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Easy Elasticity Theory

Friday, April 23, 2010. Hookes law in component form. We start with Hookes law for the strain tensor, and then substitute the E and nu. Material properties for K and mu. We see that there is still a compression term, now on the right, but not a pure shear term, and both terms contain both material constants. We mention here that nu. The shear modulus is about is about 40 of the Youngs modulus. The bulk modulus of compression is therefore about 1.5 to 2 times larger than the shear modulus. The shea.

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Easy Elasticity Theory

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Friday, April 23, 2010. Hookes law in component form. We start with Hookes law for the strain tensor, and then substitute the E and nu. Material properties for K and mu. We see that there is still a compression term, now on the right, but not a pure shear term, and both terms contain both material constants. We mention here that nu. The shear modulus is about is about 40 of the Youngs modulus. The bulk modulus of compression is therefore about 1.5 to 2 times larger than the shear modulus. The shea.

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This web page baergblog.blogspot.com states the following, "Friday, April 23, 2010." We saw that the webpage said " Hookes law in component form." It also said " We start with Hookes law for the strain tensor, and then substitute the E and nu. Material properties for K and mu. We see that there is still a compression term, now on the right, but not a pure shear term, and both terms contain both material constants. We mention here that nu. The shear modulus is about is about 40 of the Youngs modulus. The bulk modulus of compression is therefore about 1. 5 to 2 times larger than the shear modulus."

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