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A person's head can be approximated as a 25-cm diameter sphere at \(35^{\circ} \mathrm{C}\) with an emissivity of \(0.95\). Heat is lost from the head to the surrounding air at \(25^{\circ} \mathrm{C}\) by convection with a heat transfer coefficient of \(11 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\), and by radiation to the surrounding surfaces at \(10^{\circ} \mathrm{C}\). Disregarding the neck, determine the total rate of heat loss from the head. (a) \(22 \mathrm{~W}\) (b) \(27 \mathrm{~W}\) (c) \(49 \mathrm{~W}\) (d) \(172 \mathrm{~W}\) (e) \(249 \mathrm{~W}\)

Short Answer

Expert verified
Answer: (b) 27 W

Step by step solution

01

Calculate the surface area of the head.

First, we need to find the surface area of the head, which is approximated as a sphere. The formula for the surface area of a sphere is \(A = 4\pi r^2\), where \(r\) is the radius of the sphere. Since the diameter is given as 25 cm, we can find the radius by dividing the diameter by 2: \(r = \frac{25}{2} = 12.5 \, \mathrm{cm}\). Now, convert the radius to meters: \(r = 0.125 \, \mathrm{m}\). Calculate the surface area \(A\): \(A = 4\pi (0.125)^2 \approx 0.196 \, \mathrm{m}^2\).
02

Calculate the heat loss due to convection.

Now, we will determine the rate of heat loss due to convection. The formula for heat loss due to convection is \(Q_{conv} = hA(T_{head} - T_{air})\), where \(h\) is the heat transfer coefficient, \(A\) is the surface area, \(T_{head}\) is the temperature of the head, and \(T_{air}\) is the temperature of the surrounding air. Given the heat transfer coefficient \(h=11 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\), \(T_{head} = 35^{\circ} \mathrm{C}=308.15\mathrm{~K}\), and \(T_{air} = 25^{\circ} \mathrm{C}=298.15\mathrm{~K}\). Using these values, we can calculate the heat loss due to convection: \(Q_{conv} = 11 (0.196)(308.15-298.15) \approx 22 \, \mathrm{W}\).
03

Calculate the heat loss due to radiation.

Next, we will determine the rate of heat loss due to radiation. The formula for heat loss due to radiation is \(Q_{rad} = \epsilon \sigma A (T_{head}^4 - T_{surfaces}^4)\), where \(\epsilon\) is the emissivity, \(\sigma\) is the Stefan-Boltzmann constant \((5.67 \times 10^{-8} \,\mathrm{W}/\mathrm{m}^2 \cdot \mathrm{K}^4)\), \(A\) is the surface area, \(T_{head}\) is the temperature of the head, and \(T_{surfaces}\) is the temperature of the surrounding surfaces. Given the emissivity \(\epsilon=0.95\), \(T_{head}=308.15\mathrm{~K}\), and \(T_{surfaces}=283.15\mathrm{~K}\) (since \(10^{\circ} \mathrm{C}=283.15\mathrm{~K}\)). Using these values, we can calculate the heat loss due to radiation: \(Q_{rad} = 0.95(5.67 \times 10^{-8})(0.196)(308.15^4 - 283.15^4) \approx 5 \, \mathrm{W}\)
04

Calculate the total heat loss.

Finally, we will add the heat loss due to convection and radiation to find the total heat loss: \(Q_{total} = Q_{conv} + Q_{rad} = 22 \, \mathrm{W} + 5 \, \mathrm{W} = 27 \, \mathrm{W}\) So, the total rate of heat loss from the person's head is \(27 \, \mathrm{W}\). The correct answer is (b) \(27 \, \mathrm{W}\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Convection Heat Transfer
One of the primary ways that the human body loses heat to its surroundings is through convection heat transfer. This is the process by which heat is carried away by the movement of fluids, which in most cases involves the air surrounding the body. Imagine it like a gentle breeze that passes over your skin and removes some of the warmth.

The rate of convection heat loss can be calculated using the formula:
\[Q_{conv} = hA(T_{body} - T_{air})\]
In this equation, \(Q_{conv}\) represents the heat lost due to convection, \(h\) is the heat transfer coefficient that describes how well heat is transferred from the body to the air, \(A\) is the surface area of the body part losing heat, and \(T_{body} - T_{air}\) is the temperature difference between the body and the surrounding air.

For the body's head approximated as a sphere, this convection process can have significant impact on how warm you stay, especially on cold or windy days, where convection can increase and enhance heat loss.
Radiation Heat Transfer
Apart from the loss of heat through convection, our bodies also lose heat through radiation heat transfer. This type of heat transfer doesn't rely on any medium but occurs through the emission of infrared radiation. All objects, including the human body, emit some form of thermal radiation depending on their temperature.

The formula for this radiative heat loss is expressed as:
\[Q_{rad} = \[epsilon\] \[\sigma\] A (T_{body}^4 - T_{surroundings}^4)\]
Here, \(Q_{rad}\) is the heat lost through radiation, \(\epsilon\) is the emissivity of the body part (a measure of how effectively it emits heat radiation), \(\sigma\) represents the Stefan-Boltzmann constant, \(A\) stands for the surface area, and the difference in temperatures to the fourth power, \(T_{body}^4 - T_{surroundings}^4\), indicates how temperature differences affect radiant heat loss.

For humans, these radiative losses can be quite significant, and this is why we often feel colder when exposed to a cold environment even if the air is still.
Stefan-Boltzmann Constant
Central to the calculation of radiative heat transfer is the Stefan-Boltzmann constant, symbolized as \(\sigma\). It is a physical constant that plays a critical role in quantifying the total energy radiated per unit surface area of a black body per unit time.

The constant's value is approximately \(5.67 \times 10^{-8} \, \mathrm{W}/\mathrm{m}^2 \cdot \mathrm{K}^4\), and its significance in the formula for radiation heat transfer can't be overstated— it ensures that the power radiated by an object is proportional to the fourth power of its absolute temperature.

This factor is why radiative heat loss becomes more considerable for objects with higher temperatures, like the human body compared to the ambient surroundings— the warmer you are, the more heat you'll radiate away.
Spherical Surface Area Calculation
When assessing heat loss from a human head, we model it as a sphere to calculate the surface area, which is essential for both convection and radiation heat transfer calculations. The formula used to determine the surface area of any sphere is:
\[A = 4\pi r^2\]
where \(A\) symbolizes the area, \(\pi\) is the mathematical constant approximately equal to 3.14159, and \(r\) stands for the sphere's radius.

In the case of convection and radiation heat loss, the surface area is directly proportional to the amount of heat that can escape from the object. For understanding heat loss in biological terms, this calculation helps us to predict how changes in head size or shape can influence the body's thermal balance, making it a foundational concept in understanding thermal physiology and comfort.

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Most popular questions from this chapter

\(80^{\circ} \mathrm{C}\). Also, determine the convection heat transfer coefficients at the beginning and at the end of the heating process. 1-133 It is well known that wind makes the cold air feel much colder as a result of the wind chill effect that is due to the increase in the convection heat transfer coefficient with increasing air velocity. The wind chill effect is usually expressed in terms of the wind chill temperature (WCT), which is the apparent temperature felt by exposed skin. For outdoor air temperature of \(0^{\circ} \mathrm{C}\), for example, the wind chill temperature is \(-5^{\circ} \mathrm{C}\) at \(20 \mathrm{~km} / \mathrm{h}\) winds and \(-9^{\circ} \mathrm{C}\) at \(60 \mathrm{~km} / \mathrm{h}\) winds. That is, a person exposed to \(0^{\circ} \mathrm{C}\) windy air at \(20 \mathrm{~km} / \mathrm{h}\) will feel as cold as a person exposed to \(-5^{\circ} \mathrm{C}\) calm air (air motion under \(5 \mathrm{~km} / \mathrm{h}\) ). For heat transfer purposes, a standing man can be modeled as a 30 -cm- diameter, 170-cm-long vertical cylinder with both the top and bottom surfaces insulated and with the side surface at an average temperature of \(34^{\circ} \mathrm{C}\). For a convection heat transfer coefficient of \(15 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\), determine the rate of heat loss from this man by convection in still air at \(20^{\circ} \mathrm{C}\). What would your answer be if the convection heat transfer coefficient is increased to \(30 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\) as a result of winds? What is the wind chill temperature in this case?

While driving down a highway early in the evening, the air flow over an automobile establishes an overall heat transfer coefficient of \(18 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). The passenger cabin of this automobile exposes \(9 \mathrm{~m}^{2}\) of surface to the moving ambient air. On a day when the ambient temperature is \(33^{\circ} \mathrm{C}\), how much cooling must the air conditioning system supply to maintain a temperature of \(20^{\circ} \mathrm{C}\) in the passenger cabin? (a) \(670 \mathrm{~W}\) (b) \(1284 \mathrm{~W}\) (c) \(2106 \mathrm{~W}\) (d) \(2565 \mathrm{~W}\) (e) \(3210 \mathrm{~W}\)

An aluminum pan whose thermal conductivity is \(237 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\) has a flat bottom with diameter \(15 \mathrm{~cm}\) and thickness \(0.4 \mathrm{~cm}\). Heat is transferred steadily to boiling water in the pan through its bottom at a rate of \(1400 \mathrm{~W}\). If the inner surface of the bottom of the pan is at \(105^{\circ} \mathrm{C}\), determine the temperature of the outer surface of the bottom of the pan.

What is the value of the engineering software packages in ( \(a\) ) engineering education and \((b)\) engineering practice?

Consider a house in Atlanta, Georgia, that is maintained at \(22^{\circ} \mathrm{C}\) and has a total of \(20 \mathrm{~m}^{2}\) of window area. The windows are double-door type with wood frames and metal spacers and have a \(U\)-factor of \(2.5 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\) (see Prob. 1-125 for the definition of \(U\)-factor). The winter average temperature of Atlanta is \(11.3^{\circ} \mathrm{C}\). Determine the average rate of heat loss through the windows in winter.

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