Solution: (a) Source coding is the process of eﬃciently converting the output of either an analog or a digital source, with as little or no redundancy, into a sequence of binary digits. (b) The channel encoder introduces, in a controlled (structured) manner, certain amount of redundancy that can be used at the...
Many people will lose their livelihood and their homes due to the effects of environmental degradation. We need our trees to store greenhouse gases and to produce oxygen and cannot afford to cut or burn These children are more likely to behave environmentally-friendly when they grow up.
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Under conditions of low pressure and high temperature, these factors are negligible, the ideal gas equation is an accurate description of gas behavior, and the gas is said to exhibit ideal behavior. However, at lower temperatures and higher pressures, corrections for molecular volume and molecular attractions are required to account for finite ...

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• (P + a/V2) (V – b) = nRT. The value of “a” is constant as well as “b”, and therefore should be experimentally determined for each gas. SUMMARY: 1.Ideal gas has no definite volume while real gas has definite volume. 2.Ideal gas has no mass whereas real gas has mass. 3.Collision of ideal gas particles is elastic while non-elastic for ...
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The partial pressure (p) of a gas is obtained from C by introducing the molar mass (M) into the ideal gas law: p = RTC/M. Thus we have: J = -(DM/RT) (dp/dx). In other words, the diffusion permeability of ideal water vapor is DM/RT, where R is the molar gas constant: 8.314 472(15) J/K/mol.

• It (T c) is the maximum temperature at which a gas can be liquefied i.e. the temperature above which a gas can’t exist as liquid. T = 8a / 27Rb. Critical Pressure (P c) It is the minimum pressure required to cause liquefaction at T c . P c = a/27b 2 . Critical Volume; It is the volume occupied by one mol of a gas at T c and P c . V c = 3b
• Ideal Gasses vs. Real Gasses Ideal Gas assumptions: - No volume - No attractive forces between particles of gas There is no gas which exhibits these qualities, but there are many conditions which real gasses behave the same as an ideal gas. Real gasses differ most from an ideal gas at low temperatures and high pressures.

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The molar volume for s.t.p is 22.4 dm 3 (22.4 litres) at 0 o C and 1 atmosphere pressure. Historically, s.t.p unfortunately stands for standard temperature and pressure, but these days 25 o C/298K is usually considered the standard temperature (RTP, rtp, r.t.p). Some handy relationships for substance Z below:

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molar mass of a sample gas from P, V, T data: where m is the sample’s mass in grams. As with the special equation for density, it is not necessary to memorize this equation. With P, V, T data for a gas sample whose mass is known, simply calculate the number of moles, n, for the sample. The molar mass, then, is the sample mass

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Real gases behave ideally only under circumstances where the pressure is low and the temperature is high. This above mentioned are the gases which do not obey the partial pressure law proposed by Dalton at the room temperature.

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The van der Waals equation is a modi ed version of the ideal gas law that can be used to account for the non-ideal behavior of gases under conditions. 2 Key Equations Z = molar volume of gas at same T and P molar volume of ideal gas at same T and P+ n2 a V2 × (V − nb) = nRT P = P × Vm R×T measured (4) OpenStax-CNX module: m51072 6 3 ...

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