Thursday, April 29, 2021

HEAT VAPORIZATION OF WATER

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Lab # 5


Lab Title-Heat of Vaporization of Water Using the Boiling Point Method


Lab Partners- Matt Yates, Melissa Sanford and Elizabeth Natchwey


Lab Text The Elements of Physical Chemistry With Applications in Biology, by Atkins


Write my Essay on HEAT VAPORIZATION OF WATER cheap


rd Edition, Freeman, 00.


Survey of Physical Chemistry Lab Manual


Date Performed 10/11/0


Submission Date 11/8/0


I. Abstract


The vapor pressure of a liquid is the measure of the ability of molecules to escape from the surface of a solid or liquid. The intermolecular forces holding the molecule together are broken when the temperature is raised, due to the kinetic energy of the molecules. As more molecules build up in the space above the solid or liquid, more of them collide with the surface and some may adhere. At a fixed temperature the system will reach a state of dynamic equilibrium. At this point the pressure exerted by the molecules in the space above the solid or liquid, by definition, is the vapor pressure of the solid or liquid. When external pressure is exerted on the liquid, the vapor pressure also increases because the molecules are compressed, which also increases their energy.


II. Introduction


To determine the heat of vaporization we used a common method. Various external applied pressures are applied to the liquid while heating and the point at which the liquid boils is recorded.


The formula for the equilibrium between a pure liquid and its vapor is equation #1


X(l) X(g) (P, T) (eq. 1)


There is a definite relationship that exists between the pressure and the temperature at equilibrium. This relationship is equation #


dPdT = (eq. )


In equation # dP and dT are referring to an infinite number of changes for both pressure and temperature in a system at equilibrium with pure substances and both phases always present. ÄS and ÄV are referring to the entropy change and the volume when a phase transforms into another at both constant pressure and temperature. Since ÄG is 0 for a change in state the ÄS term in the equation can be replaced using and the resulting equation will produce equation #


dPdT = (eq. )


The Claperon equation is an exact expression that can be applied to many different phase equilibria. Equations and are known as the Claperon equation. When a Vaporization occurs there is a change in volume that is standard. ÄVvap (which is also Vg-V1) is about Vg. If Vg is substituted for ÄV equation #4 is the result


dpdT = (eq. 4)


Calculus says that dlnp = and that , after algebra and manipulation equation #4 can be turned magically into equation #5


= - (eq. 5)


If the compressibility factor of the gas is introduced as Z produces equation #6


Z = (eq. 6)


When equation #5 is multiplied by R/R most of the variable can be substituted with Z. When this happens a new convenient form of the Claperon equation is the result equation #7


= - (eq. 7)


Equation #7 can be rearranged to produce equation #8 and then it can be integrated to produce the Clausius Claperon equation, equation #


(eq. 8)


(eq. )


III. Experimental Methods


Equipment Needed (Typical Boiling Point Apparatus)


5 Liter Ballast Bulb Thermometer Adapter


Closed Tube Manometer Reflux Condenser


Double Neck Distillation Flask Bent Glass Tube with Adapter


Thermometers Electric Heating Mantle


Variac Long Pieces of Rubber Tubing


Rubber Pressure Tubing Long Pieces of Heavy Wall


Utility Clamps or Clamp Holders


Iron Ring Boiling Chips


The apparatus should be assembled to resemble Figure #1. Be sure to support all glass ware with clams at critical points. The double neck flask should be about one-third full of distilled de-ionized water. Add one or two boiling chips to the water. Stopcock X and stopcock S are not to be opened at the same time. Heat the water until vapor begins to condense on a drip from the thermometer bulb. Open the stopcock X and watch the manometer until both the mercury levels in the manometer and the thermometer are steady. Record the two readings. Record the ambient air temperature at the manometer every time you record both the boiling point and the vapor pressure. To take another reading close stopcock X and lower the heating mantle. Allow the flask to cool enough to stop the boiling and introduce new air into the system by opening stopcock S. Close stopcock S. Repeat the procedure until you have readings for the following pressures Decending 560, 450, 40, 40, 160, 10, and 0 Torr. Ascending 110, 10, 140, 180, 60, 60, 470, and 580 Torr. Record all data and proceed to calculations.


IV. Results and Observations


Chart #1


P (mmHg) CP (mmHg) T (°C) T (K) Height #1 (cm) Height # (cm) AAT (°C) 1/T lnP


66 6.568 4.7 67.85 71.0 8.0 4.0 0.007184 6.4501


560 557.5808 . 65.45 68.55 11.10 4.0 0.00765 6.607


450 448.056 86 5.15 6.55 17.5 4.0 0.007845 6.10418


40 8.51 7.55 5.7 57.77 .50 4.0 0.008571 5.84616


40 8.51 70.45 4.6 5.0 7.5 4.0 0.001061 5.47610


160 15.088 6.5 5.5 48.50 1.65 4.0 0.008066 5.070844


10 1.484 57.4 0.55 46.75 .40 4.0 0.000561 4.8605


0 8.611 50.4 .55 44.85 5.0 4.0 0.000071 4.4548


110 10.548 5.7 6.85 45.65 4.45 4.0 0.0005507 4.66151


10 11.4816 55.4 8.55 46.10 4.00 4.0 0.0004677 4.7816


140 1.5 58.8 1.5 47.0 .0 4.0 0.000150 4.71


180 17.4 66.5 .5 50.15 .5 4.0 0.0045508 5.18867


60 58.8768 7.5 45.5 5.10 7.00 4.0 0.008456 5.5565


60 58.4448 80.55 5.7 58.0 1.70 4.0 0.008755 5.881775


470 467.66 85. 5.05 6.55 17.5 4.0 0.0078517 6.14840


580 577.444 .6 65.75 68.85 10.70 4.0 0.0074108 6.586


Graph #1


V. Discussion and Conclusion


VI. References


The Elements of Physical Chemistry With Applications in Biology, by Atkins


rd Edition, Freeman, 00.


Survey of Physical Chemistry Lab Manual


VII. Appendices


Definitions from The Elements of Physical Chemistry With Applications in Biology, by Atkins


Vapor Pressure-The pressure of the vapor in equilibrium with its condensed phase is called the vapor pressure of the substance.


Critical Temperature-The temperature at which the surface disappears is the critical temperature.


Critical Pressure-The vapor pressure at the critical temperature is called the critical pressure.


Critical Point-The critical temperature and the critical pressure together determine the critical point.


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