Introduction & Context

The calculation determines the cooling-water requirement for a dough-kneading jacket and evaluates the heat-transfer capability of a parallel-flow two-phase (air/silicone) tube. In process engineering these calculations are essential for:

  • Sizing cooling-water pumps and ensuring adequate temperature control of the dough.
  • Verifying that the jacket operates in the turbulent regime where the Dittus-Boelter correlation is valid.
  • Assessing the combined convective performance of a gas–liquid mixture inside heat-exchange tubes.

Typical applications include bakery process lines, continuous mixers, and any thermal-controlled kneading operation where the dough temperature must be raised or held within a narrow band while removing excess heat.

Methodology & Formulas

1. Dough heat load

The rate of heat that must be supplied to the dough is obtained from the sensible-heat balance:

\[ Q = \dot m_{d}\,C_{p,d}\,\Delta T_{d} \]

where \(\Delta T_{d}=T_{d,\text{out}}-T_{d,\text{in}}\).

2. Required cooling-water flow (single-phase)

The water mass flow that can absorb the dough heat load is:

\[ \dot m_{w}= \frac{Q}{C_{p,w}\,\Delta T_{w}} \]

with \(\Delta T_{w}=T_{w,\text{out}}-T_{w,\text{in}}\). The corresponding volumetric flow is:

\[ \dot V_{w}= \frac{\dot m_{w}}{\rho_{w}} \]

3. Jacket hydraulic and convective check (single-phase water)

Reynolds number for water flowing in the jacket:

\[ \text{Re}_{w}= \frac{\rho_{w}\,V_{w}\,D_{\text{jacket}}}{\mu_{w}} \]

Prandtl number for water:

\[ \text{Pr}_{w}= \frac{C_{p,w}\,\mu_{w}}{k_{w}} \]

Using the Dittus-Boelter correlation (valid for turbulent internal flow), the Nusselt number is:

\[ \text{Nu}_{w}=0.023\,\text{Re}_{w}^{0.8}\,\text{Pr}_{w}^{0.4} \]

and the convective heat-transfer coefficient becomes:

\[ h_{w}= \frac{\text{Nu}_{w}\,k_{w}}{D_{\text{jacket}}} \]

4. Two-phase (air/silicone) heat-transfer coefficients

Separate single-phase correlations are applied to the liquid (silicone) and gas (air) streams.

Liquid side

\[ \text{Re}_{l}= \frac{\rho_{l}\,V_{l}\,D_{\text{tube}}}{\mu_{l}},\qquad \text{Nu}_{l}=0.023\,\text{Re}_{l}^{0.8}\,\text{Pr}_{l}^{0.4},\qquad h_{l}= \frac{\text{Nu}_{l}\,k_{l}}{D_{\text{tube}}} \]

Gas side

\[ \text{Re}_{g}= \frac{\rho_{g}\,V_{g}\,D_{\text{tube}}}{\mu_{g}},\qquad \text{Nu}_{g}=0.023\,\text{Re}_{g}^{0.8}\,\text{Pr}_{g}^{0.4},\qquad h_{g}= \frac{\text{Nu}_{g}\,k_{g}}{D_{\text{tube}}} \]

The overall two-phase convective coefficient for parallel flow is obtained by harmonic averaging weighted by the void fraction \(\alpha\) (gas volume fraction):

\[ h_{\text{tp}}=\left[\,\frac{\alpha}{h_{g}}+\frac{1-\alpha}{h_{l}}\,\right]^{-1} \]

5. Validity checks (Dittus-Boelter applicability)

ParameterValid RangeCheck Condition
\(\text{Re}_{w}\)\(1\times10^{4}\) ≤ \(\text{Re}_{w}\) ≤ \(1\times10^{6}\)\(\text{Re}_{w}\) within turbulent regime
\(\text{Pr}_{w}\)\(0.7\) ≤ \(\text{Pr}_{w}\) ≤ \(160\)Prandtl number suitable for correlation
\(\text{Re}_{l}\)\(1\times10^{4}\) ≤ \(\text{Re}_{l}\) ≤ \(1\times10^{6}\)Liquid side turbulent
\(\text{Pr}_{l}\)\(0.7\) ≤ \(\text{Pr}_{l}\) ≤ \(160\)Liquid Prandtl range
\(\text{Re}_{g}\)\(1\times10^{4}\) ≤ \(\text{Re}_{g}\) ≤ \(1\times10^{6}\)Gas side turbulent
\(\text{Pr}_{g}\)\(0.7\) ≤ \(\text{Pr}_{g}\) ≤ \(160\)Gas Prandtl range

6. Use of the overall coefficient

If an external convection coefficient \(h_{\text{ext}}\) and wall resistance \(R_{\text{wall}}\) are known, the overall tube heat-transfer coefficient \(U\) can be assembled as:

\[ \frac{1}{U}= \frac{1}{h_{\text{tp}}}+R_{\text{wall}}+\frac{1}{h_{\text{ext}}} \]

This reference sheet provides the algebraic framework required to size cooling-water systems for dough kneading and to evaluate the combined convective performance of a gas-liquid heat-exchange tube.