Two times this quantity times surface energy density over pi gives the square of the crack length in Griffith's formula. A sudden drop in this quantity with increasing temperature is one way of measuring the glass transition temperature. One method of calculating this quantity is using the impulse excitation technique to measure the frequency of the flexure mode. Two times the moment of inertia times this quantity appears in the denominator of the expression for the deflection angle of a cantilever. Under the assumption of isotropy, this quantity is equal to quantity one plus the Poisson (*) ratio end quantity times two times the shear modulus. Under an elastic and linear response, this quantity represents the proportionality constant in Hooke's law, and this quantity is measured as the sl
Two times this quantity times surface energy density over pi gives the square of the crack length in Griffith's formula. A sudden drop in this quantity with increasing temperature is one way of measuring the glass transition temperature. One method of calculating this quantity is using the impulse excitation technique to measure the frequency of the flexure mode. Two times the moment of inertia times this quantity appears in the denominator of the expression for the deflection angle of a cantilever. Under the assumption of isotropy, this quantity is equal to quantity one plus the Poisson (*) ratio end quantity times two times the shear modulus. Under an elastic and linear response, this quantity represents the proportionality constant in Hooke's law, and this quantity is measured as the slope of a certain curve before the yield point. For 10 points, name this quantity which is equal to the ratio of the stress to the strain on a material.
Two times this quantity times surface energy density over pi gives the square of the crack length in Griffith's formula.
Young's modulus [or tensile modulus; or elastic modulus or modulus of elasticity until "elastic" is read]