Introduction to Elasticity/Constitutive example 6

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Example 6

Given:

For an isotropic material


   K = \lambda + \frac{2}{3} \mu~,~~~
   E = \frac{\mu(3\lambda+2\mu)}{\lambda+\mu}~,~~~
   \nu = \frac{\lambda}{2(\lambda+\mu)}

Verify:

  1. \mu = \frac{E - 3\lambda + r}{4}
  2. K = \frac{E + 3\lambda + r}{6}

where r = \sqrt{E^2 + 9\lambda^2 + 2E\lambda}.

Solution

From the second equation that has been given


   E\lambda + E\mu = 3\mu\lambda + 2\mu^2

or,


   2\mu^2 - (E - 3\lambda)\mu - E\lambda = 0

Therefore,


  \mu = \frac{(E-3\lambda) \pm \sqrt{(E-3\lambda)^2 + 8E\lambda}}{4}

or,


  \mu = \frac{(E-3\lambda) \pm \sqrt{E^2 + 9\lambda^2 + 2E\lambda}}{4}

or,


  \mu = \frac{E-3\lambda \pm r}{4}

To find out whether the plus or the minus sign should be placed before r in the above equation, we put everything in terms of \nu and E. Thus,

\begin{align}
   \mu & = \frac{E}{2(1+\nu)} \\
   \lambda & = \frac{\nu E}{(1+\nu)(1-2\nu)} \\
   E - 3\lambda & = \frac{E(1 - 2\nu^2 - 4\nu)}{(1+\nu)(1-2\nu)} \\
   8E\lambda & = \frac{8\nu E^2}{(1+\nu)(1-2\nu)}
\end{align}

Plugging these into the equation for \mu, multiplying both sides by (1+\nu)(1-2\nu) and dividing by E, we get


  2(1-2\nu) = (1-2\nu^2-4\nu) \pm \sqrt{(1-2\nu^2-4\nu)^2 + 8\nu(1+\nu)(1-2\nu)}

The limiting value of \nu is 0.5. Plugging this value into the above equation, we get,


  0 = -1.5 \pm 1.5

The above can be true only if the sign is positive. Therefore, the correct relation is


  \mu = \frac{E-3\lambda + r}{4}

Plugging this relation into the first of the given equations, we have,

\begin{align}
  K & = \lambda + \cfrac{2}{3}\left(\cfrac{E-3\lambda+r}{4}\right) \\
    & = \cfrac{6\lambda + E -3\lambda+r}{6} \\
  K & = \cfrac{E +3\lambda+r}{6}
\end{align}
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