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Methanol \(\left(\rho=791 \mathrm{~kg} / \mathrm{m}^{3}\right.\) and $\left.M=32 \mathrm{~kg} / \mathrm{kmol}\right)$ undergoes evaporation in a vertical tube with a uniform cross-sectional area of \(0.8 \mathrm{~cm}^{2}\). At the top of the tube, the methanol concentration is zero, and its surface is $30 \mathrm{~cm}$ from the top of the tube (Fig. P14-111). The methanol vapor pressure is \(17 \mathrm{kPa}\), with a mass diffusivity of $D_{A B}=0.162 \mathrm{~cm}^{2} / \mathrm{s}$ in air. The evaporation process is operated at \(25^{\circ} \mathrm{C}\) and \(1 \mathrm{~atm}\). (a) Determine the evaporation rate of the methanol in \(\mathrm{kg} / \mathrm{h}\) and (b) plot the mole fraction of methanol vapor as a function of the tube height, from the methanol surface \((x=0)\) to the top of the tube \((x=L)\).

Short Answer

Expert verified
Answer: The evaporation rate of methanol from the tube is \(1.74 \times 10^{-2} \,\mathrm{kg} \, \mathrm{h}^{-1}\).

Step by step solution

01

Convert given units to SI units

To have a consistent unit system, we will convert all given quantities to the SI unit system: Area of the tube = \(0.8 \mathrm{cm}^{2} = 8 \times 10^{-5} \mathrm{m}^2\) Planar height of the tube = \(30 \mathrm{cm}=0.3 \mathrm{m}\) Mass diffusivity, \(D_{AB} =0.162 \mathrm{cm}^{2} / \mathrm{s}=1.62 \times 10^{-5} \mathrm{m}^{2} / \mathrm{s}\) Pressure of methanol = \(17 \mathrm{kPa} = 17000 \mathrm{Pa}\)
02

Apply Fick's Law to find the evaporation rate

Now, we will apply Fick's Law, which states that flux of A through B is given by: \(N_A = -D_{AB} \frac{dY_A}{dz}\) Since the methanol concentration at the top of the tube(\(z=0\)) is zero, we can integrate Fick's Law and write the molar flux of methanol as: \(N_A = D_{AB} \frac{P_A}{RT} \frac{dY_A}{dz}\) To find the gradient, we will use the ideal gas law relation: \(Y_A P = \rho_A RT\)
03

Calculate the evaporation rate of methanol

We need to find the molar fraction, Y_A, of methanol at the evaporating surface (\(z = L = 0.3\,\text{m}\)). We have: \(Y_A = \frac{P_A}{P} = \frac{17000}{101325} = 0.1679\) As we know the concentration of methanol at the top of the tube (z=L) and at z=0, we can determine the gradient \(dY_A/dz\) by: \(\frac{dY_A}{dz} = \frac{0.1679-0}{0.3}\) Using these values in Fick's Law equation: \(N_A = (1.62 \times 10^{-5}) \frac{17000}{(8.314 \times 298)} \frac{0.1679}{0.3}\) \(N_A = 1.891 \times 10^{-5} \mathrm{kmol} \, \mathrm{m}^{-2} \,\mathrm{s}^{-1}\) Now, we are able to determine the evaporation rate by multiplying the molar flux by the cross-sectional area of the tube and the molar mass of methanol: \(Evap. Rate = N_A \cdot A \cdot M = 1.891 \times 10^{-5} \cdot 8 \times 10^{-5} \cdot 32\) The evaporation rate is in \(\mathrm{kmol}\,\mathrm{m}^{-2}\,\mathrm{s}^{-1}\), to convert it to \(\mathrm{kg}\, \mathrm{h}^{-1}\), multiply by \(3600\,\text{s}\): \(Evap. Rate = 1.891 \times 10^{-5} \cdot 8 \times 10^{-5} \cdot 32 \cdot 3600 = 1.74 \times 10^{-2} \mathrm{kg} \, \mathrm{h}^{-1}\) The evaporation rate of the methanol is \(1.74 \times 10^{-2} \,\mathrm{kg} \, \mathrm{h}^{-1}\).
04

Calculate mole fraction of methanol vapor along the tube height

To determine the mole fraction of methanol vapor along the height, we will use Fick's Law: \(Y_A = \int -\frac{D_{AB}}{RT} \cdot N_A dz\) where we know the mole fraction \(Y_A(L) = 0.1679\). For different distances \((z)\) along the height, we can determine the mole fraction, \(Y_A =\int -\frac{D_{AB}}{RT} \cdot N_A dz\). Then, plot the mole fraction as a function of height from the methanol surface to the top of the tube. In conclusion, we found that the evaporation rate of methanol is \(1.74 \times 10^{-2} \,\mathrm{kg} \, \mathrm{h}^{-1}\). The plot of the mole fraction of methanol vapor along the height can be constructed by evaluating the integral \(Y_A =\int -\frac{D_{AB}}{RT} \cdot N_A dz\) for different heights.

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Most popular questions from this chapter

A glass bottle washing facility uses a well-agitated hot water bath at \(50^{\circ} \mathrm{C}\) with an open top that is placed on the ground. The bathtub is \(1 \mathrm{~m}\) high, \(2 \mathrm{~m}\) wide, and \(4 \mathrm{~m}\) long and is made of sheet metal so that the outer side surfaces are also at about \(50^{\circ} \mathrm{C}\). The bottles enter at a rate of 800 per minute at ambient temperature and leave at the water temperature. Each bottle has a mass of \(150 \mathrm{~g}\) and removes \(0.6 \mathrm{~g}\) of water as it leaves the bath wet. Makeup water is supplied at \(15^{\circ} \mathrm{C}\). If the average conditions in the plant are \(1 \mathrm{~atm}, 25^{\circ} \mathrm{C}\), and 50 percent relative humidity, and the average temperature of the surrounding surfaces is \(15^{\circ} \mathrm{C}\), determine \((a)\) the amount of heat and water removed by the bottles themselves per second, (b) the rate of heat loss from the top surface of the water bath by radiation, natural convection, and evaporation, \((c)\) the rate of heat loss from the side surfaces by natural convection and radiation, and \((d)\) the rate at which heat and water must be supplied to maintain steady operating conditions. Disregard heat loss through the bottom surface of the bath, and take the emissivities of sheet metal and water to be \(0.61\) and \(0.95\), respectively.

A glass of milk left on top of a counter in the kitchen at $15^{\circ} \mathrm{C}, 88 \mathrm{kPa}$, and 50 percent relative humidity is tightly sealed by a sheet of \(0.009\)-mm-thick aluminum foil whose permeance is $2.9 \times 10^{-12} \mathrm{~kg} / \mathrm{s} \cdot \mathrm{m}^{2} \cdot \mathrm{Pa}\(. The inner diameter of the glass is \)12 \mathrm{~cm}$. Assuming the air in the glass to be saturated at all times, determine how much the level of the milk in the glass will recede in \(12 \mathrm{~h}\). Answer: \(0.0011 \mathrm{~mm}\)

For the absorption of a gas (like carbon dioxide) into a liquid (like water) Henry's law states that partial pressure of the gas is proportional to the mole fraction of the gas in the liquid-gas solution with the constant of proportionality being Henry's constant. A bottle of soda pop \(\left(\mathrm{CO}_{2}-\mathrm{H}_{2} \mathrm{O}\right)\) at room temperature has a Henry's constant of \(17,100 \mathrm{kPa}\). If the pressure in this bottle is \(140 \mathrm{kPa}\) and the partial pressure of the water vapor in the gas volume at the top of the bottle is neglected, the concentration of the \(\mathrm{CO}_{2}\) in the liquid \(\mathrm{H}_{2} \mathrm{O}\) is (a) \(0.004 \mathrm{~mol}-\mathrm{CO}_{2} / \mathrm{mol}\) (b) \(0.008 \mathrm{~mol}-\mathrm{CO}_{2} / \mathrm{mol}\) (c) \(0.012 \mathrm{~mol}-\mathrm{CO}_{2} / \mathrm{mol}\) (d) \(0.024 \mathrm{~mol}-\mathrm{CO}_{2} / \mathrm{mol}\) (e) \(0.035 \mathrm{~mol}-\mathrm{CO}_{2} / \mathrm{mol}\)

Moisture migration in the walls, floors, and ceilings of buildings is controlled by vapor barriers or vapor retarders. Explain the difference between the two, and discuss which is more suitable for use in the walls of residential buildings.

Carbon at \(1273 \mathrm{~K}\) is contained in a \(7-\mathrm{cm}\)-innerdiameter cylinder made of iron whose thickness is \(1.2 \mathrm{~mm}\). The concentration of carbon in the iron at the inner surface is $0.5 \mathrm{~kg} / \mathrm{m}^{3}$ and the concentration of carbon in the iron at the outer surface is negligible. The diffusion coefficient of carbon through iron is $3 \times 10^{-11} \mathrm{~m}^{2} / \mathrm{s}$. The mass flow rate of carbon by diffusion through the cylinder shell per unit length of the cylinder is (a) \(2.8 \times 10^{-9} \mathrm{~kg} / \mathrm{s}\) (b) \(5.4 \times 10^{-9} \mathrm{~kg} / \mathrm{s}\) (c) \(8.8 \times 10^{-9} \mathrm{~kg} / \mathrm{s}\) (d) \(1.6 \times 10^{-8} \mathrm{~kg} / \mathrm{s}\) (e) \(5.2 \times 10^{-8} \mathrm{~kg} / \mathrm{s}\)

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