Fracture modes in brittle coatings with large interlayer modulus mismatch

Fracture modes in a model glass–polymer coating–substrate system indented with hard spheres are investigated. The large modulus mismatch between the glass and polymer results in distinctive transverse fracture modes within the brittle coating: exaggerated circumferential (C) ring cracks that initiate at the upper coating surface well outside the contact (as opposed to the near-contact Hertzian cone fractures observed in monolithic brittle materials); median–radial (M) cracks that initiate at the lower surface (i.e., at the substrate interface) on median planes containing the contact axis. Bonding between the coating and substrate is sufficiently strong as to preclude delamination in our system. The transparency of the constituent materials usefully enables in situ identification and quantification of the two transverse fracture modes during contact. The morphologies of the cracks and the corresponding critical indentation loads for initiation are measured over a broad range of coating thicknesses (20 mm to 5.6 mm), on coatings with like surface flaw states, here ensured by a prebonding abrasion treatment. There is a well-defined, broad intermediate range where the indented coating responds more like a flexing plate than a Hertzian contact, and where the M and C cracks initiate in close correspondence with a simple critical stress criterion, i.e., when the maximum tensile stresses exceed the bulk strength of the (abraded) glass. In this intermediate range the M cracks generally form first—only when the flaws on the lower surface are removed (by etching) do the C cracks form first. Finite element modeling is used to evaluate the critical stresses at crack initiation and the surface locations of the crack origins. Departures from the critical stress condition occur at the extremes of very thick coatings (monolith limit) and very thin coatings (thin-film limit), where stress gradients over the flaw dimension are large. Implications of the results concerning practical coating systems are considered.

[1]  O. Zharikov,et al.  Superconductivity of graphite intercalation compound with lithium C2Li , 1989 .

[2]  Kazuo Hokkirigawa,et al.  Fracture Mechanisms of Ceramic Coatings in Indentation , 1994 .

[3]  K. Hayashi,et al.  Elastic-Plastic Analysis of Stresses and Initiation of Cracks in a Ceramic Coating Under Indentation by an Elastic Sphere , 1998 .

[4]  B. Lawn,et al.  Effect of substrate and bond coat on contact damage in zirconia-based plasma-sprayed coatings , 1997 .

[5]  M. Dresselhaus,et al.  Excess Li ions in a small graphite cluster , 1997 .

[6]  B. Lawn,et al.  On the theory of Hertzian fracture , 1967, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[7]  Kyriakos Komvopoulos,et al.  Elastic-plastic finite element analysis of indented layered media , 1989 .

[8]  Kenji Takeuchi,et al.  The production and structure of pyrolytic carbon nanotubes (PCNTs) , 1993 .

[9]  B. Lawn Fracture of Brittle Solids by Brian Lawn , 1993 .

[10]  G. Bondarenko,et al.  Vibrational spectra of superdense lithium graphite intercalation compounds , 1998 .

[11]  B. Lawn,et al.  Indentation fracture: principles and applications , 1975 .

[12]  Fujita,et al.  Edge state in graphene ribbons: Nanometer size effect and edge shape dependence. , 1996, Physical review. B, Condensed matter.

[13]  B. Lawn,et al.  Mechanical characterization of plasma sprayed ceramic coatings on metal substrates by contact testing , 1996 .

[14]  H. M. Chan LAYERED CERAMICS: Processing and Mechanical Behavior , 1997 .

[15]  Brian R. Lawn,et al.  Deformation and fracture of mica-containing glass-ceramics in Hertzian contacts , 1994 .

[16]  M. Swain,et al.  Mechanical property characterization of thin films using spherical tipped indenters , 1994 .

[17]  Z. Ogumi,et al.  7Li NMR studies on a lithiated non-graphitizable carbon fibre at low temperatures , 1997 .

[18]  K. N. Semenenko,et al.  New Alkali Metal-Graphite Intercalation Compounds at High Pressures , 1992 .

[19]  T. Yamabe,et al.  Recent development of study on polyacenic semiconductor (PAS) materials , 1994 .

[20]  B. Lawn,et al.  A Study of Dislocation Arrays at Spherical Indentations in LiF as a Function of Indentation Stress and Strain , 1969 .

[21]  J. Fischer,et al.  High capacity carbon anode materials: Structure, hydrogen effect, and stability , 1997 .

[22]  B. Lawn,et al.  Hertzian Fracture Experiments on Abraded Glass Surfaces as Definitive Evidence for an Energy Balance Explanation of Auerbach's Law , 1969 .

[23]  B. Lawn,et al.  Contact Damage in Plasma‐Sprayed Alumina‐Based Coatings , 1996 .

[24]  F. C. Roesler,et al.  Brittle Fractures near Equilibrium , 1956 .

[25]  Bunyamin Aksakal,et al.  A finite-element analysis of the indentation of an elastic-work hardening layered half-space by an elastic sphere , 1998 .

[26]  J. Tillett,et al.  Fracture of Glass by Spherical Indenters , 1956 .

[27]  Andrew G. Glen,et al.  APPL , 2001 .

[28]  M. Dresselhaus,et al.  Electronic structure of fluorine doped graphite nanoclusters , 1999 .

[29]  Frank Richter,et al.  Comparison between an elastic-perfectly plastic finite element model and a purely elastic analytical model for a spherical indenter on a layered substrate , 1997 .

[30]  B. Lawn,et al.  Damage-resistant alumina-based layer composites , 1996 .

[31]  S. Yamazaki,et al.  Study of the states of Li doped in carbons as an anode of LiB by 7Li NMR spectroscopy , 1998 .

[32]  Pierre Montmitonnet,et al.  Finite Element Analysis of Elastoplastic Indentation: Part II—Application to Hard Coatings , 1993 .

[33]  S. Timoshenko,et al.  THEORY OF PLATES AND SHELLS , 1959 .

[34]  T. R. Wilshaw,et al.  The Hertzian fracture test , 1971 .

[35]  M. Endo,et al.  A Mechanism of Lithium Storage in Disordered Carbons , 1994, Science.

[36]  M. Dresselhaus,et al.  Lithium storage behavior for various kinds of carbon anodes in Li ion secondary battery , 1996 .

[37]  T. Bell,et al.  Finite element analysis of plastic deformation of various TiN coating/ substrate systems under normal contact with a rigid sphere , 1995 .

[38]  T. Yamabe,et al.  Characteristics of deeply Li-doped polyacenic semiconductor material and fabrication of a Li secondary battery , 1995 .

[39]  Brian R. Lawn,et al.  Indentation stress-strain curves for “quasi-ductile” ceramics , 1996 .

[40]  Yair Ein-Eli,et al.  Chemical Oxidation: A Route to Enhanced Capacity in Li‐Ion Graphite Anodes , 1997 .

[41]  E. Peled,et al.  Improved Graphite Anode for Lithium‐Ion Batteries Chemically Bonded Solid Electrolyte Interface and Nanochannel Formation , 1996 .

[42]  Wang,et al.  Coulomb-gap magnetotransport in granular and porous carbon structures. , 1994, Physical review. B, Condensed matter.

[43]  B. Lawn,et al.  Damage Modes in Dental Layer Structures , 1999, Journal of dental research.

[44]  T. Yamabe,et al.  Structure and properties of deeply Li-doped polyacenic semiconductor materials beyond C6Li stage , 1994 .

[45]  Anthony G. Evans,et al.  Spherical impression of thin elastic films on elastic–plastic substrates , 1999 .