Table 4 Comparison of \({f}^{\prime\prime} (\infty , {0}\text{)}\) and \(-\theta (\infty ,0)\) at \(\varepsilon =\phi ={N}_{R}=0\) for different Prandtl number values.
From: Thermal radiation effects on nanofluid flow over a vertical cone in the presence of pressure work
\(f^{{\prime}{\prime}}(0,\infty )\) | \(-\theta ^{\prime}(0,\infty )\) | ||||||||
|---|---|---|---|---|---|---|---|---|---|
\(\text{Pr}\) | Hering and Grosh15 | Roy14 | Present results | Na37 | Hering and Grosh15 | Roy14 | Alamgir41 | Na and Chiou38 | Present results |
0.1 | 1.0960 | – | 1.0958 | 0.2113 | – | 0.2141 | – | 0.2113 | 0.21132 |
1.0 | 0.7694 | 0.8600 | 0.7694 | 0.5104 | 0.5275 | 0.5280 | 0.5104 | 0.5104 | 0.51045 |
10 | – | 0.4899 | 0.4876 | – | 1.0354 | 1.0159 | 1.0340 | – | 1.03397 |
