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)
| Parameter | Valid Range | Check 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.