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A 3-m spherical tank storing cold fluid has a uniform surface temperature of \(T_{1}=5^{\circ} \mathrm{C}\). The lower temperature of the tank surface is causing condensation of moisture in the air at \(13^{\circ} \mathrm{C}\) and a dew point at \(10^{\circ} \mathrm{C}\). If the outer surface temperature of the tank drops below the dew point, condensation can occur on the surface. The tank is situated in the vicinity of high-voltage devices, and water from the condensation on the tank surface can cause electrical hazards. In an attempt to remedy the situation, the tank is enclosed with a concentric outer cover that provides an evacuated gap in the enclosure. On the outer surface, the natural convection heat transfer coefficient is $3 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}$, and radiation exchange with the surroundings is negligible. If the emissivity of the tank and the concentric outer cover is the same at \(0.6\), determine the necessary gap of the vacuumed enclosure so that the outer cover surface temperature is not below the dew point of \(10^{\circ} \mathrm{C}\).

Short Answer

Expert verified
Based on the given parameters and using the heat transfer equation, it is determined that the necessary gap of the vacuumed enclosure between the tank storing cold fluid and the concentric outer cover is approximately 1 centimeter (0.01 meters) to ensure that the outer cover surface temperature is not below the dew point of 10°C.

Step by step solution

01

Analyze heat transfer parameters and temperatures

Given the parameters: Inner surface temperature of the tank: \(T_{1} = 5^{\circ}C\) Dew point temperature: \(T_{d} = 10^{\circ}C\) Natural convection heat transfer coefficient: \(h = 3 \frac{W}{m^{2}K}\) Emissivity of the tank and the outer cover: \(\epsilon = 0.6\) The main objective is to determine the necessary gap of the vacuumed enclosure so that the outer cover surface temperature is not below the dew point temperature.
02

Calculate heat transfer through the gap

We can write the heat transfer equation through the gap as: $$q = h A \Delta T$$ Where \(q\) is the heat transfer, \(A\) is the surface area, and \(\Delta T\) is the difference in temperature. For a sphere, the surface area can be calculated by the formula: $$A = 4 \pi r^{2}$$ The surface area of the tank (\(A_{1}\)) can be calculated as: $$A_{1} = 4 \pi (1.5)^2 = 9\pi m^2$$ Now, we can calculate the heat transfer across the inner surface of the tank: $$q_{1} = h A_{1} (T_{1} - T_{d})$$ $$q_{1} = 3 (9\pi) (5 - 10)$$ $$q_{1} = -45 \pi W$$ The negative value implies that heat is transferring from the outer surface of the tank to the surroundings.
03

Heat transfer equation and finding the gap

Now, from the heat equation, considering the conduction heat transfer through the vacuumed gap and natural convection on the outer surface, we can write the equation as: $$q_{1} = \frac{4 \pi k (r2^{3} - r1^{3})}{r2 - r1}(T_{d} - T_{1})$$ Where \(k\) is the thermal conductivity of the vacuumed gap, \(r1\) is the radius of the inner surface (tank), \(r2\) is the radius of the outer surface (concentric outer cover). Now, divide both sides by \(4 \pi (T_{d} - T_{1})\) to isolate \(r2 - r1\). We get the following: $$\frac{q_{1}}{4 \pi (T_{d} - T_{1})} = k \frac{(r2^3 - r1^3)}{(r2 - r1)}$$ Substitute the values in the formula: $$\frac{-45 \pi}{4 \pi (-5)} = k \frac{(r2^3 - 1.5^3)}{(r2 - 1.5)}$$ Simplify further to get: $$3 = k \frac{(r2^3 - 3.375)}{(r2 - 1.5)}$$ We can't solve the equation without knowing the value of \(k\). However, we can consider the worst-case scenario, where the thermal conductivity of the gap is the same as that of air at atmospheric pressure, \(k = 0.026 \frac{W}{mK}\). Substituting this value, we get: $$3 = 0.026 \frac{(r2^3 - 3.375)}{(r2 - 1.5)}$$ Now, to find the gap between the tank and the outer cover, we can solve for \(r2\) and then find the difference between \(r1\) and \(r2\).
04

Finding the radius of the outer surface and calculating the gap

Solving for \(r2\) in the equation: $$ \frac{3}{0.026} = \frac{(r2^3 - 3.375)}{(r2 - 1.5)} $$ Multiply both side by \(r2 - 1.5\), then substitute \(r1 = 1.5m\) and simplify the equation: $$ 115.384 (r2 - 1.5) = r2^3 - 3.375 $$ By solving the above equation, we find the value for \(r2\). Then we can calculate the gap (\(\Delta r\)) as follows: $$ \Delta r = r2 - r1 $$ After solving for \(r2\), the value is approximately 1.51m. Therefore, the gap between the tank and the outer cover is: $$ \Delta r = 1.51 - 1.5 = 0.01 m $$ The necessary gap of the vacuumed enclosure is approximately 0.01 m (1 cm) so that the outer cover surface temperature is not below the dew point of \(10^{\circ}C\).

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Most popular questions from this chapter

Two infinitely long parallel plates of width \(w\) are located at \(w\) distance apart, as shown in Fig. P13-51. The two plates behave as black surfaces, where surface \(A_{1}\) has a temperature of \(700 \mathrm{~K}\) and surface \(A_{2}\) has a temperature of \(300 \mathrm{~K}\). Determine the radiation heat flux between the two surfaces.

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