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Figure  4b displays the corresponding Bland-Altman plot of thermal dose predicted treatment volume and NPV showing the absolute difference with mean ± 1.96 SD acceptance limits.

The specific heat capacity used in the study of Hyndman et al. (1979) was therefore considered suitable for use with the materials of our core samples retrieved from the JFAST borehole in the west Pacific. Figure 5 Cross plots of thermal diffusivity and thermal conductivity.

Figure 5 shows a plot of normalized thermal conductivity as a function of volume fraction for Cu, CuO, and MWNT nanofluids.

In the short-term plots, indexes of thermal anomalies were constant and nearly flat, which suggests that the effusion of lava was stationary (e.g., the nighttime of 20 June in Fig. 5a).

Open image in new window Fig. 14 The relation between f/f 0 and DR. The plots of the thermal enhancement factor with the Reynolds number with various PRs and DRs are plotted in Fig. 15.

Fig. 1 a The plot of the normalized thermal expansion coefficient α (horizontal axis) against height z (vertical axis).

Fig. 1 Plot of electrical and thermal conductivities after treatment as a function of (a) applied current density at 750 °C and (b) applied treatment temperature at 150 A cm−2. c Current density and temperature as functions of layer number (SWCNT amount, one layer = ~3 mg).

Figure 3 Arrhenius plot of effective rates of thermal electron emission from the s- and p-states calculated on the basis of Eqs.

The plot of surface roughness versus thermal annealing temperatures is shown in Fig. 8.

Open image in new window Figure 12 Contour plot of the full bridge under thermal loading.

In crystal lattice around R617, both chain B and D have fewer contacts to neighboring molecules than chain A or C. A thermal factor plot of all four chains showed chain B and D have much higher B factors than that of chain A and C in that region (Fig. 4D).