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Atmospheric air with a velocity of \(10 \mathrm{~m} / \mathrm{s}\) and a temperature of \(20^{\circ} \mathrm{C}\) is in parallel flow over a flat heater surface which is maintained at \(80^{\circ} \mathrm{C}\). The surface area of the heater is \(0.30 \mathrm{~m}^{2}\). The drag force induced by the airflow on the heater is measured to be \(0.2 \mathrm{~N}\). Using the momentum-heat transfer analogy, determine the electrical power needed to maintain the prescribed heater surface temperature of \(80^{\circ} \mathrm{C}\). Evaluate the air properties at \(50^{\circ} \mathrm{C}\) and \(1 \mathrm{~atm}\).

Short Answer

Expert verified
Answer: The electrical power needed to maintain the heater surface temperature at 80°C is approximately 1007.65 W.

Step by step solution

01

Find the Reynolds number of the flow

First, let's find the Reynolds number (\(Re\)) of the flow based on the air properties at \(50^{\circ} \mathrm{C}\) and \(1 \mathrm{~atm}\): At these conditions, the dynamic viscosity of air, \(\mu\), is around \(1.9 \times 10^{-5} \mathrm{~kg/m.s}\). The density of air, \(\rho\), is about \(1.15 \mathrm{~kg/m^3}\). We can calculate the Reynolds number using the formula: \(Re = \frac{\rho v L}{\mu}\) Assuming the heat transfer length, \(L\), equals the largest length of the heater, we get: \(Re = \frac{1.15 \times 10 \times 0.3}{1.9 \times 10^{-5}} \approx 1.81 \times 10^4\)
02

Calculate Nusselt number using Reynolds number

We will use the Sieder-Tate (or Prandtl number, \(Pr\)), which is about \(0.72\) at \(50^{\circ} \mathrm{C}\). The Nusselt number (\(Nu\)) can be calculated using the formula: \(Nu = 0.023 Re^{0.8} Pr^{0.3} \approx 0.023 \times (1.81 \times 10^4)^{0.8} \times 0.72^{0.3} \approx 158.31\)
03

Calculate heat transfer coefficient

Now we can determine the heat transfer coefficient (\(h \)) using the Nusselt number and the thermal conductivity (\(k\)) of air (around \(0.028 \mathrm{~W/m.K}\) at \(50^{\circ} \mathrm{C}\)) using the formula: \(h = \frac{Nu \times k}{L} \approx \frac{158.31 \times 0.028}{0.3} \approx 14.74 \mathrm{~W/m^2.K}\)
04

Use the momentum-heat transfer analogy to find the heat transfer rate

The momentum-heat transfer analogy states that, for flat-plate boundary layer flows under constant heat flux, the friction force (\(F\)) is proportional to the heat transfer rate (\(q\)). \(F = \frac{1}{2}\rho v^{2}AC_f\) The electrical power needed to maintain the prescribed heater surface temperature of \(80^{\circ} \mathrm{C}\) can be determined using: \(q = hA(T_{heater}-T_{air})\) Solve for the heat transfer coefficient in terms of the drag force and substitute into the second equation to find the power required. \(h = \frac{2F}{v^{2}AC_f}\) Therefore, \(q = \frac{2F}{v^{2}AC_f}A(T_{heater}-T_{air})\)
05

Calculate the electrical power needed

Using the known values, we can now determine the electrical power needed to maintain the heater surface temperature: \(q = \frac{2\times0.2}{(10)^{2}\times 0.30\times 0.00574}\times 0.30\times (80-20) \approx 1007.65 \mathrm{~W}\) So, the electrical power needed to maintain the heater surface temperature at \(80^{\circ} \mathrm{C}\) is approximately \(1007.65 \mathrm{~W}\).

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Most popular questions from this chapter

A ball bearing manufacturing plant is using air to cool chromium steel balls \((k=40 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\). The convection heat transfer coefficient for the cooling is determined experimentally as a function of air velocity to be \(h=18.05 \mathrm{~V}^{0.56}\), where \(h\) and \(V\) are in \(\mathrm{W} / \mathrm{m}^{2}, \mathrm{~K}\) and $\mathrm{m} / \mathrm{s}$, respectively. At a given moment during the cooling process with the air temperature at \(5^{\circ} \mathrm{C}\), a chromium steel ball has a surface temperature of \(450^{\circ} \mathrm{C}\). Using appropriate software, determine the effect of the air velocity \((V)\) on the temperature gradient in the chromium steel ball at the surface. By varying the air velocity from \(0.2\) to \(2.4 \mathrm{~m} / \mathrm{s}\) with increments of $0.2 \mathrm{~m} / \mathrm{s}$, plot the temperature gradient in the chromium steel ball at the surface as a function of air velocity.

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