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Consider a 7.6-cm-diameter cylindrical lamb meat chunk $\left(\rho=1030 \mathrm{~kg} / \mathrm{m}^{3}, c_{p}=3.49 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K}, k=0.456 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\right.$, \(\alpha=1.3 \times 10^{-7} \mathrm{~m}^{2} / \mathrm{s}\) ). Such a meat chunk intially at \(2^{\circ} \mathrm{C}\) is dropped into boiling water at \(95^{\circ} \mathrm{C}\) with a heat transfer coefficient of $1200 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}$. The time it takes for the center temperature of the meat chunk to rise to \(75^{\circ} \mathrm{C}\) is (a) \(136 \mathrm{~min}\) (b) \(21.2 \mathrm{~min}\) (c) \(13.6 \mathrm{~min}\) (d) \(11.0 \mathrm{~min}\) (e) \(8.5 \mathrm{~min}\)

Short Answer

Expert verified
Answer: _____ minutes

Step by step solution

01

Recall the relationship between temperature and time using the lumped capacitance method

In this case, we'll be using the lumped capacitance method to determine the relationship between temperature and time (assuming it is valid for this problem). The equation for temperature versus time is: \(T(t) - T_\infty = (T_0 - T_\infty)e^{-\frac{hA}{\rho V c_p}t}\) Where: - \(T(t)\): Temperature of the meat chunk at time \(t\) - \(T_\infty\): Temperature of the water (95°C) - \(T_0\): Initial temperature of the meat chunk (2°C) - \(h\): Heat transfer coefficient (1200 W/m²·K) - \(A\): Surface area of the cylindrical meat chunk - \(\rho\): Density of the meat (1030 kg/m³) - \(V\): Volume of the meat chunk - \(c_p\): Specific heat capacity of meat (3.49 kJ/kg·K) - \(t\): Time (s)
02

Check validity of lumped capacitance method

In order for the lumped capacitance method to be valid, the Biot number (Bi) must be less than 0.1. Calculate Bi as follows: \(Bi = \frac{hL_c}{k}\) Where: - \(L_c\): Characteristic length (in this case, \(L_c = \frac{V}{A}\)) - \(k\): Thermal conductivity (0.456 W/m·K)
03

Calculate the surface area and volume

The surface area \(A\) and volume \(V\) of a cylinder are given by the following formulas: \(A = 2 \pi r^2 + 2 \pi rh\) \(V = \pi r^2h\) Where: - \(r\): Radius of the cylinder (half of the diameter; 3.8 cm) - \(h\): Height of the cylinder (not given, assume it is equal to the diameter; 7.6 cm)
04

Solve the temperature-time equation for time

Now, we will express all lengths in meters (1 cm = 0.01 m) and replace the given values into the temperature-time equation. We need to find the time \(t\) when the center temperature of the meat chunk is 75°C. We will rearrange the temperature-time equation to isolate \(t\) on one side: \(t = -\frac{\rho V c_p}{hA} \ln \left(\frac{T(t) - T_\infty}{T_0 - T_\infty}\right)\) Plug in the given values and calculate the time \(t\).
05

Convert the time from seconds to minutes

Convert the calculated time \(t\) from seconds to minutes by dividing the result by 60. Compare the calculated time with the given options and choose the best match.

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Most popular questions from this chapter

Citrus fruits are very susceptible to cold weather, and extended exposure to subfreezing temperatures can destroy them. Consider an 8 -cm-diameter orange that is initially at \(15^{\circ} \mathrm{C}\). A cold front moves in one night, and the ambient temperature suddenly drops to \(-6^{\circ} \mathrm{C}\), with a heat transfer coefficient of $15 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}$. Using the properties of water for the orange and assuming the ambient conditions remain constant for \(4 \mathrm{~h}\) before the cold front moves out, determine if any part of the orange will freeze that night. Solve this problem using the analytical one-term approximation method.

Thick slabs of stainless steel $(k=14.9 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\( and \)\left.\alpha=3.95 \times 10^{-6} \mathrm{~m}^{2} / \mathrm{s}\right)\( and copper \)(k=401 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\( and \)\left.\alpha=117 \times 10^{-6} \mathrm{~m}^{2} / \mathrm{s}\right)$ are placed under an array of laser diodes, which supply an energy pulse of \(5 \times 10^{7} \mathrm{~J} / \mathrm{m}^{2}\) instantaneously at \(t=0\) to both materials. The two slabs have a uniform initial temperature of \(20^{\circ} \mathrm{C}\). Determine the temperatures of both slabs at $5 \mathrm{~cm}\( from the surface and \)60 \mathrm{~s}$ after receiving an energy pulse from the laser diodes.

Consider a cubic block whose sides are \(5 \mathrm{~cm}\) long and a cylindrical block whose height and diameter are also \(5 \mathrm{~cm}\). Both blocks are initially at \(20^{\circ} \mathrm{C}\) and are made of granite $\left(k=2.5 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\right.\( and \)\left.\alpha=1.15 \times 10^{-6} \mathrm{~m}^{2} / \mathrm{s}\right)$. Now both blocks are exposed to hot gases at \(500^{\circ} \mathrm{C}\) in a furnace on all of their surfaces with a heat transfer coefficient of $40 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}$. Determine the center temperature of each geometry after 10 , 20 , and \(60 \mathrm{~min}\). Solve this problem using the analytical oneterm approximation method.

In areas where the air temperature remains below \(0^{\circ} \mathrm{C}\) for prolonged periods of time, the freezing of water in underground pipes is a major concern. Fortunately, the soil remains relatively warm during those periods, and it takes weeks for the subfreezing temperatures to reach the water mains in the ground. Thus, the soil effectively serves as an insulation to protect the water from the freezing atmospheric temperatures in winter. The ground at a particular location is covered with snowpack at $-8^{\circ} \mathrm{C}$ for a continuous period of 60 days, and the average soil properties at that location are $k=0.35 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\( and \)\alpha=0.15 \times 10^{-6} \mathrm{~m}^{2} / \mathrm{s}$. Assuming an initial uniform temperature of \(8^{\circ} \mathrm{C}\) for the ground, determine the minimum burial depth to prevent the water pipes from freezing.

A small chicken $(k=0.45 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, \quad \alpha=0.15 \times\( \)10^{-6} \mathrm{~m}^{2} / \mathrm{s}$ ) can be approximated as an \(11.25-\mathrm{cm}\)-diameter solid sphere. The chicken is initially at a uniform temperature of \(8^{\circ} \mathrm{C}\) and is to be cooked in an oven maintained at \(220^{\circ} \mathrm{C}\) with a heat transfer coefficient of \(80 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). With this idealization, the temperature at the center of the chicken after a 90 -min period is (a) \(25^{\circ} \mathrm{C}\) (b) \(61^{\circ} \mathrm{C}\) (c) \(89^{\circ} \mathrm{C}\) (d) \(122^{\circ} \mathrm{C}\) (e) \(168^{\circ} \mathrm{C}\)

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