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Using the conversion factors between W and Btu/h, \(\mathrm{m}\) and \(\mathrm{ft}\), and \(\mathrm{K}\) and \(\mathrm{R}\), express the Stefan-Boltzmann constant $\sigma=5.67 \times 10^{-8} \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}^{4}\( in the English unit \)\mathrm{Btu} / \mathrm{h} \cdot \mathrm{ft}^{2} \cdot \mathrm{R}^{4}$.

Short Answer

Expert verified
Question: Convert the Stefan-Boltzmann constant from SI (W, m, K) units to English (Btu/h, ft, R) units. Answer: Approximately, 1.714 × 10^-9 Btu/h*ft^2*R^4.

Step by step solution

01

Convert W to Btu/h

Multiply the given Stefan-Boltzmann constant by the W to Btu/h conversion factor: \(\sigma = 5.67 \times 10^{-8} \frac{\mathrm{W}}{\mathrm{m}^2 \cdot \mathrm{K}^4} \cdot \frac{3.412142\, \mathrm{Btu/h}}{1\, \mathrm{W}}\)
02

Simplify and cancel W

Now we can simplify the expression by canceling out watts (W): \(\sigma = (5.67 \times 10^{-8}) \times (3.412142) \frac{\mathrm{Btu/h}}{\mathrm{m}^2 \cdot \mathrm{K}^4}\)
03

Convert m to ft

Multiply the expression by the m to ft conversion factor: \(\sigma = (5.67 \times 10^{-8}) \times (3.412142) \cdot \left( \frac{1\, \mathrm{m}}{3.28084\, \mathrm{ft}} \right)^2 \cdot \frac{\mathrm{Btu/h}}{\mathrm{ft}^2 \cdot \mathrm{K}^4}\)
04

Simplify and cancel m

Now we can simplify the expression by canceling out meters (m): \(\sigma = (5.67 \times 10^{-8}) \times (3.412142) \cdot \left( \frac{1}{3.28084} \right)^2 \frac{\mathrm{Btu/h}}{\mathrm{ft}^2 \cdot \mathrm{K}^4}\)
05

Convert K to R

Multiply the expression by the K to R conversion factor: \(\sigma = (5.67 \times 10^{-8}) \times (3.412142) \cdot \left( \frac{1}{3.28084} \right)^2 \cdot \left( \frac{1\,\mathrm{K}}{1.8\,\mathrm{R}} \right)^4 \frac{\mathrm{Btu/h}}{\mathrm{ft}^2 \cdot \mathrm{R}^4}\)
06

Simplify and cancel K

Now we can simplify the expression by canceling out Kelvin (K): \(\sigma = (5.67 \times 10^{-8}) \times (3.412142) \cdot \left( \frac{1}{3.28084} \right)^2 \cdot \left( \frac{1}{1.8} \right)^4 \frac{\mathrm{Btu/h}}{\mathrm{ft}^2 \cdot \mathrm{R}^4}\)
07

Calculate the final expression

Now we can calculate the final expression: \(\sigma = (5.67 \times 10^{-8}) \times (3.412142) \times \left( \frac{1}{3.28084} \right)^2 \times \left( \frac{1}{1.8} \right)^4 \frac{\mathrm{Btu/h}}{\mathrm{ft}^2 \cdot \mathrm{R}^4} \approx 1.714 \times 10^{-9} \, \frac{\mathrm{Btu/h}}{\mathrm{ft}^2 \cdot \mathrm{R}^4}\) So, the Stefan-Boltzmann constant in Btu/h, ft, and R is \(\sigma \approx 1.714 \times 10^{-9} \, \frac{\mathrm{Btu/h}}{\mathrm{ft}^2 \cdot \mathrm{R}^4}\).

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Most popular questions from this chapter

A hollow spherical iron container with outer diameter \(20 \mathrm{~cm}\) and thickness \(0.2 \mathrm{~cm}\) is filled with iced water at $0^{\circ} \mathrm{C}\(. If the outer surface temperature is \)5^{\circ} \mathrm{C}$, determine the approximate rate of heat gain by the iced water in \(\mathrm{kW}\) and the rate at which ice melts in the container. The heat of fusion of water is \(333.7 \mathrm{~kJ} / \mathrm{kg}\). Treat the spherical shell as a plain wall, and use the outer area.

Solar radiation is incident on a \(5-\mathrm{m}^{2}\) solar absorber plate surface at a rate of \(800 \mathrm{~W} / \mathrm{m}^{2}\). Ninety-three percent of the solar radiation is absorbed by the absorber plate, while the remaining 7 percent is reflected away. The solar absorber plate has a surface temperature of \(40^{\circ} \mathrm{C}\) with an emissivity of \(0.9\) that experiences radiation exchange with the surrounding temperature of $-5^{\circ} \mathrm{C}$. In addition, convective heat transfer occurs between the absorber plate surface and the ambient air of \(20^{\circ} \mathrm{C}\) with a convection heat transfer coefficient of \(7 \mathrm{~W} / \mathrm{m}^{2}\). \(\mathrm{K}\). Determine the efficiency of the solar absorber, which is defined as the ratio of the usable heat collected by the absorber to the incident solar radiation on the absorber.

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. 1-120 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.

The rate of heat loss through a unit surface area of a window per unit temperature difference between the indoors and the outdoors is called the \(U\)-factor. The value of the \(U\)-factor ranges from about $1.25 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\( (or \)0.22 \mathrm{Btw} / \mathrm{h} \cdot \mathrm{ft}^{2} \cdot{ }^{\circ} \mathrm{F}$ ) for low-e coated, argon-filled, quadruple-pane windows to \(6.25 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\) (or $1.1 \mathrm{Btu} / \mathrm{h} \cdot \mathrm{ft}^{2}{ }^{\circ} \mathrm{F}$ ) for a single-pane window with aluminum frames. Determine the range for the rate of heat loss through a $1.2-\mathrm{m} \times 1.8-\mathrm{m}\( window of a house that is maintained at \)20^{\circ} \mathrm{C}\( when the outdoor air temperature is \)-8^{\circ} \mathrm{C}$.

A cylindrical resistor element on a circuit board dissipates \(0.8 \mathrm{~W}\) of power. The resistor is \(2 \mathrm{~cm}\) long and has a diameter of $0.4 \mathrm{~cm}$. Assuming heat to be transferred uniformly from all surfaces, determine \((a)\) the amount of heat this resistor dissipates during a \(24-\mathrm{h}\) period, \((b)\) the heat flux, and \((c)\) the fraction of heat dissipated from the top and bottom surfaces.

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