TWI577488B - Surface processing method - Google Patents

Surface processing method Download PDF

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TWI577488B
TWI577488B TW103139756A TW103139756A TWI577488B TW I577488 B TWI577488 B TW I577488B TW 103139756 A TW103139756 A TW 103139756A TW 103139756 A TW103139756 A TW 103139756A TW I577488 B TWI577488 B TW I577488B
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laser light
laser
workpiece
processing method
light
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TW103139756A
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TW201618879A (en
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陳園迪
蔡武融
劉松河
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財團法人工業技術研究院
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Description

表面加工方法 Surface processing method

本揭露是有關於一種表面加工方法,且特別是有關於一種增加加工表面平坦度的表面加工方法。 The present disclosure relates to a surface processing method, and more particularly to a surface processing method for increasing the flatness of a machined surface.

模具產業為製造業的基礎,且拋光作業流程的改善為提升模具的生產速度的關鍵一步。拋光作業除了直接影響到模具的品質,此步驟的成本更佔模具製造的30~40%。目前模具拋光主要利用機械或微放電技術再加上人工拋光來降低加工表面的表面粗糙度。然而精微元件(如高亮度LED及IC封裝模具)的尺度越來越小、表面形貌也越來複雜,因此其表面粗糙度的要求也越來越小(如:Ra<200nm),而傳統機械或人工拋光技術不論在加工品質控制與加工效能上,都無法應付未來精密模具產業的需求。此外,使用人力進行操作拋光作業程序,人工拋光技術的培養及傳承不易,容易造成技術流失。為加速模具產業的發展,建立完整之自動化模具拋光系統勢在必行。 The mold industry is the foundation of the manufacturing industry, and the improvement of the polishing process is a key step in increasing the production speed of the mold. In addition to directly affecting the quality of the mold, the cost of this step is 30-40% of the mold manufacturing. At present, mold polishing mainly uses mechanical or micro-discharge technology plus manual polishing to reduce the surface roughness of the machined surface. However, the precision of fine components (such as high-brightness LEDs and IC package molds) is getting smaller and smaller, and the surface topography is becoming more complex, so the surface roughness requirements are getting smaller and smaller (eg Ra<200nm), while the traditional Mechanical or manual polishing technology cannot meet the needs of the future precision mold industry regardless of processing quality control and processing efficiency. In addition, the use of manpower to operate the polishing operation program, the cultivation and transfer of manual polishing technology is not easy, and it is easy to cause technology loss. In order to accelerate the development of the mold industry, it is imperative to establish a complete automated mold polishing system.

雷射拋光技術為近年來國際研究機構所注目的關鍵技術,被視為下一世代自動化模具拋光系統的主流,其優勢在於可 局部控制的加工精度及高產出效能等技術特點。但傳統雷射由於熱影響區大,會在拋光表面層產生重熔層,此重熔層將影響模具表面硬度與特性,且在表面會形成熔融的微凸起結構(如圖1示),此微凸起結構產生的機制為高低溫差所產生的回流造成,且這些凸起結構成為雷射拋光表面粗糙度難以再提升的主因。 Laser polishing technology is the key technology of international research institutions in recent years. It is regarded as the mainstream of the next generation of automated mold polishing system. Its advantage lies in Technical characteristics such as machining accuracy and high output efficiency of local control. However, due to the large heat-affected zone, the conventional laser will produce a remelted layer on the polished surface layer. This remelted layer will affect the hardness and characteristics of the mold surface, and a molten micro-convex structure will be formed on the surface (as shown in Figure 1). The mechanism generated by the micro-bump structure is caused by the reflow caused by the high and low temperature difference, and these convex structures become the main cause of the difficulty in further improving the surface roughness of the laser polishing.

傳統雷射拋光若要達到平坦化,需要進行兩道次雷射製程。第一道製程先將表面的起伏利用雷射熔融或剝除機制加以移除,此時工件的表面粗糙度可降低到數十微米之間,但表面仍呈現帶灰色或略呈白色的狀態,因光線在表面粗糙度數十微米的狀態下將會呈現散射,無法達到亮面的效果。Fraunhofer ILT為了解決此議題,提出兩道製程拋光的手法,如圖2。首先,第一道製程利用長脈衝雷射對材料表面進行平坦化製程,此時表面熔化深度可達100μm,表面粗糙度Ra達0.4~10μm。第一道製程處理完之後,接續再進入另一道製程,以奈秒雷射對於平坦面進行再熔化使工件表面亮澤化效果,表面粗糙度達0.2~0.8μm(200~800nm)。 To achieve flattening in conventional laser polishing, a two-pass laser process is required. The first process first removes the surface undulation by laser melting or stripping mechanism. At this time, the surface roughness of the workpiece can be reduced to several tens of micrometers, but the surface is still grayish or slightly white. Since the light will scatter at a surface roughness of several tens of micrometers, the effect of the bright surface cannot be achieved. In order to solve this problem, Fraunhofer ILT proposed two methods of polishing the process, as shown in Figure 2. First, the first process uses a long pulse laser to planarize the surface of the material. At this time, the surface melting depth can reach 100 μm, and the surface roughness Ra reaches 0.4 to 10 μm. After the first process is processed, another process is continued, and the nanosecond laser is used to re-melt the flat surface to brighten the surface of the workpiece, and the surface roughness is 0.2-0.8 μm (200-800 nm).

Fraunhofer ILT之兩道製程拋光後會產生兩層厚度不同之熔融層,如圖2示,且表面仍具有突起結構,Fraunhofer ILT之技術須花費比一般單道次雷射拋光雙倍的時間,增加許多額外的成本,且變質層較厚,緻密度也較差。 The two processes of the Fraunhofer ILT are polished to produce two layers of different thicknesses, as shown in Figure 2, and the surface still has a raised structure. The Fraunhofer ILT technology takes twice as long as the general single-pass laser polishing. There are many additional costs, and the metamorphic layer is thicker and the density is also poor.

本揭露提供一種增加工件表面平坦度的表面加工方法。 The present disclosure provides a surface processing method that increases the flatness of a surface of a workpiece.

本揭露的表面加工方法,至少包括下列步驟:提供雷射加工裝置,所述雷射加工裝置用以提供第一雷射光以及第二雷射光,且所述第一雷射光與所述第二雷射光之間相隔一段可調變距離;沿著加工方向移動所述雷射加工裝置以對工件進行掃描,其中所述雷射加工裝置提供第一道雷射光施加於工件上,所述工件受到所述第一道雷射光照射處熔融以形成熔融區,且隨著所述第一道雷射光的移動,所述熔融區內的工件材料熱回流並形成凸起結構;以及在所述凸起結構凝固前,所述雷射加工裝置提供第二道雷射光施加於所述凸起結構上,其中所述第二道雷射光的強度低於所述第一道雷射光的強度,以藉由所述第二道雷射光的光壓將所述凸起結構壓平。 The surface processing method of the present disclosure includes at least the following steps: providing a laser processing apparatus for providing first laser light and second laser light, and the first laser light and the second laser The illuminating light is separated by an adjustable variable distance; the laser processing apparatus is moved along the machining direction to scan the workpiece, wherein the laser processing apparatus provides a first laser light to be applied to the workpiece, the workpiece is subjected to Melting at the first laser light irradiation to form a melting zone, and with the movement of the first laser light, the workpiece material in the melting zone is thermally reflowed and forming a convex structure; and in the convex structure Prior to solidification, the laser processing apparatus provides a second laser beam applied to the raised structure, wherein the intensity of the second laser light is lower than the intensity of the first laser light The light pressure of the second laser light flattens the raised structure.

在本揭露表面加工方法的一實施例中,上述的第一道雷射光的光功率的範圍為30~4000W,且掃描速度範圍為1~200mm/s,而所述第二道雷射光的光功率範圍為0.0001~20W,且掃描速度範圍為1~200mm/s。 In an embodiment of the surface processing method of the present disclosure, the optical power of the first laser light ranges from 30 to 4000 W, and the scanning speed ranges from 1 to 200 mm/s, and the light of the second laser light The power range is 0.0001~20W, and the scanning speed ranges from 1~200mm/s.

在本揭露表面加工方法的一實施例中,上述的第一道雷射光與所述第二道雷射光先後通過工件上相同的一點的時距介於0~200ms之間。 In an embodiment of the surface processing method of the present disclosure, the time interval between the first laser light and the second laser light passing through the same point on the workpiece is between 0 and 200 ms.

在本揭露表面加工方法的一實施例中,沿著所述第一道雷射光的掃描軌跡,所述熔融區的定義是所述工件材料升溫至熔點以上的區域。 In an embodiment of the present surface processing method, along the scan trajectory of the first laser light, the melting zone is defined as a region where the workpiece material is heated above the melting point.

在本揭露表面加工方法的一實施例中,上述的第二道雷 射光的脈衝寬度小於1奈秒。 In an embodiment of the disclosed surface processing method, the second mine is The pulse width of the light is less than 1 nanosecond.

在本揭露表面加工方法的一實施例中,上述的第二道雷射光的能量小於工件的剝除閥值。 In an embodiment of the disclosed surface processing method, the energy of the second laser light is less than the stripping threshold of the workpiece.

在本揭露表面加工方法的一實施例中,上述的第二道雷射光的光斑直徑介於第一道雷射光的光斑直徑的0.8至1.5倍之間。 In an embodiment of the disclosed surface processing method, the spot diameter of the second laser light is between 0.8 and 1.5 times the spot diameter of the first laser light.

在本揭露表面加工方法的一實施例中,上述的第二道雷射光的光型為高斯分布或平頂光分布。 In an embodiment of the disclosed surface processing method, the light pattern of the second laser light is a Gaussian distribution or a flat top light distribution.

基於上述,本揭露表面加工方法利用在同一道製程中對工件表面進行序列式的雷射掃描,其中第一道雷射光使工件表面熔融,且在熔融區形成的凸起結構尚未凝固前利用強度小於第一道雷射光的第二道雷射光所產生的光壓壓平此凸起結構,減低了加工過程中因熱回流所造成的表面粗糙度、增加了工件的表面平坦度,且與一般表面加工方法相比提升了加工後工件的表面的緻密度。 Based on the above, the disclosed surface processing method utilizes a sequential laser scanning of the surface of the workpiece in the same process, wherein the first laser light melts the surface of the workpiece, and the convex structure formed in the molten region is not used before solidification. The light pressure generated by the second laser light smaller than the first laser light flattens the convex structure, reduces the surface roughness caused by heat reflow during processing, increases the surface flatness of the workpiece, and is generally The surface processing method increases the density of the surface of the workpiece after processing.

為讓本揭露的上述特徵和優點能更明顯易懂,下文特舉實施例,並配合所附圖式作詳細說明如下。 The above described features and advantages of the present invention will be more apparent from the following description.

200‧‧‧雷射加工裝置 200‧‧‧ Laser processing equipment

210、220‧‧‧雷射光源 210, 220‧‧ ‧ laser source

230‧‧‧擴束器 230‧‧‧beam expander

240、250、280、282‧‧‧角度可動式反射鏡 240, 250, 280, 282 ‧ ‧ angle movable mirror

260‧‧‧同軸視覺系統 260‧‧‧Coaxial vision system

270‧‧‧掃描頭 270‧‧‧ scan head

284‧‧‧物鏡 284‧‧‧ Objective lens

292、294‧‧‧發散角調整模組 292, 294‧‧‧ divergence angle adjustment module

P‧‧‧第一道雷射光以及第二道之間施加在工件的表面上的距離 P‧‧‧The distance between the first laser beam and the second track applied to the surface of the workpiece

D‧‧‧第一道雷射光的中心至往後數的第二個凸起結構的中心的距離 D‧‧‧The distance from the center of the first laser light to the center of the second raised structure

d1‧‧‧兩個凸起結構的距離 D1‧‧‧Distance of two raised structures

S100~S120‧‧‧步驟 S100~S120‧‧‧Steps

圖1為習知對工件表面進行表面加工而在工件表面因為熱回流產生凸起結構的示意圖。 BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a schematic view showing the surface processing of a workpiece surface to produce a convex structure on the surface of the workpiece due to heat reflow.

圖2為依據Fraunhofer ILT之技術對工件表面進行加工後工件的局部的示意圖。 Figure 2 is a schematic illustration of a portion of the workpiece after machining the surface of the workpiece in accordance with the Fraunhofer ILT technique.

圖3為本實施例表面加工方法的流程圖。 3 is a flow chart of a surface processing method of the present embodiment.

圖4為施作圖3的表面加工方法的示意圖。 4 is a schematic view of a surface processing method of FIG. 3.

圖5為一種施作此表面加工方法的雷射加工裝置的示意圖。 Fig. 5 is a schematic view of a laser processing apparatus applied to the surface processing method.

圖6為另一種施作此表面加工方法的雷射加工裝置的示意圖。 Fig. 6 is a schematic view showing another laser processing apparatus applied to the surface processing method.

圖7為又一種施作此表面加工方法的雷射加工裝置的示意圖。 Fig. 7 is a schematic view showing still another laser processing apparatus applied to the surface processing method.

圖8為工件表面上形成有週期性的凸起結構的示意圖。 Fig. 8 is a schematic view showing a periodic convex structure formed on the surface of the workpiece.

圖9為以本實施例之表面加工方法對工件施行表面加工前、僅施加第一道雷射光後以及有施加第二道雷射光之後的表面粗糙度量測結果的示意圖。 Fig. 9 is a view showing the measurement results of the surface roughness after the surface processing of the workpiece, the application of only the first laser light, and the application of the second laser light by the surface processing method of the present embodiment.

圖10為第二道雷射光的光型為高斯分布的示意圖。 Figure 10 is a schematic diagram showing the Gaussian distribution of the light pattern of the second laser light.

圖11為第二道雷射光的光型為平頂光分布的示意圖。 Figure 11 is a schematic diagram showing the light pattern of the second laser light as a flat top light distribution.

圖12為對工件施行表面加工製程時,工件表面、第一道雷射光、第二道雷射光與熔融區的示意圖。 Fig. 12 is a schematic view showing the surface of the workpiece, the first laser light, the second laser light, and the melting zone when the surface processing process is performed on the workpiece.

下面將參照所附圖式以更全面地敍述本揭露的各實施例。本揭露的各實施例也可表現為許多不同的形態,而不應理解為侷限於本文所列舉的實施例。確切地講,提供這些實施例是為 了使揭露的內容更透徹更完整,且將各實施例之概念全面傳達給所屬技術領域中具有通常知識者。在這些圖式中,為清楚起見,各層或各區域的厚度被放大。 Embodiments of the present disclosure will be described more fully hereinafter with reference to the accompanying drawings. The various embodiments of the present disclosure may also be embodied in many different forms and should not be construed as being limited to the embodiments set forth herein. Specifically, these embodiments are provided for The disclosure is made more thorough and complete, and the concepts of the various embodiments are fully conveyed to those of ordinary skill in the art. In these figures, the thickness of each layer or region is exaggerated for clarity.

容易理解的是,在整個圖式中,相同的符號代表相同的元件。本文中所用的術語“及/或”包括一個或一個以上的相關列舉項的任意及全部組合。其他用來表述各元件或各層之間關係的詞語應按相同方式來理解(例如,“介於……之間”相對於“直接介於……之間”、“與……相鄰”相對於“與……直接相鄰”、“位於……上”相對於“直接位於……上”)。 It is easy to understand that the same symbols represent the same elements throughout the drawings. The term "and/or" used herein includes any and all combinations of one or more of the associated listed. Other words used to describe the relationship between elements or layers should be understood in the same manner (for example, "between" and "directly between" and "adjacent to" "directly adjacent to", "on", as opposed to "directly on").

附帶說明的是,本文中所使用的術語如“第一”、“第二”等來敍述各元件、構件、區域、層及/或區段,但這些術語並非對這些元件、構件、區域、層及/或區段的限定。這些術語只是用來區分一個元件、構件、區域、層或區段與另一元件、構件、區域、層或區段。因此,在不脫離各實施例之教示的前提下,下文所提及的第一元件、構件、區域、層或區段也可稱為第二元件、構件、區域、層或區段。 It is to be understood that the terms "a", "a", "" The definition of layers and/or sections. These terms are only used to distinguish one element, component, region, layer or section with another element, component, region, layer or section. Thus, a first element, component, region, layer or section that is referred to hereinafter may also be referred to as a second element, component, region, layer or section, without departing from the teachings of the various embodiments.

為了便於敍述,本文會使用與空間有關的術語(如“在……下方”、“在……下面”、“下面的”、“在……上方”、“上面的”等等)來敍述如圖所示的一個元件或結構特徵相對於其他元件或結構特徵的關係。對於正在使用或正在操作的裝置或設備而言,與空間有關的術語除了包含如圖所示的方位外,也包含不同的方位。舉例而言,若將圖式中的裝置或設備翻 轉,則原本位於其他元件或結構特徵“下面”或“下方”的元件將變成位於其他元件或結構特徵的“上方”。因此,作為示範的術語“下方”可包含上方和下方這兩種方位,取決於基準點。設備也可採用其他方式定位(旋轉90度或其他方位),且按相同方式來理解本文所用的與空間有關的解說詞。 For ease of description, this article will use space-related terms (such as "below", "below", "below", "above", "above", etc.) The relationship of one element or structural feature shown in the figures to other elements or structural features. For devices or devices that are in use or in operation, space-related terms include different orientations in addition to the orientations shown. For example, if you turn the device or device in the diagram Turning, elements that are "under" or "below" other elements or structural features will become "above" the other elements or structural features. Thus, by way of example, the term "lower" can encompass both the orientations above and below, depending on the reference point. The device can also be positioned in other ways (rotated 90 degrees or other orientations) and the space-related transcripts used herein are understood in the same manner.

本文所用的術語只是為了敍述具體實施例,而非意圖限制實施例。如本文所用的單數形式“一”、“一種”及“所述”也應包括複數形式,除非文中另行明確指出。更容易理解的是,若本文使用術語“包括”及/或“包含”,則表明存在著指定的結構特徵、整體、步驟、操作、元件及/或構件,但並不排除存在或增加一個或一個以上的其他結構特徵、整體、步驟、操作、元件、構件及/或其群組。 The terminology used herein is for the purpose of describing particular embodiments, The singular forms "a", "the", and "the" It will be further understood that the use of the terms "comprises" and "comprising" or "comprises" or "comprises" or "includes" or "comprises" or "comprises" More than one other structural feature, integer, step, operation, component, component, and/or group thereof.

本文是參照各圖式來敍述本揭露的各實施例,這些圖面是各實施例的理想化實施方案(及中間結構)的示意圖。如此一來,由(例如)製造技術及/或公差而引起的圖式形狀的變動應在預料當中。因此,本揭露的各實施例不應理解為侷限於本文所述的各區域的具體形狀,而是應當包括因(例如)製造而引起的形狀偏差。因此,如圖所示的各區域本質上是示意圖,其形狀並非意圖繪示設備的區域的實際形狀,也並非意圖限制各實施例的範圍。 Embodiments of the present disclosure are described herein with reference to the drawings, which are schematic illustrations of idealized embodiments (and intermediate structures) of the various embodiments. As such, variations in the shape of the drawings caused by, for example, manufacturing techniques and/or tolerances are to be expected. Thus, the various embodiments of the present disclosure should not be construed as limited to the specific shapes of the various regions described herein, but should include the shape variations resulting from, for example, manufacturing. Therefore, the various regions in the figures are schematic and are not intended to depict the actual shapes of the regions of the device, and are not intended to limit the scope of the various embodiments.

除非另行規定,否則本文所用的全部術語(包括技術及科學術語)的含義都與本揭露之實施例所屬之技術領域中具有通 常知識者普遍理解的含義相同。更容易理解的是,如通用字典中定義的那些術語應當理解為其含義與先前技術中這些術語的含義相同,而不應理解得理想化或過於正式,除非本文有此明確規定。 Unless otherwise stated, all terms (including technical and scientific terms) used herein have the same meaning as in the technical field to which the embodiments of the present disclosure pertain. Commonly understood by people with common knowledge has the same meaning. It will be more readily understood that terms such as those defined in the general dictionary should be understood to have the same meaning as those of the prior art, and should not be construed as ideal or too formal, unless expressly stated herein.

本揭露的表面加工方法,主要是利用同一個製程中對工件提供的序列式的雷射掃描,其中第一道雷射光用以使工件的表面被熔融而形成熔融區,而因為熱回流而在熔融區中所形成的凸起結構利用第二道雷射光產生的光壓壓平熔融凸起結構,以減少工件表面因加工而引發的表面粗糙度且提升工件表面的緻密度。 The surface processing method of the present disclosure mainly utilizes a sequential laser scanning provided to a workpiece in the same process, wherein the first laser light is used to melt the surface of the workpiece to form a melting zone, and the heat is reflowed. The convex structure formed in the melting zone flattens the molten convex structure by the light pressure generated by the second laser light to reduce the surface roughness of the workpiece surface due to processing and to increase the density of the surface of the workpiece.

圖3為本實施例表面加工方法的流程圖、圖4為施作圖3的表面加工方法的示意圖,而圖5為一種施作此表面加工方法的雷射加工裝置的示意圖。請同時參考圖3、圖4及圖5,如步驟S100,提供雷射加工裝置200,所述雷射加工裝置200例如具有兩個雷射光源210與220、分別位在兩個雷射光源210與220的光路上的兩個角度可動式反射鏡240與250、設置在雷射光源220以及角度可動式反射鏡250之間的擴束器230、同軸視覺系統260、掃描頭270以及位在同軸視覺系統260以及掃描頭270之間的角度可動式反射鏡280。簡單來說,同軸視覺系統260、掃描頭270以及角度可動式反射鏡280大致排列成一直線,且角度可動式反射鏡240、250、280也大致排列成一直線,但角度可動式反射鏡240、250、280彼此之間的角度不完全相同。 3 is a flow chart of the surface processing method of the present embodiment, FIG. 4 is a schematic view of the surface processing method of FIG. 3, and FIG. 5 is a schematic view of a laser processing apparatus for applying the surface processing method. Referring to FIG. 3, FIG. 4 and FIG. 5 simultaneously, in step S100, a laser processing apparatus 200 is provided. The laser processing apparatus 200 has, for example, two laser light sources 210 and 220 respectively located at two laser light sources 210. Two angle movable mirrors 240 and 250 on the optical path of 220, a beam expander 230 disposed between the laser source 220 and the angle movable mirror 250, a coaxial vision system 260, a scanning head 270, and a coaxial An angle between the vision system 260 and the scan head 270 is a movable mirror 280. Briefly, the coaxial vision system 260, the scanning head 270, and the angular movable mirror 280 are generally arranged in a straight line, and the angular movable mirrors 240, 250, 280 are also arranged substantially in a straight line, but the angular movable mirrors 240, 250 The angles between 280 and 280 are not exactly the same.

經由上述的配置關係,雷射光源210所投出的雷射光經過角度可動式反射鏡240後反射至角度可動式反射鏡280,再經由 角度可動式反射鏡280反射至掃描頭270後,投射出去為第一道雷射光。此雷射光源210例如是連續式(Continuous Wave,CW)雷射,其所提供的第一道雷射光的光功率範圍為30~4000W,且掃描速度範圍為1~200mm/s。 Through the above arrangement relationship, the laser light emitted by the laser light source 210 is reflected by the angle movable mirror 240 and then reflected to the angle movable mirror 280, and then After the angle movable mirror 280 is reflected to the scanning head 270, it is projected as the first laser light. The laser source 210 is, for example, a continuous wave (CW) laser, which provides a first laser light having an optical power range of 30 to 4000 W and a scanning speed ranging from 1 to 200 mm/s.

雷射光源220例如為超快雷射(Ultrafast laser),其投射出的雷射光經過擴束器230射至角度可動式反射鏡250後,經由角度可動式反射鏡250反射至角度可動式反射鏡280,再經由角度可動式反射鏡280反射至掃描頭270後投射出去為第二道雷射光。此第二道雷射光的光功率範圍為0.0001~20W,且掃描速度範圍為1~200mm/s。上述的擴束器230是用來改變雷射光的光束直徑的器件,且經由擴束器230調整過的光束能夠搭配不同的光學儀器應用。以本實施例而言,雷射光源220所發射出來的雷射光經由擴束器230的調整之後變為准直(平行)的光束,且雷射光的光束的直徑可經由擴束器230依照需求設定及調整。在雷射加工裝置200的另一種實施態樣中,可以在雷射光源210以及角度可動式反射鏡240之間設置發散角調整模組292,亦在擴束器230以及角度可動式反射鏡240之間設置發散角調整模組294,如圖6示,以藉由發散角調整模組294獲得細小的高功率密度光斑。或者,可以將掃描頭270以角度可動式反射鏡282以及物鏡284的組合取代,如圖7示。在其他的應用方面,還可以在擴束器230中或是在雷射光的光束的光路上更設置空間濾波器以使非對稱光束分布變為對稱分布,使光能量分布更加均勻。雷射加工裝置200中所能夠 應用的器件是本領域所屬人員可依照需求而選用,因此不再多做舉例說明。 The laser light source 220 is, for example, an ultrafast laser, and the projected laser light is incident on the angular movable mirror 250 through the beam expander 230, and is reflected by the angle movable mirror 250 to the angle movable mirror. 280, after being reflected by the angle movable mirror 280 to the scanning head 270, is projected as a second laser light. The optical power of the second laser light ranges from 0.0001 to 20 W, and the scanning speed ranges from 1 to 200 mm/s. The beam expander 230 described above is a device for changing the beam diameter of the laser light, and the beam adjusted by the beam expander 230 can be used with different optical instrument applications. In the present embodiment, the laser light emitted by the laser light source 220 is converted into a collimated (parallel) light beam after being adjusted by the beam expander 230, and the diameter of the laser beam of the laser light can be adjusted according to the requirements of the beam expander 230. Settings and adjustments. In another embodiment of the laser processing apparatus 200, a divergence angle adjustment module 292 may be disposed between the laser source 210 and the angle movable mirror 240, also in the beam expander 230 and the angle movable mirror 240. A divergence angle adjustment module 294 is provided between them, as shown in FIG. 6, to obtain a fine high power density spot by the divergence angle adjustment module 294. Alternatively, scan head 270 can be replaced with a combination of angular movable mirror 282 and objective lens 284, as shown in FIG. In other applications, a spatial filter may be further disposed in the beam expander 230 or on the optical path of the beam of the laser light to make the asymmetric beam distribution become symmetrically distributed, so that the light energy distribution is more uniform. Capable in the laser processing apparatus 200 The device to be applied can be selected by those skilled in the art according to requirements, and therefore no more examples are given.

上述的第一道雷射光以及第二道雷射光之間沿著一方向(例如是加工方向)形成前、後順序(即第一道雷射光在前且第二道雷射光在後),並且第一道雷射光以及第二道雷射光之間相隔一段距離P。而同軸視覺系統260的設置就是用來觀察工件進行表面加工處理時工件表面的熔融狀況,以判斷第一道雷射光以及第二道之間施加在工件的表面上的距離P是否需要調整。於本實施例中,第一道雷射光與第二道雷射光先後於工件表面上到達相同的一點的時距為0-200ms之間。簡單來說,即是當工件上的某一處受到第一道雷射光照射且第一道雷射光移開之後,歷經此段時距後,第二道雷射光會照設於該處上。 The first laser light and the second laser light are formed in a front and rear sequence along a direction (for example, a processing direction) (ie, the first laser light is in front and the second laser light is behind), and The first laser light and the second laser light are separated by a distance P. The arrangement of the coaxial vision system 260 is used to observe the melting condition of the surface of the workpiece during the surface processing of the workpiece to determine whether the distance P between the first laser beam and the second track applied to the surface of the workpiece needs to be adjusted. In this embodiment, the time interval between the first laser light and the second laser light reaching the same point on the surface of the workpiece is between 0 and 200 ms. In simple terms, after a certain portion of the workpiece is irradiated with the first laser light and the first laser light is removed, after the time interval, the second laser light is illuminated there.

如步驟S110,沿著加工方向移動雷射加工裝置200,而第一道雷射光施加於工件上,工件受到第一道雷射光照射的位置會熔融,進而在工件表面上形成了熔融區,且隨著第一道雷射光的移動,熔融區內剛剛被熔融的工件材料會在第一道雷射光往前移動繼續進行加工製程的同時,因為前方的工件材料受熱被熔融而產生新的熔融區範圍,且前方被熔融的工件材料一方面因為更前方的工件材料是固體而形成阻障壁所以無法往前推移,一方面由於後方的被熔融的工件材料因為第一道雷射光的離開所以後方的被熔融的工件材料的溫度比正被第一道雷射光照射而熔融的工件材料稍低,因此基於熱往低溫流動的特性,前方被熔融的工件 材料往回流動而堆積在之前被熔融的工件材料上而形成凸起結構。因此,隨著雷射加工裝置200沿著加工方向持續移動並且施加第一道雷射光,如果不對凸起結構施行其他的步驟,凸起結構就會冷卻而凝固,因而在工件表面上形成週期性的凸起結構,如圖8示。 In step S110, the laser processing apparatus 200 is moved along the processing direction, and the first laser light is applied to the workpiece, and the position where the workpiece is irradiated with the first laser light is melted, thereby forming a melting zone on the surface of the workpiece, and As the first laser beam moves, the material of the workpiece that has just been melted in the melting zone moves forward while the first laser beam is moving forward, while the workpiece material in front is melted by heat to create a new melting zone. On the one hand, the workpiece material that is melted in the front is formed on the one hand because the workpiece material in front is solid and forms a barrier wall, so it cannot be moved forward. On the one hand, the material of the workpiece to be melted at the rear is removed because of the first laser light. The temperature of the material to be melted is slightly lower than the material of the workpiece being melted by the first laser light, so that the workpiece is melted ahead based on the characteristics of heat flowing to low temperature. The material flows back and accumulates on the previously melted workpiece material to form a raised structure. Therefore, as the laser processing apparatus 200 continues to move along the machining direction and the first laser light is applied, if no other steps are performed on the raised structure, the raised structure cools and solidifies, thereby forming a periodicity on the surface of the workpiece. The raised structure is shown in Figure 8.

特別的是,為了避免在工件表面上會形成週期性的凸起結構而導致工件表面的表面粗糙度無法達到預期,如步驟S120,因此在凸起結構凝固前,更在還呈現熔融態的凸起結構上施加強度低於第一道雷射光的強度的第二道雷射光,以藉由第二道雷射光的光壓將凸起結構壓平,如圖4示。相比於第一道雷射光施加在工件上會造成工件的表面熔融而形成熔融區,第二道雷射光的光功率範圍為0.0001~20W,明顯遠低於第一道雷射光的光功率(30~4000W之間),所以第二道雷射光並不會對還在熔融態且還未凝固的凸起結構提供熱而造成凸起結構再次熔融,而是僅對凸起結構施加光壓以將凸起結構向下壓平。圖9為以本實施例之表面加工方法對工件施行表面加工前、僅施加第一道雷射光後以及有施加第二道雷射光之後的表面粗糙度量測結果的示意圖。從圖9可以看出,工件表面還沒有被施加第一道雷射光之前,工件的表面粗糙度Ra約為450nm;而在僅施行第一道雷射光製程之後,表面粗糙度Ra降到約367nm;而施行本實施例之表面加工方法之後,工件的表面粗糙度Ra可以降到約200nm。所以,工件的表面粗糙不平的狀況有效地被抑制下來。 In particular, in order to avoid the formation of a periodic convex structure on the surface of the workpiece, the surface roughness of the surface of the workpiece cannot be expected to be as expected, as in step S120, and therefore, before the solidification of the convex structure, the convexity of the molten state is further exhibited. A second laser beam having a lower intensity than the intensity of the first laser light is applied to the structure to flatten the raised structure by the light pressure of the second laser light, as shown in FIG. Compared with the first laser light applied to the workpiece, the surface of the workpiece is melted to form a melting zone, and the optical power of the second laser light ranges from 0.0001 to 20 W, which is significantly lower than the optical power of the first laser light ( Between 30 and 4000 W), so the second laser light does not provide heat to the raised structure that is still in the molten state and has not yet solidified, causing the convex structure to melt again, but only applying light pressure to the convex structure. Flatten the raised structure down. Fig. 9 is a view showing the measurement results of the surface roughness after the surface processing of the workpiece, the application of only the first laser light, and the application of the second laser light by the surface processing method of the present embodiment. It can be seen from Fig. 9 that the surface roughness Ra of the workpiece is about 450 nm before the first laser light is applied to the surface of the workpiece; and the surface roughness Ra is reduced to about 367 nm after only the first laser light process is performed. After performing the surface processing method of the present embodiment, the surface roughness Ra of the workpiece can be lowered to about 200 nm. Therefore, the condition that the surface of the workpiece is rough is effectively suppressed.

此外,本實施例中所施加的第二道雷射光的脈衝寬度小於1奈秒。又,第二道雷射光的光型可為高斯分布(如圖10示)或平頂光分布(如圖11示),其中高斯光型的雷射光具有能量高度集中因此熱熔效應明顯的優點,而平頂光型的雷射光具有能量分布均勻以使加工特徵均勻的優點。此外,第二道雷射光的光斑直徑介於第一道雷射光的光斑直徑的0.8至1.5倍之間,但並不以此為限,所屬領域技術人員可以依照需求來調整第二道雷射光的光斑直徑。 Further, the pulse width of the second laser light applied in this embodiment is less than 1 nanosecond. Moreover, the light pattern of the second laser light may be a Gaussian distribution (as shown in FIG. 10) or a flat top light distribution (as shown in FIG. 11), wherein the Gaussian light type laser light has the advantages of high energy concentration and obvious hot melt effect. The flat top light type of laser light has the advantage of uniform energy distribution to make the processing characteristics uniform. In addition, the spot diameter of the second laser light is between 0.8 and 1.5 times the spot diameter of the first laser light, but is not limited thereto, and those skilled in the art can adjust the second laser light according to requirements. The spot diameter.

所述第二道雷射光所提供的光壓可利用Navier-Stokes方程式計算工件被熔融後熔融區內的工件材料的表面張力,然後再去找出何種雷射光的光壓能夠大於熔融區的工件材料的表面張力,以達到壓平凸起結構的功效。所利用的公式如下:2-D Navier-Stokes方程式: The light pressure provided by the second laser light can use the Navier-Stokes equation to calculate the surface tension of the workpiece material in the molten region after the workpiece is melted, and then find out which laser light has a greater light pressure than the melting region. The surface tension of the workpiece material to achieve the effect of flattening the raised structure. The formula used is as follows: 2-D Navier-Stokes equation:

其中μ為流體黏滯係數、σ為流體表面張力且ρ為固態密度。 Where μ is the fluid viscosity coefficient, σ is the fluid surface tension and ρ is the solid density.

之後,再由下列公式求得雷射光的單位面積能量為E的光線所產生的光壓,便可選定何種雷射光的光壓能大於熔融區的工件材料的表面張力。 Then, the light pressure generated by the light of the laser light per unit area E is obtained by the following formula, and the laser light energy of the laser light can be selected to be larger than the surface tension of the workpiece material in the melting zone.

p=h/λ=>p=h υ/c=>pc=E=>p=E/c p=h/λ=>p=h υ/c=>pc=E=>p=E/c

光壓F=πω0 2P Light pressure F=πω 0 2 P

表1為本實施例所選用的工件的表面張力與各種雷射所能提供的作用力(光壓)的比較表。 Table 1 is a comparison table of the surface tension of the workpiece selected for the present embodiment and the force (light pressure) that various lasers can provide.

以本實施例來說,所選用的工件的材料例如為SKD61、不鏽鋼、模具鋼等,其在受到第一道雷射光照射之後,熔融區的範圍為自所述第一道雷射光起至所述第一道雷射光之後的約800微米內的範圍內,且此熔融區的形狀呈現如尾巴拖曳的形狀(如圖12示),而第一道雷射光的中心至往後數的第二個凸起結構的中心的距離D(示於圖1),兩個凸起結構的距離約為第一道雷射光束的直徑d1(示於圖1),而第二道雷射光在與第一道雷射光距離D-d1 處(示於圖1)的熔融區中施加,其中被熔融的工件材料的表面張力約為4.397*10-4N,而從表1中可以看出奈秒雷射以及連續雷射所能提供的光壓都小於表面張力,而飛秒雷射以及皮秒雷射能提供大於表面張力的光壓,以將凸起結構壓平。 In the present embodiment, the material of the selected workpiece is, for example, SKD61, stainless steel, die steel, etc., after being irradiated by the first laser light, the melting zone ranges from the first laser light to the Within a range of about 800 microns after the first laser light, and the shape of the molten region assumes a shape like a tail drag (as shown in FIG. 12), and the center of the first laser light is second to the next. The distance D of the center of the raised structure (shown in Figure 1), the distance between the two raised structures is about the diameter d1 of the first laser beam (shown in Figure 1), and the second laser is in the same A laser beam is applied in the melting zone at D-d1 (shown in Figure 1), wherein the surface tension of the molten workpiece material is about 4.397*10 -4 N, and the nanosecond mine can be seen from Table 1. Both the shot and the continuous laser provide less light pressure than the surface tension, while femtosecond lasers and picosecond lasers provide a light pressure greater than the surface tension to flatten the raised structure.

此外,第二道雷射光的能量需小於工件的剝除閥值,以避免在對工件施加第二道雷射光的時候,第二道雷射光的能量強到足以使工件受到加工處理的部分剝落。工件的剝除閥值會隨著工件的材質而不同,因此第二道雷射光的能量也可以隨著工件的材質不同而改變;當然,第一道雷射光的能量也會隨著工件的材質不同而調整。 In addition, the energy of the second laser light needs to be smaller than the stripping threshold of the workpiece to avoid that when the second laser light is applied to the workpiece, the energy of the second laser light is strong enough to cause the workpiece to be partially peeled off. . The stripping threshold of the workpiece will vary with the material of the workpiece, so the energy of the second laser can also vary with the material of the workpiece; of course, the energy of the first laser will also vary with the material of the workpiece. Different adjustments.

利用本揭露的表面加工方法對工件進行表面加工與利用傳統雷射拋光的不同之處在於變質層的厚度不同,利用本揭露的表面加工方法進行加工的工件的變質層較薄,改善了表面凸起結構的問題,且結構緻密度較佳。而與以Fraunhofer ILT的方式進行加工比較,以Fraunhofer ILT的方式進行加工的工件會產生兩層厚度不同之熔融層,變質層的厚度較厚,緻密度也較差,且表面仍具有凸起結構,因此表面粗糙度也無法有效地降低。此外,Fraunhofer ILT的技術因為是在第一道雷射光先對工件表面進行全面性的照射之後,再施行第二道雷射光照射,所以須要花費比一般單道次雷射拋光雙倍的時間,增加許多額外的成本。 The surface processing of the workpiece by the surface processing method of the present disclosure differs from the conventional laser polishing in that the thickness of the altered layer is different, and the modified layer of the workpiece processed by the surface processing method of the present invention is thinner, and the surface convex is improved. The structure is problematic and the structure density is better. Compared with the method of Fraunhofer ILT, the workpiece processed by Fraunhofer ILT will produce two layers of different thicknesses. The thickness of the metamorphic layer is thicker, the density is also poor, and the surface still has a convex structure. Therefore, the surface roughness cannot be effectively reduced. In addition, Fraunhofer ILT's technology is based on the first laser light after the first laser beam is applied to the surface of the workpiece, and then the second laser light is irradiated, so it takes twice as long as the general single-pass laser polishing. Add a lot of extra cost.

相比之下,本揭露的表面加工方法是以序列的方式讓兩道雷射光在同一道製程中施作,即第一道雷射光照射之後,第二 道雷射光在適當的時距後隨即對熔融區中未凝固的凸起結構施行,所以雷射光施行的加工時間較Fraunhofer ILT的技術更短,進而提升雷射加工裝置在一定時間內可以施作的工件的數量。而經由本揭露的表面加工方法所形成的工件的表面的結構平坦度提升、變質層薄且緻密度高,因此加工後的表面的硬度與耐磨度都隨著提升。 In contrast, the surface processing method of the present disclosure is to sequentially apply two laser beams in the same process, that is, after the first laser light irradiation, the second The ray light is applied to the unsolidified convex structure in the melting zone immediately after the appropriate time interval, so the processing time of the laser light is shorter than that of the Fraunhofer ILT, and the laser processing device can be applied for a certain period of time. The number of artifacts. On the other hand, the surface flatness of the surface formed by the surface processing method disclosed by the present invention is improved, the metamorphic layer is thin, and the density is high, so that the hardness and wear resistance of the surface after processing are improved.

再者,施行此表面加工方法的雷射加工裝置的元件設置簡單,而該領域人員可以在不須大幅調整或變動舊有的加工光路的情況下依照需求挑選適用的器件來對雷射加工裝置進行升級,有效控制雷射加工裝置的升級花費。 Furthermore, the components of the laser processing apparatus for performing the surface processing method are simple to set up, and the field personnel can select suitable devices for the laser processing apparatus according to requirements without greatly adjusting or changing the old processing optical path. Upgrade to effectively control the upgrade cost of the laser processing unit.

雖然本發明已以實施例揭露如上,然其並非用以限定本發明,任何所屬技術領域中具有通常知識者,在不脫離本發明的精神和範圍內,當可作些許的更動與潤飾,故本發明的保護範圍當視後附的申請專利範圍所界定者為準。 Although the present invention has been disclosed in the above embodiments, it is not intended to limit the present invention, and any one of ordinary skill in the art can make some changes and refinements without departing from the spirit and scope of the present invention. The scope of the invention is defined by the scope of the appended claims.

S100~S120‧‧‧步驟 S100~S120‧‧‧Steps

Claims (8)

一種表面加工方法,包括:提供雷射加工裝置,所述雷射加工裝置用以提供相隔一段可調變距離的第一道雷射光以及第二道雷射光;沿著加工方向移動所述雷射加工裝置,其中所述雷射加工裝置提供所述第一道雷射光施加於工件上,所述工件受到所述第一道雷射光照射處熔融以形成熔融區,且隨著所述第一道雷射光的移動,所述熔融區內的工件材料熱回流並形成凸起結構;以及在所述凸起結構凝固前,所述雷射加工裝置在所述第一道雷射光沿著加工方向繼續向前移動之後提供第二道雷射光施加於所述凸起結構上,其中所述第二道雷射光的強度低於所述第一道雷射光的強度,以藉由所述第二道雷射光的光壓將所述凸起結構壓平。 A surface processing method comprising: providing a laser processing apparatus for providing a first laser light and a second laser light separated by a variable variable distance; moving the laser along a machining direction a processing apparatus, wherein the laser processing apparatus provides the first laser light to be applied to a workpiece, the workpiece being melted by the first laser light to form a melting zone, and along with the first track Movement of the laser light, the workpiece material in the molten region is thermally reflowed and forms a raised structure; and the laser processing apparatus continues the first laser light along the processing direction before the raised structure solidifies Providing a second laser light applied to the raised structure after moving forward, wherein the intensity of the second laser light is lower than the intensity of the first laser light to The light pressure of the light illuminates the raised structure. 如申請專利範圍第1項所述的表面加工方法,其中所述第一道雷射光的光功率範圍為30~4000W,且掃描速度範圍為1~200mm/s,而所述第二道雷射光的光功率範圍為0.0001~20W,且掃描速度範圍為1~200mm/s。 The surface processing method according to claim 1, wherein the first laser light has an optical power range of 30 to 4000 W, and a scanning speed ranges from 1 to 200 mm/s, and the second laser light The optical power range is 0.0001~20W, and the scanning speed ranges from 1~200mm/s. 如申請專利範圍第1項所述的表面加工方法,其中所述第一道雷射光與所述第二道雷射光先後通過所述工件上相同的一點的時距介於0~200ms之間。 The surface processing method according to claim 1, wherein the time interval between the first laser light and the second laser light passing through the same point on the workpiece is between 0 and 200 ms. 如申請專利範圍第1項所述的表面加工方法,其中沿著所述第一道雷射光的掃描軌跡,所述熔融區的定義是所述工件材料 升溫至熔點以上的區域。 The surface processing method according to claim 1, wherein the melting zone is defined as the workpiece material along a scanning trajectory of the first laser light. Warm up to a region above the melting point. 如申請專利範圍第1項所述的表面加工方法,其中所述第二道雷射光的脈衝寬度小於1奈秒。 The surface processing method of claim 1, wherein the second laser light has a pulse width of less than 1 nanosecond. 如申請專利範圍第1項所述的表面加工方法,其中所述第二道雷射光的能量小於工件的剝除閥值。 The surface processing method of claim 1, wherein the energy of the second laser light is less than a stripping threshold of the workpiece. 如申請專利範圍第1項所述的表面加工方法,其中所述第二道雷射光的光斑直徑介於第一道雷射光的光斑直徑的0.8至1.5倍之間。 The surface processing method according to claim 1, wherein the spot diameter of the second laser light is between 0.8 and 1.5 times the spot diameter of the first laser light. 如申請專利範圍第1項所述的表面加工方法,其中所述第二道雷射光的光型為高斯分布或平頂光分布。 The surface processing method according to claim 1, wherein the second laser light has a Gaussian distribution or a flat top light distribution.
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