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Water is boiling in a 12 -cm-deep pan with an outer diameter of $25 \mathrm{~cm}$ that is placed on top of a stove. The ambient air and the surrounding surfaces are at a temperature of \(25^{\circ} \mathrm{C}\), and the emissivity of the outer surface of the pan is \(0.80\). Assuming the entire pan to be at an average temperature of \(98^{\circ} \mathrm{C}\), determine the rate of heat loss from the cylindrical side surface of the pan to the surroundings by \((a)\) natural convection and \((b)\) radiation. (c) If water is boiling at a rate of \(1.5\) \(\mathrm{kg} / \mathrm{h}\) at \(100^{\circ} \mathrm{C}\), determine the ratio of the heat lost from the side surfaces of the pan to that by the evaporation of water. The enthalpy of vaporization of water at \(100^{\circ} \mathrm{C}\) is 2257 \(\mathrm{kJ} / \mathrm{kg}\). Answers: $46.2 \mathrm{~W}, 47.3 \mathrm{~W}, 0.099$

Short Answer

Expert verified
Short Answer: The heat loss from the cylindrical side surface of the boiling pan due to convection is 46.2 W, and due to radiation is 47.3 W. The ratio of the total heat loss from the side surfaces to the heat loss by evaporation of water is 0.099.

Step by step solution

01

(Step 1: Find the convective heat transfer coefficient (hc))

As given, Outer diameter of pan (D) = 25 cm = 0.25 m Height of pan (H) = 12 cm = 0.12 m Pan Temperature (Ts) = 98 °C = 371 K Ambient Temperature (T∞ ) = 25 °C = 298 K The constant properties of air at a film temperature \((T_s+T_\infty) / 2\) = 334.5 K are: k = 0.0262 W/(m⋅K) ν = 15.89 × \(10^{-6} \mathrm{m^2/s}\) Pr = 0.708 First, we find the Grashof (Gr) and Rayleigh (Ra) numbers: \(\mathrm{Gr} = \frac{g \cdot \beta \cdot (T_s - T_\infty) \cdot D^3}{\nu^2} \) \(\mathrm{Ra} = \mathrm{Gr} \cdot \mathrm{Pr}\) By knowing the Rayleigh number, we can find the convective heat transfer coefficient (hc). For laminar flow (Ra\(_{D} \leq 10^9\)), \( h_c = 0.15(\mathrm{Ra}_D)^{1/3} \cdot \frac{k}{D} \) For turbulent flow (Ra\(_{D} > 10^9\)), \( h_c = 0.10(\mathrm{Ra}_D)^{1/3} \cdot \frac{k}{D} \)
02

(Step 2: Calculate convective heat loss (Qconv))

To calculate convective heat loss (Qconv), we need the convective heat transfer coefficient (hc) and the area of the cylindrical side surface (Ac). \(A_c = \pi D H\) Now apply the formula for Qconv: \(Q_{conv} = h_c A_c (T_s - T_\infty)\)
03

(Step 3: Calculate radiative heat loss (Qrad))

For the radiative heat loss, we need the emissivity (ε), the Stefan-Boltzmann constant (σ), and the area of the cylindrical side surface (Ar). The emissivity is given as 0.80, and Ar is equal to Ac. The Stefan-Boltzmann constant is \(5.67 \times 10^{-8} \mathrm{W/(m^2 K^4)}\). Now apply the formula for Qrad: \(Q_{rad} = \epsilon \sigma A_r (T_s^4 - T_\infty^4)\)
04

(Step 4: Find the heat loss due to evaporation of water)

We are given the rate of evaporation of water (1.5 kg/h) and the enthalpy of vaporization (2257 kJ/kg). \(\dot{m} = 1.5\,\text{kg/h} = \frac{1.5}{3600}\,\text{kg/s}\) \(h_v = 2257\,\text{kJ/kg} = 2257\times10^3\,\text{J/kg}\) Now apply the formula for Qevap: \(Q_{evap} = \dot{m}h_v\)
05

(Step 5: Compute the ratio of heat lost from side surfaces to that by evaporation)

Now that we have calculated Qconv, Qrad, and Qevap, we can calculate the requested ratio using the formula: \(\frac{Q_{conv}+Q_{rad}}{Q_{evap}}\) By performing the calculations, we get: a) Qconv = 46.2 W b) Qrad = 47.3 W c) Ratio of heat loss = 0.099

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Most popular questions from this chapter

When is natural convection negligible and when is it not negligible in forced convection heat transfer?

A hot liquid $\left(c_{p}=1000 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\right)\( flows at a flow rate of \)0.05 \mathrm{~kg} / \mathrm{s}$ inside a copper pipe with an inner diameter of \(45 \mathrm{~mm}\) and a wall thickness of \(5 \mathrm{~mm}\). At the pipe exit, the liquid temperature decreases by \(10^{\circ} \mathrm{C}\) from its temperature at the inlet. The outer surface of the \(5-\mathrm{m}\)-long copper pipe is black oxidized, which subjects the outer surface to radiation heat transfer. The air temperature surrounding the pipe is \(10^{\circ} \mathrm{C}\). Assuming that the properties of air can be evaluated at \(35^{\circ} \mathrm{C}\) and \(1 \mathrm{~atm}\) pressure, determine the outer surface temperature of the pipe. Is $35^{\circ} \mathrm{C}$ an appropriate film temperature for evaluation of the air properties?

Consider a vertical plate with length \(L\), placed in quiescent air. If the film temperature is \(20^{\circ} \mathrm{C}\) and the average Nusselt number in natural convection is of the form \(\mathrm{Nu}=\mathrm{CRa}_{L}^{n}\), show that the average heat transfer coefficient can be expressed as $$ \begin{aligned} h &=1.51(\Delta T / L)^{1 / 4} \quad 10^{4}<\mathrm{Ra}_{L}<10^{9} \\ h &=1.19 \Delta T^{1 / 3} \quad 10^{10}<\mathrm{Ra}_{L}<10^{13} \end{aligned} $$

Skylights or "roof windows" are commonly used in homes and manufacturing facilities since they let natural light in during daytime and thus reduce the lighting costs. However, they offer little resistance to heat transfer, and large amounts of energy are lost through them in winter unless they are equipped with a motorized insulating cover that can be used in cold weather and at nights to reduce heat losses. Consider a \(1-\mathrm{m}\)-wide and \(2.5\)-m-long horizontal skylight on the roof of a house that is kept at \(20^{\circ} \mathrm{C}\). The glazing of the skylight is made of a single layer of \(0.5-\mathrm{cm}\)-thick glass $(k=0.78 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\( and \)\varepsilon=0.9$ ). Determine the rate of heat loss through the skylight when the air temperature outside is \(-10^{\circ} \mathrm{C}\) and the effective sky temperature is \(-30^{\circ} \mathrm{C}\). Compare your result with the rate of heat loss through an equivalent surface area of the roof that has a common \(R-5.34\) construction in SI units (i.e., a thickness-to- effective-thermal-conductivity ratio of $5.34 \mathrm{~m}^{2} . \mathrm{K} / \mathrm{W}\( ). Evaluate air properties at a film temperature of \)-7^{\circ} \mathrm{C}\( and \)1 \mathrm{~atm}$ pressure. Is this a good assumption?

Thick fluids such as asphalt and waxes and the pipes in which they flow are often heated in order to reduce the viscosity of the fluids and thus to reduce the pumping costs. Consider the flow of such a fluid through a \(100-\mathrm{m}\)-long pipe of outer diameter \(30 \mathrm{~cm}\) in calm, ambient air at \(0^{\circ} \mathrm{C}\). The pipe is heated electrically, and a thermostat keeps the outer surface temperature of the pipe constant at \(25^{\circ} \mathrm{C}\). The emissivity of the outer surface of the pipe is \(0.8\), and the effective sky temperature is \(-30^{\circ} \mathrm{C}\). Determine the power rating of the electric resistance heater, in \(\mathrm{kW}\), that needs to be used. Also, determine the cost of electricity associated with heating the pipe during a 15-h period under the above conditions if the price of electricity is \(\$ 0.09 / \mathrm{kWh}\). Answers: \(29.1 \mathrm{~kW}, \$ 39.30\)

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