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charle [14.2K]
3 years ago
14

A rigid, sealed cylinder initially contains 100 lbm of water at 70 °F and atmospheric pressure. Determine: a) the volume of the

tank (ft3 ). Later, a pump is used to extract 10 lbm of water from the cylinder. The water remaining in the cylinder eventually reaches thermal equilibriu
Engineering
1 answer:
soldier1979 [14.2K]3 years ago
3 0

Answer:

Determine A) The Volume Of The Tank (ft^3) Later A Pump Is Used To Extract ... A rigid, sealed cylinder initially contains 100 lbm of water at 70 degrees F and atmospheric pressure. ... Later a pump is used to extract 10 lbm of water from the cylinder. The water remaining in the cylinder eventually reaches thermal equilibrium ...

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Water flows through a pipe of 100 mm at the rate of 0.9 m3 per minute at section A. It tapers to 50mm diameter at B, A being 1.5
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Answer:

The velocities in points A and B are 1.9 and 7.63 m/s respectively. The Pressure at point B is 28 Kpa.

Explanation:

Assuming the fluid to be incompressible we can apply for the continuity equation for fluids:

Aa.Va=Ab.Vb=Q

Where A, V and Q are the areas, velocities and volume rate respectively. For section A and B the areas are:

Aa=\frac{pi.Da^2}{4}= \frac{\pi.(0.1m)^2}{4}=7.85*10^{-3}\ m^3

Ab=\frac{pi.Db^2}{4}= \frac{\pi.(0.05m)^2}{4}=1.95*10^{-3}\ m^3

Using the volume rate:

Va=\frac{Q}{Aa}=\frac{0.9m^3}{7.85*10^{-3}\ m^3} = 1.9\ m/s

Vb = \frac{Q}{Ab}= \frac{0.9m^3}{1.96*10^{-3}\ m^3} = 7.63\ m/s

Assuming no losses, the energy equation for fluids can be written as:

Pa+\frac{1}{2}pa.Va^2+pa.g.za=Pb+\frac{1}{2}pb.Vb^2+pb.g.zb

Here P, V, p, z and g represent the pressure, velocities, height and gravity acceleration. Considering the zero height level at point A and solving for Pb:

Pb=Pa+\frac{1}{2}pa(Va^2-Vb^2)-pa.g.za

Knowing the manometric pressure in point A of 70kPa, the height at point B of 1.5 meters, the density of water of 1000 kg/m^3 and the velocities calculated, the pressure at B results:

Pb = 70000Pa+ \frac{1}{2}*1000\ \frac{kg}{m^3}*((1.9m/s)^2 - (7.63m/s)^2) - 1000\frac{kg}{m^3}*9,81\frac{m}{s^2}*1.5m

Pb = 70000\ Pa-27303\ Pa - 14715\ Pa

Pb = 27,996\ Pa = 28\ kPa

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Neon is compressed from 100 kPa and 20◦C to 500 kPa in an isothermal compressor. Determine the change in the specific volume and
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Answer:

The specific volume is reduced in 80 per cent due to isothermal compression.

Specific enthalpy remains constant.

Explanation:

Let suppose that neon behaves ideally, the equation of state for ideal gases is:

P\cdot V = n\cdot R_{u}\cdot T

Where:

P - Pressure, measured in kilopascals.

V - Volume, measured in cubic meters.

n - Molar quantity, measured in kilomoles,

T - Temperature, measured in kelvins.

R_{u} - Ideal gas constant, measured in \frac{kPa\cdot m^{3}}{kmol\cdot K}.

On the other hand, the molar quantity (n) and specific volume (\nu), measured in cubic meter per kilogram, are defined as:

n = \frac{m}{M} and \nu = \frac{V}{m}

Where:

m - Mass of neon, measured in kilograms.

M - Molar mass of neon, measured in kilograms per kilomoles.

After replacing in the equation of state, the resulting expression is therefore simplified in term of specific volume:

P\cdot V = \frac{m}{M}\cdot R_{u}\cdot T

P\cdot \nu = \frac{R_{u}\cdot T}{M}

Since the neon is compressed isothermally, the following relation is constructed herein:

P_{1}\cdot \nu_{1} = P_{2}\cdot \nu_{2}

Where:

P_{1}, P_{2} - Initial and final pressure, measured in kilopascals.

\nu_{1}, \nu_{2} - Initial and final specific volume, measured in cubic meters per kilogram.

The change in specific volume is given by the following expression:

\frac{\nu_{2}}{\nu_{1}} = \frac{P_{1}}{P_{2}}

Given that P_{1} = 100\,kPa and P_{2} = 500\,kPa, the change in specific volume is:

\frac{\nu_{2}}{\nu_{1}} = \frac{100\,kPa}{500\,kPa}

\frac{\nu_{2}}{\nu_{1}} = \frac{1}{5}

The specific volume is reduced in 80 per cent due to isothermal compression.

Under the ideal gas supposition, specific enthalpy is only function of temperature, as neon experiments an isothermal process, temperature remains constant and, hence, there is no change in specific enthalpy.

Specific enthalpy remains constant.

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