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The temperature distribution along the boundary layer increases with increasing thermal dispersion parameter.
From Figure 3, it is clear that interfacial thickness increases with increasing thermal motion.
In Figure 8(a) the skin friction coefficient increases with increasing thermal radiation K and decreases with increasing velocity slip factor, which is expected on a lubricated surface.
Because the expression Bolmatov et al. derive for C V, based on their phonon theory, also contains the thermal expansion coefficient (in fact, their C V increases with increasing thermal expansion), the calculation or modeling of the latter may offer a theoretical approach to c P. At least from the perspective of molecular computer simulation, thermal expansion appears to be the simpler quantity.
The obtained crystallite sizes as function of the thermally decomposed temperature for the samples with 0 ≤ x ≤ 0.5 are listed in Table 1and also displayed in Fig. 2. It is clearly seen that the crystallite size increases with increasing thermal decomposition temperature and decreases with the increase of Sr content.
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Ti4+ peak increased with increasing thermal oxidation time.
Nuclease stability of ORNs increased with increasing thermal stability of the duplex formed.
It is, however, increased with increasing thermal fluctuations for relatively low mean initial temperature resulting from a longer overall ignition delay of the mixture.
This high concentration of N2 is mainly derived from Cambria Ordovician shale carbonates at mature and highly mature stages, and the N2 contents tend to increase with increasing thermal stress.
It can be seen that the temperature increases with increasing pin length, while it decreases with increasing thermal length characteristic parameter.
In general, the mean heat release rate increases more slowly with increasing thermal stratification regardless of the mean initial temperature.
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