Kinematics of deformation (Continuum mechanics)

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Homework Help Overview

The discussion revolves around a problem from continuum mechanics, specifically focusing on the kinematics of deformation. The original poster is seeking assistance with part (a) of a question related to the governing equations of deformation as presented in a textbook.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants are discussing the application of gradient operations and product rules in the context of deformation. The original poster has attempted to express the gradient of a function related to deformation, while others are suggesting alternative approaches to define differential position vectors between material points.

Discussion Status

There are multiple lines of reasoning being explored, with participants questioning the correctness of their approaches and seeking clarification on the definitions and applications of certain mathematical expressions. Some guidance has been offered regarding the interpretation of the radial coordinate direction and its implications for the deformation gradient tensor.

Contextual Notes

Participants are navigating through the complexities of the problem, with some expressing uncertainty about their calculations and assumptions. The discussion reflects a collaborative effort to clarify the mathematical relationships involved in the kinematics of deformation.

Jinjolee
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Homework Statement
Calculating the deformation gradient, velocity field and acceleration field of a cavity motion
Relevant Equations
F=grad(x)
J=det(F)
v=dx/dt
A=dv/dt
Question is extracted from "Ellad B Tadmor, Ronald E Miller, Ryan S Elliott - Continuum mechanics and thermodynamics From fundamental concepts to governing equations".
I just got stuck at part (a). I think if part(a) is solved, I may be able to do the other parts.
 

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What have you done so far?
 
Chestermiller said:
What have you done so far?
I tried to do grad(x) = $$grad(\frac {f(R,t)}{R} X)$$
and by product rules:
=$$\frac{f(R,t)}{R} ∇X + X ⋅ ∇(\frac {f(R,t)}{R})$$
If I am correct, ∇X should be I, so
=$$\frac{f(R,t)}{R} I + X ⋅ ∇(\frac {f(R,t)}{R})$$
This is by far what I have done.
 
Let's try this a little differently. Suppose, in the initial configuration, you have two material points at R and R+dR connected by a differential position vector $$\mathbf{dX}=dR\mathbf{i_r}$$ In terms of f(R,t), what is the differential position vector between these same two material points at time t?
 
Last edited:
Chestermiller said:
Let's try this a little differently. Suppose, in the initial configuration, you have two material points at R and R+dR connected by a differential position vector $$\mathbf{dX}=dR\mathbf{i_r}$$ In terms of f(R,t), what is the differential position vector between these same two material points at time t?
I this it should apply $$dx=x(X+dX)-x(X)$$
But I am not sure about the answer. Is it$$\frac{f(R+dR{\mathbf{i_r}},t)}{R+dR\mathbf{i_r}}(R\mathbf{i_r}+dR\mathbf{i_r})-\frac{f(R,t)}{R}R\mathbf{i_r}$$?
 
Jinjolee said:
I this it should apply $$dx=x(X+dX)-x(X)$$
But I am not sure about the answer. Is it$$\frac{f(R+dR{\mathbf{i_r}},t)}{R+dR\mathbf{i_r}}(R\mathbf{i_r}+dR\mathbf{i_r})-\frac{f(R,t)}{R}R\mathbf{i_r}$$?
No. You may be overthinking it. The quantity ##\frac{\mathbf{X}}{R}## is the unit vector in the radial spherical coordinate direction ##\mathbf{i_r}## (which is constant). So the differential position vector between the same two material points at time t is $$\mathbf{dx}=\mathbf{i_r}df=\frac{\partial f}{\partial R}(\mathbf{i_r}dR)$$What does that tell you about the r-r component of the deformation gradient tensor ##\mathbf{F}##?
Next, let's consider a differential position vector between two material points that are initially oriented in the ##\theta## polar coordinate direction: $$\mathbf{dX}=(Rd{\theta})\mathbf{i_{\theta}}$$In terms of f(R,t), what is the differential position vector between this same pair of material points at time t?
 
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