Cheng-fu Chen

Dr. Cheng-fu Chen

Department of Mechanical Engineering, University of Alaska Fairbanks, Fairbanks, Alaska, USA
orcid

Research Focus & Metrics

Academic Career Length

27Years (2000-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 June 2012 in Applied Surface Science
Verified
Journal Article
Closed access
YGYanhong Gu
Yanhong Gu
Cheng-fu ChenCheng-fu Chen
Cheng-fu Chen
SBSukumar Bandopadhyay
Sukumar Bandopadhyay
CNChengyun Ning
Chengyun Ning
YZYongjun Zhang
Yongjun Zhang
YGYuanjun Guo
Yuanjun Guo

1 December 2012 in Journal of Alloys and Compounds
Verified
Journal Article
Closed access
YGYanhong Gu
Yanhong Gu
SBSukumar Bandopadhyay
Sukumar Bandopadhyay
Cheng-fu ChenCheng-fu Chen
Cheng-fu Chen
YGYuanjun Guo
Yuanjun Guo
CNChengyun Ning
Chengyun Ning

1 April 2013 in Materials & Design (1980-2015)
Verified
Journal Article
Closed access
YGYanhong Gu
Yanhong Gu
SBSukumar Bandopadhyay
Sukumar Bandopadhyay
Cheng-fu ChenCheng-fu Chen
Cheng-fu Chen
CNChengyun Ning
Chengyun Ning
YGYuanjun Guo
Yuanjun Guo

5 January 2017 in RSC Advances
Verified
Journal Article
Open access
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Cheng-fu ChenCheng-fu Chen
Cheng-fu Chen
KWK. Wharton
K. Wharton
Bonding of air plasma oxidized polydimethylsiloxane (PDMS) strips is evaluated in this paper by peel testing. Two PDMS–PDMS strips, after being treated with air plasma, were brought together for bonding into a specimen, which was subsequently subjected to peeling until breaking apart. The maximum load applied in each peel test was used to indicate the bonding strength. Among the 68 specimens tested, 40 experienced a maximum load in the range of 0.1–0.2 N mm−1. Seventy-six percent of the specimens under peel testing failed at the cohesive mode, meaning that the air plasma-based bonding can be strong enough to retain its integrity after peeling. Correlation between the maximum load and failure modes suggests that strong bonding can be achieved with a higher plasma power for 50–60 seconds of treatment in air plasma. Based on the Kendall energy balance equation, we suggest that the higher the maximum load per unit width applied in the peel test, the larger the adhesion energy in the bonding interface.

4 December 2017 in Journal of Adhesion Science and Technology
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Journal Article
Closed access
Cheng-fu ChenCheng-fu Chen
Cheng-fu Chen
The fracture energy, toughness and failure modes of air plasma oxidized polydimethylsiloxane (PDMS) bonding are evaluated in this paper. Each PDMS–PDMS bonded specimen was subjected to T-peel testing at a constant-displacement rate. The load–extension curve from each test was analyzed by the principle of energy balance in linearly elastic fracture mechanics, to calculate the fracture energy (critical strain energy), which is the maximal strain energy a bonded specimen can withstand without losing its assembly integrity, and toughness (surface energy), which is the bonding energy at the interface. A distribution of calculated values against the air plasma treatment parameters shows the predominant range of 0.1 to 0.4 N/mm for fracture energy and 0.1 to 0.2 N/mm for toughness. Together with an analysis of three failure modes (cohesive, adhesive, and mixed), the results suggest 0.1 N/mm as the threshold of the fracture energy for weak bonding, below which a specimen will be likely to fail through debonding. A set of treatment parameters are recommended for using air plasma to achieve strong bonding.

1 August 2012 in Surface Engineering
Verified
Journal Article
Closed access
YGY H Gu
Y H Gu
Cheng-fu ChenCheng-fu Chen
Cheng-fu Chen
SBS Bandopadhyay
S Bandopadhyay
CNC Y Ning
C Y Ning
YGY J Guo
Y J Guo
This paper addresses the residual stress in the microarc oxidation (MAO) coating on AZ31 magnesium alloy. The MAO coating was deposited by pulsed direct current (dc) and examined by scanning electron microscopy and X-ray diffraction for its microstructure and composition. The porosity of the coatings was measured by potentiodynamic polarisation tests and found to be in the range of 3–6%. The residual stresses in the MAO coatings prepared at 300, 500, 1000 and 3000 Hz respectively were found to be between −860 and −1272 MPa. Using a high pulse frequency at 3000 Hz can produce a less porous and less stressed MAO coating, a desirable feature in the biomedical applications of MAO coated AZ31. This finding was further verified by establishing a first principle relation between the residual stress and the porosity via Stoney equation, which enables extrapolation of the experimental data measured.