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    Multi-scale friction modeling for manufacturing processes: The boundary layer regime

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    This paper presents a multi-scale friction model for largescale forming simulations. A friction framework has been developed including the effect of surface changes due to normal loading and straining the underlying bulk material. A fast and efficient translation from micro to macro modeling, based on stochastic methods, is incorporated to reduce the computational effort. Adhesion and ploughing effects have been accounted for to characterize friction conditions on the micro scale. A discrete model has been adopted which accounts for the formation of contact patches ploughing through the contacting material. To simulate metal forming processes a coupling has been made with an implicit Finite Element code. Simulations on a typical metal formed product shows a distribution of friction values. The modest increase in simulation time, compared to a standard Coulomb-based FE simulation, proves the numerical feasibility of the proposed method

    ์ž๋™์ฐจ์šฉ ํŒ์žฌ์„ฑํ˜• ํ•ด์„ ์ ์šฉ์„ ์œ„ํ•œ ๋‹ค์ค‘ ์Šค์ผ€์ผ ๋งˆ์ฐฐ ๋ชจ๋ธ ๊ฐœ๋ฐœ ๋ฐ ํ‰๊ฐ€

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์žฌ๋ฃŒ๊ณตํ•™๋ถ€, 2022.2. ์ด๋ช…๊ทœ.Sheet metal forming of advanced high strength steels (AHSS) has drawn significant attentions in automotive industry for their improved fuel efficiency by lightweightness and passenger safety by higher strength. However, the manufacturing of automotive parts with the AHSS accompanies inferior springback and formability compared to the conventional lower strength steels, which results in more time consuming trial and error in the tool design stage. To overcome this challenges in applying the AHSS to the automotive parts, finite element simulations have been commonly used as a numerical tool for predicting springback and formability of sheet metal parts prior to real try-out. Accurate modeling of finite element simulation in sheet metal forming process requires reliable numerical techniques, constitutive models, realistic boundary conditions, etc. Among these, the friction is one of important factors to determine the accuracy of the simulation, but it has been overlooked in most simulations. The frictional behavior in sheet metal forming is known to be very complex and depend on various parameters such as surface roughness, contact pressure, sliding velocity, lubrication condition, etc. However, it is a common practice to use the simplest Coulomb friction law in the finite element modeling. In the present study, a microscale asperity based friction model is further modified by imposing new model parameters for satisfying force equilibrium between contact surfaces. In addition, a geometrical shape model of the tool surface is newly proposed to determine the plowing effect of the friction. The tool geometry is modeled based on primary summits in tool height distribution determined by the measured wavelength, rather than the summits dependent on the resolution of surface measurement instrument. The friction models are required not only in the preceding boundary lubrication condition, but also in the mixed-boundary lubrication condition where sufficient lubrication exists in non-contacting surface valleys. The hydrodynamic friction model uses a load-sharing concept that considers the lubrication area and metal-to-metal contact separately. In this study, the hydrodynamic friction model is combined with the boundary lubrication friction model to account for the friction in the mixed lubrication domain. The lubricant film thickness, calculated as the volume of non-contacting surface valleys, is used to realize the coupling. The film lubrication behavior is implemented by the finite element coding of the Reynolds equation, which enables the calculation of the hydrodynamic pressure. To validate the boundary lubrication friction model, the calculated friction coefficient and the measured friction coefficient are compared according to the contact pressure under boundary lubrication conditions. Also, the boundary lubrication friction model is verified by the finite element simulation that is applied to the U-draw/bending process. Finally, the boundary lubrication friction model and the mixed boundary lubrication friction model are applied to the finite element simulation of the newly developed press-forming process, which represents the influence of various variables such as contact pressure, sliding speed and lubrication. The results of the validations show that the developed multi-scale friction models and their implementation can be efficiently used to the sheet metal forming simulations where the frictional behavior is critical for the quality of the automotive parts.AHSS(๊ณ ์žฅ๋ ฅ๊ฐ•ํŒ)์˜ ํŒ๊ธˆ ์„ฑํ˜•์€ ๊ฒฝ๋Ÿ‰ํ™”์— ์˜ํ•œ ์—ฐ๋น„ ํ–ฅ์ƒ๊ณผ ๊ณ ๊ฐ•๋„ํ™”์— ์˜ํ•œ ์Šน๊ฐ ์•ˆ์ „์œผ๋กœ ์ž๋™์ฐจ ์‚ฐ์—…์—์„œ ํฐ ์ฃผ๋ชฉ์„ ๋ฐ›๊ณ  ์žˆ์Šต๋‹ˆ๋‹ค. ๊ทธ๋Ÿฌ๋‚˜ AHSS๋ฅผ ์ด์šฉํ•œ ์ž๋™์ฐจ ๋ถ€ํ’ˆ ์ œ์กฐ๋Š” ๊ธฐ์กด์˜ ์ €๊ฐ•๋„ ๊ฐ•์žฌ์— ๋น„ํ•ด ์Šคํ”„๋ง๋ฐฑ ๋ฐ ์„ฑํ˜•์„ฑ์ด ์ข‹์ง€์•Š๊ธฐ์— ํˆด ์„ค๊ณ„ ๋‹จ๊ณ„์—์„œ ์‹œํ–‰์ฐฉ์˜ค๊ฐ€ ๋” ๋งŽ์ด ๋ฐœ์ƒํ•˜๊ฒŒ ๋ฉ๋‹ˆ๋‹ค. ์ž๋™์ฐจ ๋ถ€ํ’ˆ์— AHSS๋ฅผ ์ ์šฉํ•  ๋•Œ ์ด๋Ÿฌํ•œ ๋ฌธ์ œ๋ฅผ ๊ทน๋ณตํ•˜๊ธฐ ์œ„ํ•ด ์œ ํ•œ ์š”์†Œ ์‹œ๋ฎฌ๋ ˆ์ด์…˜์€ ์‹ค์ œ ์‹œํ—˜ ์ „์— ํŒ์žฌ ์„ฑํ˜• ๋ถ€ํ’ˆ์˜ ์Šคํ”„๋ง๋ฐฑ ๋ฐ ์„ฑํ˜•์„ฑ์„ ์˜ˆ์ธกํ•˜๊ธฐ ์œ„ํ•œ ์ˆ˜์น˜ํ•ด์„์  ๋„๊ตฌ๋กœ ์ผ๋ฐ˜์ ์œผ๋กœ ์‚ฌ์šฉ๋˜์—ˆ์Šต๋‹ˆ๋‹ค. ํŒ์žฌ ์„ฑํ˜• ๊ณต์ •์—์„œ ์œ ํ•œ ์š”์†Œ ์‹œ๋ฎฌ๋ ˆ์ด์…˜์˜ ์ •ํ™•ํ•œ ๋ชจ๋ธ๋ง์€ ์‹ ๋ขฐํ•  ์ˆ˜ ์žˆ๋Š” ์ˆ˜์น˜ํ•ด์„์  ๊ธฐ์ˆ , ๊ตฌ์„ฑ ๋ฐฉ์ •์‹, ์ •ํ™•ํ•œ ๊ฒฝ๊ณ„ ์กฐ๊ฑด ๋“ฑ์ด ํ•„์š”ํ•ฉ๋‹ˆ๋‹ค. ์ด ์ค‘ ๋งˆ์ฐฐ์€ ์‹œ๋ฎฌ๋ ˆ์ด์…˜์˜ ์ •ํ™•๋„๋ฅผ ๊ฒฐ์ •ํ•˜๋Š” ์ค‘์š”ํ•œ ์š”์†Œ ์ค‘ ํ•˜๋‚˜์ด์ง€๋งŒ ๋Œ€๋ถ€๋ถ„์˜ ์‹œ๋ฎฌ๋ ˆ์ด์…˜์—์„œ ๊ฐ„๊ณผ๋˜์–ด ์™”์Šต๋‹ˆ๋‹ค. ํŒ์žฌ ์„ฑํ˜•์—์„œ ๋งˆ์ฐฐ ๊ฑฐ๋™์€ ๋งค์šฐ ๋ณต์žกํ•˜๊ณ  ํ‘œ๋ฉด ๊ฑฐ์น ๊ธฐ, ์ ‘์ด‰ ์••๋ ฅ, ๋ฏธ๋„๋Ÿผ ์†๋„, ์œคํ™œ ์กฐ๊ฑด ๋“ฑ๊ณผ ๊ฐ™์€ ๋‹ค์–‘ํ•œ ๋งค๊ฐœ๋ณ€์ˆ˜์— ๋”ฐ๋ผ ๋‹ฌ๋ผ์ง€๋Š” ๊ฒƒ์œผ๋กœ ์•Œ๋ ค์ ธ ์žˆ์Šต๋‹ˆ๋‹ค. ๊ทธ๋Ÿฌ๋‚˜, ๋Œ€๋ถ€๋ถ„์˜ ์œ ํ•œ ์š”์†Œ ํ•ด์„์—์„œ ๊ฐ€์žฅ ๊ฐ„๋‹จํ•œ ์ฟจ๋กฑ ๋งˆ์ฐฐ ๋ฒ•์น™์„ ์‚ฌ์šฉํ•˜๋Š” ๊ฒƒ์ด ์ผ๋ฐ˜์ ์ž…๋‹ˆ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์ ‘์ด‰๋ฉด ์‚ฌ์ด์˜ ํž˜ ํ‰ํ˜•์„ ๋งŒ์กฑ์‹œํ‚ค๊ธฐ ์œ„ํ•ด ์ƒˆ๋กœ์šด ๋ชจ๋ธ ๋งค๊ฐœ๋ณ€์ˆ˜๋ฅผ ๋ถ€๊ณผํ•˜์—ฌ ๋งˆ์ดํฌ๋กœ ์Šค์ผ€์ผ ๋Œ๊ธฐ ๊ธฐ๋ฐ˜ ๋งˆ์ฐฐ ๋ชจ๋ธ์„ ์ถ”๊ฐ€๋กœ ์ˆ˜์ •ํ–ˆ์Šต๋‹ˆ๋‹ค. ๋˜ํ•œ ๋งˆ์ฐฐ์˜ ์Ÿ๊ธฐ์งˆ ํšจ๊ณผ๋ฅผ ๊ฒฐ์ •ํ•˜๊ธฐ ์œ„ํ•ด ํˆด ํ‘œ๋ฉด์˜ ๊ธฐํ•˜ํ•™์  ํ˜•์ƒ ๋ชจ๋ธ์ด ์ƒˆ๋กœ ์ œ์•ˆ๋˜์—ˆ์Šต๋‹ˆ๋‹ค. ํˆด ํ˜•์ƒ์€ ํ‘œ๋ฉด ์ธก์ • ์žฅ๋น„์˜ ๋ถ„ํ•ด๋Šฅ์— ์˜์กดํ•˜๋Š” ์ •์ ์ด ์•„๋‹ˆ๋ผ ์ธก์ •๋œ ํŒŒ์žฅ์— ์˜ํ•ด ๊ฒฐ์ •๋˜๋Š” ํˆดํ‘œ๋ฉด ๋†’์ด ์กฐ๋„์˜ ์„œ๋ฐ‹์„ ๊ธฐ๋ฐ˜์œผ๋กœ ๋ชจ๋ธ๋ง๋ฉ๋‹ˆ๋‹ค. ๋งˆ์ฐฐ๋ชจ๋ธ์€ ๊ฒฝ๊ณ„์œคํ™œ์กฐ๊ฑด๋ฟ๋งŒ ์•„๋‹ˆ๋ผ ์ถฉ๋ถ„ํ•œ ์œคํ™œ์ด ์กด์žฌํ•˜๋Š” ํ˜ผํ•ฉ๊ฒฝ๊ณ„์œคํ™œ์กฐ๊ฑด์—์„œ๋„ ํ•„์š”ํ•˜๋‹ค. ์œ ์ฒด์—ญํ•™์  ๋งˆ์ฐฐ ๋ชจ๋ธ์€ ์œคํ™œ ์˜์—ญ๊ณผ ๊ธˆ์† ๋Œ€ ๊ธˆ์† ์ ‘์ด‰์„ ๋ณ„๋„๋กœ ๊ณ ๋ คํ•˜๋Š” ํ•˜์ค‘ ๊ณต์œ  ๊ฐœ๋…์„ ์‚ฌ์šฉํ•ฉ๋‹ˆ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์œ ์ฒด์—ญํ•™์  ๋งˆ์ฐฐ ๋ชจ๋ธ์„ ๊ฒฝ๊ณ„ ์œคํ™œ ๋งˆ์ฐฐ ๋ชจ๋ธ๊ณผ ๊ฒฐํ•ฉํ•˜์—ฌ ํ˜ผํ•ฉ ์œคํ™œ ์˜์—ญ์˜ ๋งˆ์ฐฐ์„ ์„ค๋ช…ํ•ฉ๋‹ˆ๋‹ค. ๋น„์ ‘์ด‰ ํ‘œ๋ฉด ๋ฐธ๋ฆฌ์˜ ๋ถ€ํ”ผ๋กœ ๊ณ„์‚ฐ๋œ ์œคํ™œ์œ  ํ•„๋ฆ„ ๋‘๊ป˜๋Š” ์ปคํ”Œ๋ง์„ ๊ตฌํ˜„ํ•˜๋Š” ๋ฐ ์‚ฌ์šฉ๋ฉ๋‹ˆ๋‹ค. ํ•„๋ฆ„ ์œคํ™œ ๊ฑฐ๋™์€ ์œ ์ฒด์—ญํ•™์  ์••๋ ฅ์˜ ๊ณ„์‚ฐ์„ ๊ฐ€๋Šฅํ•˜๊ฒŒ ํ•˜๋Š” Reynolds ๋ฐฉ์ •์‹์˜ ์œ ํ•œ ์š”์†Œ ๋ฐฉ๋ฒ•์„ ์‚ฌ์šฉํ•ด ๊ตฌํ˜„๋ฉ๋‹ˆ๋‹ค. ๊ฒฝ๊ณ„ ์œคํ™œ ๋งˆ์ฐฐ ๋ชจ๋ธ์„ ๊ฒ€์ฆํ•˜๊ธฐ ์œ„ํ•ด ๊ฒฝ๊ณ„ ์œคํ™œ ์กฐ๊ฑด์—์„œ ์ ‘์ด‰ ์••๋ ฅ์— ๋”ฐ๋ผ ๊ณ„์‚ฐ๋œ ๋งˆ์ฐฐ ๊ณ„์ˆ˜์™€ ์ธก์ •๋œ ๋งˆ์ฐฐ ๊ณ„์ˆ˜๋ฅผ ๋น„๊ตํ•ฉ๋‹ˆ๋‹ค. ๋˜ํ•œ ๊ฒฝ๊ณ„ ์œคํ™œ ๋งˆ์ฐฐ ๋ชจ๋ธ์€ U-draw/bending ๊ณผ์ •์— ์ ์šฉ๋œ ์œ ํ•œ ์š”์†Œ ์‹œ๋ฎฌ๋ ˆ์ด์…˜์„ ํ†ตํ•ด ๊ฒ€์ฆ๋˜์—ˆ์Šต๋‹ˆ๋‹ค. ๋งˆ์ง€๋ง‰์œผ๋กœ ๊ฒฝ๊ณ„ ์œคํ™œ ๋งˆ์ฐฐ ๋ชจ๋ธ๊ณผ ํ˜ผํ•ฉ ๊ฒฝ๊ณ„ ์œคํ™œ ๋งˆ์ฐฐ ๋ชจ๋ธ์„ ์ƒˆ๋กœ ๊ฐœ๋ฐœ๋œ ํ”„๋ ˆ์Šค ์„ฑํ˜• ๊ณต์ •์˜ ์œ ํ•œ ์š”์†Œ ์‹œ๋ฎฌ๋ ˆ์ด์…˜์— ์ ์šฉํ–ˆ๋Š”๋ฐ, ์ด๋Š” ์ ‘์ด‰ ์••๋ ฅ, ๋ฏธ๋„๋Ÿผ ์†๋„ ๋ฐ ์œคํ™œ๊ณผ ๊ฐ™์€ ๋‹ค์–‘ํ•œ ๋ณ€์ˆ˜์˜ ์˜ํ–ฅ์„ ๋‚˜ํƒ€๋ƒ…๋‹ˆ๋‹ค. ๊ฒ€์ฆ ๊ฒฐ๊ณผ๋Š” ๊ฐœ๋ฐœ๋œ ๋‹ค์ค‘ ์Šค์ผ€์ผ ๋งˆ์ฐฐ ๋ชจ๋ธ๊ณผ ๊ทธ ๊ตฌํ˜„์ด ๋งˆ์ฐฐ ๊ฑฐ๋™์ด ์ž๋™์ฐจ ๋ถ€ํ’ˆ ํ’ˆ์งˆ์— ์ค‘์š”ํ•œ ํŒ์žฌ ์„ฑํ˜• ์‹œ๋ฎฌ๋ ˆ์ด์…˜์— ํšจ์œจ์ ์œผ๋กœ ์‚ฌ์šฉ๋  ์ˆ˜ ์žˆ์Œ์„ ๋ณด์—ฌ์ค๋‹ˆ๋‹ค.1. Introduction 1 1.1. Sheet metal forming and deep drawing process 1 1.2. Motivation and objective 2 1.3. Literature review 5 1.3.1. Friction modeling on the boundary lubrication condition 6 1.3.2. Friction modeling on the mixed-boundary lubrication condition 22 2. Friction model in boundary lubrication 35 2.1. Framework of friction model in boundary lubrication 35 2.2. Statistical contact model for describing surface deformation 38 2.2.1. Assumptions for modeling 39 2.2.2. Flattening of workpiece asperity due to normal load 41 2.2.3. Flattening of workpiece asperity due to normal load and sliding 48 2.2.4. Flattening of workpiece asperity due to normal load and bulk strain 50 2.3. Friction model through a new approach 53 2.3.1. An elliptical paraboloid asperity model 53 2.3.2. A tool geometry model 56 3. Friction model in mixed-boundary lubrication 65 3.1. Overview of the mixed-boundary friction model (Hol [106]) 67 3.2. Finite element modeling for film fluid behavior 71 3.3. Verification of the developed finite element modeling 75 4. Application of boundary lubrication and mixed-boundary lubrication friction model to sheet metal forming process 82 4.1. Friction model parameters 82 4.1.1. Material properties 82 4.1.2. Surface data 83 4.1.3. Friction experiments 86 4.2. Application to sheet metal forming processes under non-lubrication conditions 91 4.2.1. Application to U-draw/bending simulation 94 4.2.2. Application to prototype press-forming process without lubricant 105 4.3. Application to sheet metal forming processes under lubrication conditions 116 5. Conclusions 129 Reference 134๋ฐ•

    Numerical Simulation in Microforming for Very Small Metal Elements

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    Microforming is a technology of very small metal elements production, which are required as a parts for many industrial products resulting from microtechnology. This chapter gives a review of the state-of-the-art microforming of metals and its numerical simulations. Phenomena occurring in the miniaturization of microbulk-forming technologies are described. The main problems in microforming are size effects, which have physical and structural sources and directly affect the material flow mechanics in microscale. Size effects must be taken into account in all areas of the forming process chain, demanding new solutions, especially in workpiece structure and die surface numerical modeling

    Advanced friction modeling in sheet metal forming

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    The Coulomb friction model is frequently used for sheet metal forming simulations. This model incorporates a constant coefficient of friction and does not take the influence of important parameters such as contact pressure or deformation of the sheet material into account. This article presents a more advanced friction model for large-scale forming simulations based on the surface changes on the micro-scale. When two surfaces are in contact, the surface texture of a material changes due to the combination of normal loading and stretching. Consequently, shear stresses between contacting surfaces, caused by the adhesion and ploughing effect between contacting asperities, will change when the surface texture changes. A friction model has been developed which accounts for these microscopic dependencies and its influence on the friction behavior on the macro-scale. The friction model has been validated by means of finite element simulations on the micro-scale and has been implemented in a finite element code to run large scale sheet metal forming simulations. Results showed a realistic distribution of the coefficient of friction depending on the local process conditions
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