Understanding Bulk Modulus: Explaining the Relationship with Pressure and Volume

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SUMMARY

The discussion focuses on the derivation of the bulk modulus (K) from the relationship between pressure (delta p) and volume change (delta V) in isotropic materials. The formula K = -V dp/dV is established by taking the limit of delta p approaching zero, which aligns with the definition of bulk modulus. The first equation, delta V = [-3V delta p (1 - 2c)] / E, is derived from the generalized Hooke's law for isotropic materials, incorporating Young's modulus (E) and Poisson's ratio (c). The bulk modulus for isotropic materials is ultimately expressed as K = E / [3(1 - 2c)].

PREREQUISITES
  • Understanding of Young's modulus (E)
  • Familiarity with Poisson's ratio (c)
  • Knowledge of isotropic materials and their properties
  • Basic calculus, particularly limits and derivatives
NEXT STEPS
  • Study the derivation of the generalized Hooke's law for isotropic materials
  • Explore the applications of bulk modulus in material science
  • Learn about the relationship between pressure, volume, and elasticity in fluids
  • Investigate the implications of Poisson's ratio on material behavior under stress
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Students and professionals in materials science, mechanical engineering, and physics who are looking to deepen their understanding of material elasticity and the relationships between pressure and volume changes in isotropic materials.

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Homework Statement



My textbook says, delta V = [-3V delta p (1 - 2c)] /E
where,
delta V = change in volume
delta p = change in pressure
c = poisson's ratio
E = young's modulus

Taking the limit as delta p tends to zero, we can write the bulk modulus K as,
K = -V dp/dV

but I'm not clear with how they got K by taking the limit as delta p goes to zero...could someone explain that please. Thanks!
 
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The second equation isn't meant to follow from the first. The second equation is the definition of the bulk modulus. The first equation comes from using the generalized Hooke's equation for an isotropic material (in your notation):

\epsilon=\frac{1}{E}\sigma_1-\frac{c}{E}\sigma_2-\frac{c}{E}\sigma_3

where we plug in the pressure p for all three stresses. Also, the change in volume

\Delta V=(1+\epsilon)^3-1\approx3\epsilon

for small strains. The bulk modulus for an isotropic material would therefore be

K=\frac{E}{3(1-2c)}
 

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