• 대한수학회논문집
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• 제35권1호
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• pp.321-338
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• 2020

In this paper, we investigate the viscoelastic plate equation with a constant delay term and logarithmic nonlinearities. Under some conditions, we will prove the global existence. Furthermore, we use weighted spaces to establish a general decay rate of solution.

• 한국정밀공학회:학술대회논문집
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• 한국정밀공학회 2008년도 춘계학술대회 논문집
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• pp.355-356
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• 2008

• 한국섬유공학회:학술대회논문집
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• 한국섬유공학회 1994년도 춘계학술발표회 프로그램 및 초록
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• pp.78-79
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• 1994

• 대한토목학회논문집
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• 제30권3A호
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• pp.221-228
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• 2010

탄소섬유시트 보강공법은 열화 손상된 콘크리트 구조물의 보강에 가장 많이 사용되는 보강공법 중 하나이다. 탄소섬유시트 보강공법은 에폭시접착제를 사용하여 탄소섬유시트를 콘크리트의 외부에 부착하는 보강공법으로 탄소섬유시트에 의한 휨보강이 에폭시 접착 경계면을 통하여 콘크리트로 전달된다. 따라서 사용기간이 경과함에 따라 에폭시 접착 경계면에 발생하는 크리프 등의 시간의존적 거동은 보강효과를 감소시키는 요인이 된다. 본 연구에서는 경계면에서 발생하는 크리프 영향을 해석하기 위하여 콘크리트의 크리프 거동에 대한 기존의 연구들을 고찰하고, 이를 바탕으로 에폭시 접착 경계면의 크리프 영향을 예측할 수 있는 이론적인 연구를 수행하였다. 제안된 유한요소해석기법은 기존의 콘크리트 크리프 거동 분석을 위해 사용되던 유변모델을 에폭시 접착 경계면에 적용한 것으로 기존 실험결과와 비교를 통하여 타당성을 검증하였다. 또한, 제안된 유한요소해석을 통하여 탄소섬유시트로 보강된 콘크리트 구조물의 시간의존적 거동에 경계면 재료의 크리프 영향을 반드시 고려해야 한다는 것을 입증하였다.

• 한국유변학회:학술대회논문집
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• 한국유변학회 2006년도 춘계 학술발표회 논문집
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• pp.143-147
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• 2006

• 폴리머
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• 제39권3호
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• pp.475-479
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• 2015

모폴로지 분석을 통하여 반복압출에 의한 LCP(Vectra A950)와 PET 블렌드의 droplet 분산 상태를 확인하였다. 반복압출은 블렌드 조건별로 각각 2회, 3회 진행하였으며, 1회 압출 시료의 droplet 분산은 균일한 형태를 보였다. 하지만, 2회 및 3회 반복 압출 시료의 droplet 크기는 증가하였고 droplet이 시료의 중앙에 집중되는 현상을 확인할 수 있었다. 이러한 현상은 LCP/PET 블렌드의 상용성과 점탄성 거동에 기인한 것으로 생각된다. 끝으로 동일 방사조건에서 반복압출 LCP/PET 블렌드 chip을 방사하면 직경이 다른 섬유 제조가 가능할 것으로 생각된다.

• 한국소음진동공학회논문집
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• 제22권1호
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• pp.53-60
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• 2012

To reduce the vibration in industrial settings, the viscous fluid dampers have been widely used. Since the damper shows a viscoelastic behavior, many methods to predict the behavior have been investigated. But the methods did not consider a change of damper size that is important factor for practical design engineer. In this study, to predict a change of damper ability with respect to a change of damper size, the dynamic experiment were conducted with fixed aspect ratio and gap. The damping coefficient at zero frequency was computed through theoretical and experiment approach in order to fit the experimental results using fractional derivative Maxwell model.

• Journal of Pharmaceutical Investigation
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• 제33권1호
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• pp.15-19
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• 2003

The rheological behavior of poloxamer 407 solution as function of concentration and temperature was evaluated by rotational viscometer. The viscosity of poloxamer 407 solution was increased as the concentration of poloxamer 407 and temperature increased. At $4^{\circ}C$, poloxamer 407 solution showed the Newtonian flow characteristics regardless of concentration. Upon increasing temperature the poloxamer solution changed to the pseudoplastic flow pattern. And at gelation temperature, rheological profiles showed the abrupt increase in viscosity. Gelation temperature was decreased as the concentration of poloxamer 407 increased, while it increased as the concentration of poly(ethylene glycol) 4000 increased. Poly(ethylene glycol) might be expected to reduce the driving force for hydrophobic interaction resulting in slow gelation. From the viscoelastic properties of poloxamer gel system, we obtained the storage and loss modulus depending on the shear stress and frequency. And the sol-gel transition temperature was also obtained from the viscoelastic properties of poloxamer 407 gel.

• 한국전기전자재료학회논문지
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• 제18권4호
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• pp.313-320
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• 2005

Stick-slip friction is one of the material removal mechanisms in tribology. It occurs when the static friction force is larger than the dynamic friction force, and make the friction curve fluctuated. In the friction monitoring of chemical mechanical polishing(CMP), the friction force also vibrates just as stick-slip friction. In this paper, an attempt to show the similarity between stick-slip friction and the friction of CMP was conducted. The prepared hard pa(IC1000/Suba400 stacked/sup TM/) and soft pad(Suba400/sup TM/) were tested with SiO₂ slurry. The friction force was measured by piezoelectric sensor. According to this experiment, it was shown that as the head and table velocity became faster, the stick-slip time shortened because of the change of real contact area. And, the gradient of stick-slip period as a function of head and table speed in soft pad was more precipitous than that of hard one. From these results, it seems that the fluctuating friction force in CMP is stick-slip friction caused by viscoelastic behavior of the pad and the change of real contact area.

• Korea-Australia Rheology Journal
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• 제21권1호
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• pp.47-58
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• 2009

We have investigated the transient behavior of 1D fully developed Poiseuille viscoelastic flow under finite pressure gradient described by the Oldroyd-B and Leonov constitutive equations. For analysis we employ a simple $2^{nd}$ order discretization scheme such as central difference for space and the Crank-Nicolson for time approximation. For the analysis of the Oldroyd-B model, we also apply the analytical solution, which is obtained again in this work in terms of elementary solution procedure simpler than the previous one (Waters and King, 1970). Both models demonstrate qualitatively similar solutions, but their eventual steady flowrate exhibits noticeable difference due to the absence or presence of shear thinning behavior. In the inertialess flow, the flowrate instantaneously attains a large value corresponding to the Newtonian creeping flow and then decreases to its steady value when the applied pressure gradient is low. However with finite liquid density the flow field shows severe fluctuation even accompanying reversals of flow directions. As the assigned pressure gradient increases, the flowrate achieves its steady value significantly higher than its value during oscillations after quite long period of time. We have also illustrated comparison between 1D and 2D results and possible mechanism of complex 2D flow rearrangement employing a previous solution of [mite element computation. In addition, we discuss some mathematical points regarding missing boundary conditions in 2D modeling due to the change of the type of differential equations when varying from inertialess to inertial flow.