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Question 12.8: Water Flow Inside Tubes* The internal convective heat transf......

Water Flow Inside Tubes*

The internal convective heat transfer coefficient is to be computed for conditions when water at a temperature of 10°C with a velocity of 2.5 m/s flows through a tube with 8 mm internal diameter. These conditions are common in the water side of the evaporator of a refrigeration system.
Given: v = 2.5 m/s, characteristic length D = 8 mm
Find: h_{con} using Equation 12.20 for cooling condition
Lookup values: From property tables of water, \rho = 1000  kg/m³, \mu = 0.00131  Pa · s, c_{p} = 4190  J/(kg · K), k = 0.573  W/(m·K)

N uD_{D} = 0.023 Re_{D}^{0.8}Pr^{n}          (12.20)

n = 0.4 heating

n = 0.3 cooling

* Same inputs as Example 2.11 that was solved using a dimensional correlation.

Step-by-Step
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First, the Reynolds number is determined from Equation 12.14 as

Re = \frac{\rho v D}{\mu} = \frac{1000  kg/m^{3} \times 2.5  m/s \times 0.008   m}{0.00131  Pa \cdot s}

= 15,267

The flow is clearly turbulent.
Next, the Prandtl number is computed from Equation 12.15 as follows:

P r = \frac{\mu c_{p}}{k}               (12.15)

Pr = \frac{4190  J/kg \times 0.00131  Pa \cdot s}{0.573  W/(m \cdot K)} = 9.6

We then use Equation 12.20 with n = 0.3 to find

Nu_{D} = 0.023 \times 15,267^{0.8} \times 9.6^{0.3} = 100.8

from which the convective heat transfer coefficient is deduced from Equation 12.16 as

Nu = \frac{h_{con} D}{k}               (12.16)

h_{con} = \frac{0.573  W/(m \cdot K) \times 100.8 }{0.008  m} = 7220  W/(m^{2} \cdot K)

Comments
This example is identical to Example 2.11 that was solved using simplied dimensional equations.
In that case, h_{con} = 5171  W/(m6{2} K), which is about a 25% difference from the value found using the more accurate dimensionless equation.

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