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in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 1 Physical model CNT nanofluid stagnation flow regime More about this image found in Physical model CNT nanofluid stagnation flow regime
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 2 Comparison of dimensionless velocity f ′( η ) More about this image found in Comparison of dimensionless velocity f ′( η )
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 3 Comparison of dimensionless temperature θ ( η ) More about this image found in Comparison of dimensionless temperature θ ( η )
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 4 Effects of melting parameter ( M ) on dimensionless skin friction coefficient f ″(0) of water-based SWCNT nanofluid as a function of stretching parameter ( ε ) when Pr = 6.2 and φ = 0.2 More about this image found in Effects of melting parameter ( M ) on dimensionless skin friction coefficie...
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 5 Effects of melting parameter ( M ) on dimensionless skin friction coefficient f ″(0) of water-based MWCNT nanofluid as a function of stretching parameter ( ε ) when Pr = 6.2 and φ = 0.2 More about this image found in Effects of melting parameter ( M ) on dimensionless skin friction coefficie...
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 6 Effects of melting parameter ( M ) on dimensionless skin friction coefficient f ″(0) of kerosene oil-based SWCNT nanofluid as a function of stretching parameter ( ε ) when Pr = 21 and φ = 0.2 More about this image found in Effects of melting parameter ( M ) on dimensionless skin friction coefficie...
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 7 Effects of melting parameter ( M ) on dimensionless skin friction coefficient f ″(0) of kerosene oil-based MWCNT nanofluid as a function of stretching parameter ( ε ) when Pr = 21 and φ = 0.2 More about this image found in Effects of melting parameter ( M ) on dimensionless skin friction coefficie...
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 8 Effects of nanoparticle volume fraction ( φ ) on dimensionless skin friction coefficient f ″(0) of water-based SWCNT as a function of stretching parameter ( ε ) when Pr = 6.2 and M = 1 More about this image found in Effects of nanoparticle volume fraction ( φ ) on dimensionless skin frictio...
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 9 Effects of nanoparticle volume fraction ( φ ) on dimensionless skin friction coefficient f ″(0) of water-based MWCNT as a function of stretching parameter ( ε ) when Pr = 6.2 and M = 1 More about this image found in Effects of nanoparticle volume fraction ( φ ) on dimensionless skin frictio...
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 10 Effects of nanoparticle volume fraction ( φ ) on dimensionless skin friction coefficient f ″(0) of kerosene-based SWCNT nanofluid as function of stretching parameter ( ε ) for Pr = 21 and M = 1 More about this image found in Effects of nanoparticle volume fraction ( φ ) on dimensionless skin frictio...
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 11 Effects of nanoparticle volume fraction ( φ ) on dimensionless skin friction coefficient f ″(0) of kerosene-based MWCNT nanofluid as function of stretching parameter ( ε ) for Pr = 21 and M = 1 More about this image found in Effects of nanoparticle volume fraction ( φ ) on dimensionless skin frictio...
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 12 Effects of melting parameter ( M ) on dimensionless heat transfer − θ ′(0) of water-based SWCNT nanofluid as a function of stretching parameter ( ε ) when Pr = 6.2 and φ = 0.2 More about this image found in Effects of melting parameter ( M ) on dimensionless heat transfer − θ ′(0) ...
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 13 Effects of melting parameter ( M ) on dimensionless heat transfer − θ ′(0) of water-based MWCNT nanofluid as a function of stretching parameter ( ε ) when Pr = 6.2 and φ = 0.2 More about this image found in Effects of melting parameter ( M ) on dimensionless heat transfer − θ ′(0) ...
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 14 Effects of melting parameter ( M ) on dimensionless heat transfer − θ ′(0) of kerosene-based SWCNT nanofluid as a function of stretching parameter ( ε ) when Pr = 21 and φ = 0.2 More about this image found in Effects of melting parameter ( M ) on dimensionless heat transfer − θ ′(0) ...
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 15 Effects of melting parameter ( M ) on dimensionless heat transfer − θ ′(0) of kerosene-based MWCNT nanofluid as a function of stretching parameter ( ε ) when Pr = 21 and φ = 0.2 More about this image found in Effects of melting parameter ( M ) on dimensionless heat transfer − θ ′(0) ...
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 16 Effects of nanoparticle volume fraction φ on dimensionless heat transfer − θ ′(0) of water-based SWCNT nanofluid as a function of stretching parameter ( ε ) when Pr = 6.2 and M = 1 More about this image found in Effects of nanoparticle volume fraction φ on dimensionless heat transfer ...
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 17 Effects of nanoparticle volume fraction φ on dimensionless heat transfer − θ ′(0) of water-based MWCNT nanofluid as a function of stretching parameter ( ε ) when Pr = 6.2 and M = 1 More about this image found in Effects of nanoparticle volume fraction φ on dimensionless heat transfer ...
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 18 Effects of nanoparticle volume fraction φ on dimensionless heat transfer − θ ′(0) of kerosene-based SWCNT nanofluid as a function of stretching parameter ( ε ) when Pr = 6.2 and M = 1 More about this image found in Effects of nanoparticle volume fraction φ on dimensionless heat transfer ...
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 19 Effects of nanoparticle volume fraction φ on dimensionless heat transfer − θ ′(0) of kerosene-based MWCNT as a function of stretching parameter ( ε ) when Pr = 6.2 and M = 1 More about this image found in Effects of nanoparticle volume fraction φ on dimensionless heat transfer ...
Image
in Computation of Stagnation Point Convection Flow of Carbon Nanotube Nanofluids From a Stretching Sheet With Melting: Dual Solutions
> ASME Open Journal of Engineering
Published Online: November 6, 2023
Fig. 20 Effect of various melting parameter ( M ) on velocity profile, f ′( η ) water-based CNT nanofluids More about this image found in Effect of various melting parameter ( M ) on velocity profile, f ′( η ) wa...
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