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We use the ratio I = I (200) / I (006) + I (200) to evaluate the a-axis grains' volume fraction of the GdBCO film, as shown in Figure 2.
This illustrates that a-axis-oriented grains appear in the 1,030-nm-thick 1,030-nm-thick 1,030-nm-thickains' volume fraction becomes more and more as the thickness comes up to 1,450 nm.
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Density measurements for a given specimen involve the determination of any two of the following quantities: pore volume, bulk volume, or grain volume, along with the weight.
The shrinkage and disappearance of small Ba5Nb4O15 grains in a large grain matrix at 1133 K observed by transmission electron microscopy (TEM), included grain volume and boundary shrinkage.
Further reaction in the grains takes place according to a shrinking, partially-reacted-core mechanism, accompanied by an increase in grain volume.
We have shown that the individual grains in the antiferromagnetic (AF) layer of exchange bias systems contain a single AF domain and reverse over an energy barrier which is grain volume dependent.
A detailed characterization of the austenite grain volume distribution at room temperature was performed as a function of the prior bainitic holding time.
Consequently, the addition of phosphorus leads to a higher degree of carbon enrichment and a narrower grain volume distribution of the metastable austenite.
The concepts of five parameters of nominal water cement ratio, equivalent water cement ratio, average paste thickness, fly ash binder ratio, grain volume fraction of fine aggregates and Modified Tourfar's Model were introduced.
It is defined as the interstitial surface area of the pores and pore channels for each unit of bulk volume, grain volume, or pore volume, or for a unit of weight of a material.
The stability of the individual austenite grains with respect to their martensitic transformation depends on both the local carbon content and the grain volume for austenite grains smaller than 20 μm3.
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