The Effect of Temperature and Sizes on Deformation of Cantilever Rectangular Plate with Double Layer

Article Preview

Abstract:

As depositing layers with different thermal expansion coefficients, the residual gradient stress will cause the structure deformed. The deformation of structure in the free ending, middle section, and clamped end are detail investigated. It is found the clamped end often has complex deformation shape. The warpage due to buckling is found. The results show if the thickness of structure is much larger than above deposing layer, warpage will hardly happen and the free ending will have more flat region. As the thickness of structure layer being not much larger than above deposing layer, the warpage happens and the free ending is parabolic shape. In the clamped end, the complex deformation even is concave shape in the center part but protruding shape in the side region. The larger temperature difference will be more easily warpage and be no more flat. The results also show that as the ratio of length to width decreasing, seriously warpage and complex deformation happens. The free ending may be a little protruding shape. However, if the ratio of length to width is larger, the free ending will have concave shape.

You might also be interested in these eBooks

Info:

Periodical:

Key Engineering Materials (Volumes 326-328)

Pages:

1157-1160

Citation:

Online since:

December 2006

Export:

Price:

Permissions CCC:

Permissions PLS:

Сopyright:

© 2006 Trans Tech Publications Ltd. All Rights Reserved

Share:

Citation:

[1] R. Maboudian, and R. T. Howe, Critical review: Adhesion in surface micromechanical structures, " J. Vac. Sci. Technol. B, vol. 15, pp.1-20.

Google Scholar

[3] Fang, W.; Wickert, J.A. Post-buckling of micromachined beams" MEMS , 94, Proceedings, 1994, Page(s): 182 -187.

Google Scholar

[4] Xin Zhang; Tong-Yi Zhang; Man Wong; Yitshak Zohar Effects of high-temperature rapid thermal annealing on the residual stress of LPCVD-polysilicon thin films "MEMS , 97, Proceedings, 1997, Page(s): 535 -540.

DOI: 10.1109/memsys.1997.581922

Google Scholar

[5] Abe, T.; Reed, M.L. Low strain sputtered polysilicon for micromechanical structures" Micro Electro Mechanical Systems, 1996, MEMS , 96, Proceedings. , 1996, Page(s): 258 -262.

DOI: 10.1109/memsys.1996.493990

Google Scholar

[6] H. Yen, C. Lee, R. Chen, and M. J. Lin, 2001, Analysis and Fabrication of Deformable Focusing Micromirrors, IMECE 2001, Nov. 11-16, 2001, New York, NY, U. S. A.

Google Scholar

[7] Max Ti-kuang Hou and Rongshun Chen, Effect of width on the stress-induced bending of micromachined bilayer cantilevers, JMM, vol. 13, 2003, pp.141-148. Figure 1 Numerical model. 0.

DOI: 10.1088/0960-1317/13/1/320

Google Scholar

5 0 20 40 width(µm) deformation(µm) T=800℃ T=700℃ T=600℃ T=500℃ T=400℃ T=300℃ T=200℃ T=100℃ (A)Free ending(L1) 0.

Google Scholar

2 0 20 40 width(µm) deformation(µm) T=800℃ T=700℃ T=600℃ T=500℃ T=400℃ T=300℃ T=200℃ T=100℃ (B)Center line(L2).

Google Scholar

020 0 20 40 width(µm) deformation(µm) T=800℃ T=700℃ T=600℃ T=500℃ T=400℃ T=300℃ T=200℃ T=100℃ (C)Clamp ending(L3) Figure 2 Effect of process temperature on deformation. 0.

Google Scholar

7 0 10 20 30 40 width(μ m) deformation(μ m) h1=1. 5μ m h1=1μ m h1=0. 5μ m h1=0. 2μ m h1=0. 1μ m h1=0. 05μ m (A)Free ending(L1) 0.

DOI: 10.31274/rtd-180816-1958

Google Scholar

25 0 10 20 30 40 width(μ m) deformation(μ m) h1=1. 5μ m h1=1μ m h1=0. 5μ m h1=0. 2μ m h1=0. 1μ m h1=0. 05μ m (B)Center line(L2) 0. 00E+00.

DOI: 10.31274/rtd-180816-1958

Google Scholar

[5] 00E-03.

Google Scholar

[1] 00E-02.

Google Scholar

[1] 50E-02.

Google Scholar

[2] 00E-02.

Google Scholar

[2] 50E-02.

Google Scholar

[3] 00E-02 0 10 20 30 40 width(μ m) deformation(μ m) h1=1. 5μ m h1=1μ m h1=0. 5μ m h1=0. 2μ m h1=0. 1μ m h1=0. 05μ m (C)Clamp ending(L3) Figure 3 Effect of metal layer thickness on deformation. 0.

DOI: 10.7717/peerj.10368/fig-3

Google Scholar

[1] 5 2.

Google Scholar

[2] 5 0 10 20 30 40 width(μ m) deformation(μ m) h2=3. 5μ m h2=3μ m h2=2μ m h2=1μ m h2=0. 5μ m (A)Free ending(L1).

Google Scholar

00E+00.

Google Scholar

[1] 00E-01.

Google Scholar

[2] 00E-01.

Google Scholar

[3] 00E-01.

Google Scholar

[4] 00E-01.

Google Scholar

[5] 00E-01.

Google Scholar

[6] 00E-01.

Google Scholar

[7] 00E-01 0 10 20 30 40 width(μ m) deformation(μ m) h2=3. 5μ m h2=3μ m h2=2μ m h2=1μ m h2=0. 5μ m (B)Center line(L2) -1. 00E-02.

Google Scholar

00E+00.

Google Scholar

[1] 00E-02.

Google Scholar

[2] 00E-02.

Google Scholar

[3] 00E-02.

Google Scholar

[4] 00E-02.

Google Scholar

[5] 00E-02.

Google Scholar

[6] 00E-02 0 10 20 30 40 width(μ m) deformation(μ m) h2=3. 5μ m h2=3μ m h2=2μ m h2=1μ m h2=0. 5μ m (C)Clamp ending(L3) Figure 4 Effect of structure layer thickness on the deformation. 0.

Google Scholar

8 0 10 20 30 40 width(μ m) deformation(μ m) L=50μ m L=40μ m L=30μ m L=20μ m L=10μ m (A)Free ending(L1) 0.

Google Scholar

25 0 10 20 30 40 width(μ m) deformation(μ m) L=50μ m L=40μ m L=30μ m L=20μ m L=10μ m (B)Center line(L2).

Google Scholar

00E+00.

Google Scholar

[2] 00E-03.

Google Scholar

[4] 00E-03.

Google Scholar

[6] 00E-03.

Google Scholar

[8] 00E-03.

Google Scholar

[1] 00E-02.

Google Scholar

[1] 20E-02.

Google Scholar

[1] 40E-02.

Google Scholar

[1] 60E-02 0 10 20 30 40 width(μ m) deformation(μ m) L=50μ m L=40μ m L=30μ m L=20μ m L=10μ m (C)Clamp ending(L3) Figure 5 Effect of length on deformation.

Google Scholar