Kinematics of deformation (Continuum mechanics)

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SUMMARY

The discussion focuses on the kinematics of deformation in continuum mechanics, specifically addressing the calculation of differential position vectors between material points. The participants analyze the expression for the gradient of a function, $$grad(x) = grad(\frac{f(R,t)}{R} X)$$, and apply product rules to derive the relationship between initial and deformed configurations. The correct differential position vector is established as $$\mathbf{dx}=\mathbf{i_r}df=\frac{\partial f}{\partial R}(\mathbf{i_r}dR)$$, which leads to insights about the deformation gradient tensor $$\mathbf{F}$$.

PREREQUISITES
  • Understanding of continuum mechanics principles
  • Familiarity with differential calculus and vector analysis
  • Knowledge of deformation gradient tensor concepts
  • Experience with spherical coordinate systems in mechanics
NEXT STEPS
  • Study the derivation of the deformation gradient tensor $$\mathbf{F}$$ in continuum mechanics
  • Learn about the application of polar coordinates in kinematics
  • Explore the implications of the gradient operator in material deformation
  • Investigate the relationship between material points and their deformations over time
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Students and professionals in mechanical engineering, particularly those specializing in continuum mechanics, material science, and applied mathematics, will benefit from this discussion.

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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