2008
DOI: 10.1016/j.jmps.2008.06.005
|View full text |Cite
|
Sign up to set email alerts
|

Modeling the growth and branching of plants: A simple rod-based model

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
20
1

Year Published

2010
2010
2017
2017

Publication Types

Select...
5
3

Relationship

0
8

Authors

Journals

citations
Cited by 25 publications
(21 citation statements)
references
References 47 publications
0
20
1
Order By: Relevance
“…By treating the growing rod as a one-dimensional continuum that can change its reference length, diameter and stiffness, various authors have formulated a theory for how its shape can vary with time [10,[21][22][23][24]. A general discussion of possible evolution equations for the natural curvature has also been considered [22,25], with autotropism being the primary driver.…”
Section: Introductionmentioning
confidence: 99%
“…By treating the growing rod as a one-dimensional continuum that can change its reference length, diameter and stiffness, various authors have formulated a theory for how its shape can vary with time [10,[21][22][23][24]. A general discussion of possible evolution equations for the natural curvature has also been considered [22,25], with autotropism being the primary driver.…”
Section: Introductionmentioning
confidence: 99%
“…XIX ]. The discussion in Love's classic text [23] is supplemented by material on branching, adhesion and material momentum from recent works (see [19,22,24,25] and references therein). Referring to Figure 4, the centerline of the rod is parameterized by an arc-length coordinate s ∈ [0, ℓ] and the position of a point on the centerline is denoted by the vector-valued function r(s).…”
Section: A Simple Model Of An Adhered Cnt Pairmentioning
confidence: 99%
“…Assuming that the Euler-Lagrange differential equation is satisfied by θ * (s), and given that the Weierstrass and Erdmann-Weierstrass conditions are satisfied, it is well-known that satisfaction of either J1 (where applicable) 5 or L1 is sufficient for θ * (s) to be a weak minimum of I (see, e.g., [2,6]). …”
Section: Other Necessary and Sufficient Conditionsmentioning
confidence: 99%
“…Furthermore, the absence of a solution to the Riccati equation for the free-free strut is a clear indication of the degenerate nature of this case and the need for a modified treatment of the type proposed recently by Manning [16] (see also Kuznetsov and Levyakov [10,13]). We close the paper with a discussion of future applications to Legendre's treatment to the stability of branched equilibria of elastic rods such as those discussed in [5,19].…”
mentioning
confidence: 99%