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Table 5 Approximation of hydraulic results following the scheme \({c_{\text{opt}}}({\text{SDR}})= \frac{m}{{\text{SDR}}} +b\)

From: Net-exergetic, hydraulic and thermal optimization of coaxial heat exchangers using fixed flow conditions instead of fixed flow rates

Case

Parameters regression

Material

\({r_a}\)

Slope m

intercept b

RMSE

  

Laminar

0.5604

0.5367

0.0011

  

Turbulent

Plastic

\(r_{\min}\)

0.5996

0.6093

0.0010

\(r_{m}\)

0.5994

0.6093

0.0010

\(r_{\max}\)

0.5992

0.6093

0.0010

Steel

\(r_{\min}\)

0.6068

0.6105

0.0009

\(r_{m}\)

0.6081

0.6118

0.0009

\(r_{\max}\)

0.6099

0.6126

0.0010

Stand.

\(r_{\min}\)

0.5954

0.5639

0.0011

\(r_{m}\)

0.5935

0.5770

0.0010

\(r_{\max}\)

0.5927

0.5940

0.0010

Switch

\(r_{\min}\)

0.5959

0.6293

0.0009

\(r_{m}\)

0.5997

0.6274

0.0009

\(r_{\max}\)

0.6074

0.6226

0.0009

  

Turbulent rough regime

Plastic

\(r_{\min}\)

0.6092

0.6191

0.0009

\(r_{m}\)

0.6092

0.6193

0.0009

\(r_{\max}\)

0.6092

0.6198

0.0009

Steel

\(r_{\min}\)

0.6064

0.6109

0.0009

\(r_{m}\)

0.6073

0.6126

0.0009

\(r_{\max}\)

0.6082

0.6147

0.0009

Stand.

\(r_{\min}\)

0.6407

0.5238

0.0013

\(r_{m}\)

0.6414

0.5321

0.0013

\(r_{\max}\)

0.6412

0.5438

0.0012

Switch

\(r_{\min}\)

0.5933

0.6306

0.0009

\(r_{m}\)

0.5950

0.6298

0.0009

\(r_{\max}\)

0.5973

0.6288

0.0009