating electrode, discharge surface treating device and discharge surface treating method |
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