This journal is © The Royal Society of Chemistry 2022 Soft Matter, 2022, 18, 2979–2991 | 2979
Cite this: Soft Matter, 2022,
18, 2979
Interaction of a defect with the reference
curvature of an elastic surface
Manish Singh, Animesh Pandey and Anurag Gupta *
The morphological response of two-dimensional curved elastic sheets to an isolated defect (dislocation/
disclination) is investigated within the framework of Fo
¨
ppl–von Ka
´
rma
´
n shallow shell theory. The reference
surface, obtained as a shell configuration in the absence of defect and external forces, accordingly has a
finite non-zero curvature. The interaction of the defect with the curvature of the reference surface is
emphasized through the problem of defect driven buckling of an elastic sheet. Detailed bifurcation
diagrams, including the post-buckling deformation behaviour, are plotted for several combinations of defect
types, reference curvatures, and boundary conditions. A pitchfork bifurcation is obtained when the reference
surface is flat irrespective of the defect type and boundary condition. For curved reference surfaces there
are some cases where the pitchfork bifurcation persists and others where it does not. The varied response
demonstrates the rich interaction of the defects with the curvature of the reference surface.
1 Introduction
The mechanical behaviour of a two-dimensional (2D) elastic
surface, in response to an isolated defect (dislocation/disclination),
is fundamentally different from that of a three-dimensional (3D)
elastic body. Whereas a dislocation (or a disclination) in a 3D
elastic body necessarily causes a far field stress distribution,
1
the elastic surface can explore the third (out-of-plane) dimen-
sion so as to keep the stress fields localized around the defect
point.
2
Consequently, disclinations in elastic surfaces are fea-
sible (energetically) while disclinations in 3D elastic solids are
not. The response of an elastic surface to a defect is therefore
predominantly geometric, characterized in terms of kine-
matical quantities such as transverse deflection and Gaussian
curvature. This understanding has led to significant literature
in the recent past where defect induced shape transformations
have been used to explain novel physical characteristics of 2D
crystalline and amorphous surfaces.
3–8
When posed as a boundary value problem, the isolated
defect problem has been well studied assuming the elastic
sheet to be a Fo ¨ppl–von Ka ´rma ´n plate with a flat reference
surface and free boundary condition.
2,9–11
The reference
surface refers to the configuration achieved in the absence of
defects and external forces. In accordance with the physical
observations, depending on a dimensionless parameter, which
is a function of the plate size, elastic constants, and defect
strength, the plate may choose to respond (to the defect, in the
absence of external forces) either through pure stretching,
thereby remaining flat, or by buckling out of the plane. The
buckled plate due to a positive disclination, for instance,
acquires a conical shape whereas it acquires a saddle shape
due to a negative disclination.
2
The buckled solution in fact
appears as a symmetric pitchfork bifurcation regardless of the
defect type (dislocation or disclination) and boundary conditions,
as long as the reference surface remains flat; this is further
elaborated in a paragraph below, see also Fig. 1.
Our interest is in studying the deformation behaviour of a
2D elastic sheet with an isolated defect whose reference surface
has a finite non-zero curvature. We restrict ourselves to elastic
Fig. 1 The global bifurcation diagram for a positive disclination in an
elastic sheet with a flat reference surface and free boundary.
Department of Mechanical Engineering, Indian Institute of Technology Kanpur,
208016, India. E-mail: ag@iitk.ac.in
Received 26th January 2022,
Accepted 14th March 2022
DOI: 10.1039/d2sm00126h
rsc.li/soft-matter-journal
Soft Matter
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