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disa [49]
3 years ago
7

The normal boiling point of ethanol is 78.4 oC and its heat of vaporization is 38.56 kJ/mol. What is the vapor pressure of ethan

ol at 15 oC?
Physics
1 answer:
Leno4ka [110]3 years ago
7 0

Answer: 0.05470atm

Explanation:

The vapor pressure is determined by Clausius Clapeyron equation:

ln(\frac{P_2}{P_1})=\frac{\Delta H_{vap}}{R}(\frac{1}{T_1}-\frac{1}{T_2})

where,

P_1 = initial pressure at  = 1 atm (standard atmospheric pressure

P_2 = final pressure at 15^oC = ?

\Delta H_{vap} = enthalpy of vaporisation = 38.56 kJ/mol = 38560 J/mol

R = gas constant = 8.314 J/mole.K

T_1= initial temperature = 78.4^oC=273+78.4=351.4K

T_2 = final temperature =15^oC=273+15=288K

Now put all the given values in this formula, we get

\log (\frac{P_2}{1atm})=\frac{38560}{2.303\times 8.314J/mole.K}[\frac{1}{351.4K}-\frac{1}{288K}]

\log (\frac{P_2}{1atm})=-1.262

P_2=0.05470atm

Thus the vapor pressure of ethanol at 15^0C is 0.05470atm

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Answer:

i. The radius 'r' of the electron's path is 4.23 × 10^{-5} m.

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Explanation:

The radius 'r' of the electron's path is called a gyroradius. Gyroradius is the radius of the circular motion of a charged particle in the presence of a uniform magnetic field.

                 r = \frac{mv}{qB}

Where: B is the strength magnetic field, q is the charge, v is its velocity and m is the mass of the particle.

From the question, B = 1.63 × 10^{-5}T, v = 121 m/s, Θ = 90^{0} (since it enters perpendicularly to the field), q = e  = 1.6 × 10^{-19}C and m = 9.11 × 10^{-31}Kg.

Thus,

         r = \frac{mv}{qB} ÷ sinΘ

But,  sinΘ =  sin 90^{0} = 1.

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          r = \frac{mv}{qB}

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            = 1.10231 × 10^{-28}   ÷ 2.608 × 10^{-24}

            = 4.2266 × 10^{-5}

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B. The frequency 'f' of the motion is called cyclotron frequency;

           f = \frac{qB}{2\pi m}

             =  (1.6 × 10^{-19}  × 1.63 × 10^{-5}) ÷ (2 ×\frac{22}{7} × 9.11 × 10^{-31})

             =  2.608 × 10^{-24} ÷  5.7263 × 10^{-30}

             = 455442.4323

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The frequency 'f' of the motion is 455.44 KHz.

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