Sentence examples for this modulus is from inspiring English sources

The Young's modulus of elasticity represented by the initial slope of the curve was computed for each mix and the variation of this modulus is shown as an inset in Fig. 6.

The modulus of the ring ({mathcal{S}}{setminus} [-r,r]) tends to infinity as (rsearrow 0) and 0 for (r=infty.) This modulus is continuous and so the intermediate value theorem gives us an r so that (mathrm{Mod}({mathcal{S}}{setminus} [-r,r])=mathrm{Mod}({mathcal{S}}{setminus} Omega )).

The local modulus of continuity of a function g : [ 0, 1 ] → R at a point x is defined by ω ( g, x, t ) = sup { | g ( v ) − g ( w ) | : v, w ∈ [ x − t, x + t ] ∩ [ 0, 1 ] }, t ≥ 0. For p ≥ 1, the average modulus of continuity is defined by τ ( g, t ) p = ∥ ω ( g, ⋅, t ) ∥ p. This modulus is well defined whenever g is a bounded measurable function.

This modulus is close to experimental results, where a range of ≈7.15 MPa was reported [8], [34].

This modulus was 8.2, 7.8, and 6.8 for plain fused silica, aluminosilicate, and borosilicate glasses, respectively.

This change in the modulus is attributed to decohesion at the matrix-reinforcement interface.

This growth factor in the modulus is there for technical reasons, but has important consequences for representation theory and in the case of our orientation maps, it will have a clear influence on the pinwheel density we shall calculate later; we shall discuss this at the end of the present section.

If the modulus is large, the material is stiff.

If the modulus is low, the fractures will be wider.

This low modulus is attributed to the stress-induced martensite transformation under compressive load.

This Weibull modulus is used to relate the strengths for different test methods using an equivalent volume method.