stage 2 physical chem.experiment(1,2,3,4,5)111

54
Experiment (1) The Density of a liquid as a Function of Temperature Theory The density of liquid is the mass of unit volume of the liquid. The generally accepted unit of volume is the milliliter which is defined as the volume occupied by 1 gm of water at the temperature of maximum density (4°C) . The density of liquid at (t°C) is expressed relation to that of water at 4°C and is represented by the symbol d t(liq) 4°C(H2O) The density of liquid at a particular temperature (t) is the product of the relative density of the liquid d t(liq) 4°C(H2O) The density of water at that temperature, i.e . d t (liq) 4°C(H2O) = d t (liq) t(H2O) . d t (H 2 O) 4°C(H2O) ------ (1) d t (liq) 4°C(H2O) = ẁ/w . d t°(H 2 O) 4°C(H2O) -----------(2) Where w is the apparent weight of water and ẁ the apparent weight of liquid at the temperature (t) . The relation between density of liquid and temperature can be represented by this equation : 1 / d t = (1/d ° ) . (1+αt) ------------ (3) 1

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Page 1: Stage 2 Physical Chem.experiment(1,2,3,4,5)111

Experiment (1)

The Density of a liquid as a Function of Temperature

Theory The density of liquid is the mass of unit volume of the liquid. The generally accepted unit of volume is the milliliter which is defined as the volume occupied by 1 gm of water at the temperature of maximum density (4°C) . The density of liquid at (t°C) is expressed relation to that of water at 4°C and is represented by the symbol

dt(liq) 4°C(H2O)

The density of liquid at a particular temperature (t) is the product of the relative density of the liquid

dt(liq) 4°C(H2O)

The density of water at that temperature, i.e.

dt (liq)4°C(H2O) = dt (liq)

t(H2O) . dt (H2O)4°C(H2O) ------ (1)

dt (liq)4°C(H2O) = ẁ/w . d t°(H2O)

4°C(H2O) -----------(2)

Where w is the apparent weight of water and ẁ the apparent weight of liquid at the temperature (t).

The relation between density of liquid and temperature can be represented by this equation :

1/dt = (1/d°) . (1+αt) ------------ (3)

A plot of 1/dt against (t) will have a slope of α/d° and an intercept (1/d°), when t=0 . Thus, α, the coefficient of expansion may be determined.

Apparatus and chemicals

Pyknometer , balance , dropper , water bath , thermometer , benzene or carbon tetra chloride.

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Procedure

1 -The pyknometer is cleaned and dried thoroughly and then weight let is be (w) .2 -The pyknometer is filled with distilled water, and then is suspended in a

thermostat at 20°C . 3 -After allowing 10- 15 min for thermal equilibrium to be established, the

amount of water in the pyknometer is adjusted to the mark on it . 4 -pyknometr is then removed from the thermostat and the out side carefully dried (care is taken not to expel water from the pyknometer by the heat of the

hand ) . 5-The pyknometer and contents are weighted let is be (w1).

6 -The above procedure repeated at 30 and 40°C, and let the weights will be w2 and w3 respectively .

7 -Repeat steps (2-6) by using a liquid such as benzene or CCl4, let the weights will be ẁ1, ẁ2 and ẁ3 respectively for 20, 30 and 40°C.

Calculation

1 -Regulate the data at such a table:

1/dliqd t(liq)Weight of liquid (gm)

dt (H2O)Weight

of water (gm)

t°C

w - ẁ1 from constantsPhysical

chemistrybooks

w1- w 20w - ẁ2w - w230w - ẁ3w - w340

2 -Find 1/dt by using equation (3) 3 -Plot 1/dt against (t) and find the value of d° (liq) and α

1/dt(liq) slope= α/ d° (liq)

t,°C

Experiment (2)

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Density of solid

Theory The density of a substance is defined as its mass per unit volume . The most obvious way to determine the density of a solid is to weigh a sample of the solid and then find out the volume that the sample occupies. In this experiment, you will be supplied with variously shaped pieces of things. You are asked to determine the density of each specimen

Apparatus and chemicals Balance, distilled water, samples , cylinder.

Procedure

1 -Obtain an unknown specimen from your teacher .2 -Weigh the samples accurately on an analytical balance.

3 -Determine the volume of your specimen directly by carefully sliding the specimen into a graduated cylinder containing a known volume of water

makes sure that the specimen is completely coved with water and that no air bubbles are trapped . Note the total volume of the water and specimen .

Calculation

d = w/v By putting the weight and volume which we founded them later, find the density of solid .

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Experiment (3)

Viscosity of Liquid as a function of Temperature

Theory Viscosity is the resistance that one part of a fluid offers to the flow of a contiguous part of the liquid. The viscosity coefficient η is the force required per unit area to maintain unit difference of velocity between two parallel planes in the fluid, 1 cm apart. The unit of viscosity in c.g.s. units is called poise. The viscosity of a liquid may be determined by measuring its rate of flow through a capillary tube.For a liquid flowing through a capillary tube of radius r, for a time t, under a constant pressure head p, the volume v of liquid issuing from the tube is given by poiseuille's equation:

υ = π p t r4/8 ℓ η ---------------- (1)

where ℓ is the length of the tube. If the dimensions of the capillary and the volume of the liquid flowing through it are constant, equation (1) reduces to

η = k p t ------------------ (2)

Thus although the determination of absolute viscosity is a matter of some difficulty, the ratio of the viscosities of two liquids may be readily determined using a viscometer. The pressure p at any instant driving the liquid of density d though the capillary of a viscometer is ( hdg), where h is the difference in height between the levels in each limb of the instrument. Although h varies throughout the experiment the initial and final values are the same in every case; hence p is proportional to the density. The relationship between the viscosities η1 and η2 of two liquids 1 and 2 having densities d1 and d2 is

η1 / η2 = d1 t1 / d2 t2 ………………..…. (3)

where t1 and t2 are the times of flow. The viscometer must therefore be calibrated by using a liquid of known viscosity and density, e.g. water. The variation of the viscosity of a liquid with temperature may be expressed by the equation:

η = A . e E/RT -------------------- (4)

i.e., ln η = E / RT + ln A ---------- (5)

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where A is a constant and E is a measure of the energy required to overcome the elementary flow process.

Apparatus and Chemicals

Ostwald viscometer, stop watch, thermostat, rubber tubing, beaker,

sucrose, distilled water .

Procedure

1-The viscometer is cleaned and dried.2-50ml of water is added to a beaker and clamped in the thermostat at

25°C, 10 min allowed for thermal equilibrium.3 -By a piece of rubber tube, the liquid is sucked up the capillary arm of

the viscometer until the surface of the liquid is above the upper mark ) Fig.1.(

4 -The liquid is then allowed to flow down the aim .The time required for the surface of the liquid to pass from the upper mark to the lower

mark is noted .5 -The process is repeated at 35°C and 45°C .

6 -The whole procedure is then repeated using the same volume of 3% sucrose .

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Calculation

1 -Regulate the data in such a table:

1/TT(K)=t+273Log η2η2t2d2t1d1η1t°C

From eq. (3)

ConstantConstantConstant25

ConstantConstantConstant35

ConstantConstantConstant45

2 -Find η2 from equation 3. 3 -A graph is then plotted of logη2 vs. 1/T. This graph should be a straight

line of slope E/2.303 R from which E may be determined .

Experiment (4)

Determination of molecular weight by elevation of the boiling point

Theory

The normal boiling point of a pure liquid or solution is the temperature which it’s vapor pressure equals 1 atm.

The boiling point of a liquid is a characteristic property which is often useful for purposes of identification and for the determination of purity.

When a non volatile solute is dissolved in a solvent, the vapor pressure of the latter is decreased as a consequence; the boiling point of the solution is higher than that of the pure solvent. The extent of the elevation (∆T) depends upon the concentration of the solute.

∆ T= Tb- To --------------- (1)

Where Tb is the boiling point of the solution and To is the boiling point of pure solvent.

The addition of a solute (A) to solvent (B) usually elevates the boiling point as in this equation:

∆ Tb = Kb m -------------- (2)

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)--------------- 3 (

) --------- 4 (

WhereMA= molecular weight of soluteKb= molal boiling point elevation constantWA= weight of solute (g)WB= weight of solvent (g)

∆Tb= the extent of the elevation of boiling point

Procedure

1- The boiling point apparatus is shown in Fig.22- 50ml of solvent (water) is placed in the boiling flask and heated by Mental

heater.3- When the boiling starts, read the thermometer;To

4- Let the apparatus to cool and after cooling place 1g of sample in the boiling flask, repeat the same procedure then read the thermometer;Tb

Fig. 2

Calculation

1 -Find ∆T by: ∆T= Tb- T0 2 -Find MA by equation (4) and write it’s unit.

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Experiment (5)

Determination of molecular weight by freezing point depression

Theory

The freezing point of a solute is lower than that of the pure solvent. Freezing point depression data are of considerable value in the thermodynamic study of solution.

The addition of a solute to a solvent, in general, lowers the freezing point of the solvent. For a given solvent, the freezing point lowering is directly proportional to the concentration of particles dissolved in it.

∆ Tf = To- Tf --------------- (1)

To = freezing point of pure solventTf = freezing point of solute in solvent(solution)

The molal depression constant(Kf) is characteristic of a solvent and is defined as the lowering of the freezing point caused by dissolving 1g molecule of solute in 1000g of solvent.

)---------------- 2 (

WhereMA= molecular weight of soluteKf = molal freezing point depression constantWA= weight of solute (g)WB= weight of solvent (g)

∆Tf = difference in the freezing point of pure solvent and solution

Apparatus and chemicals

Beaker, test tube, Beckman thermometer, Benzene, sample (solute), ice

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Procedure

1- A known weight of benzene (about 10g) is added to the center of the test tube.

2- The thermometer is immersed in the tube, then cooled by direct immersion in the ice bath with continuous stirring until the benzene starts to freeze, read the thermometer; To

3- Remove the tube from the ice bath and melt the benzene with gentle warming then add a known weight of an unknown solid to the benzene

4- Repeat the same procedure to determine the freezing point of the solution, Tf

Calculation

1 -Calculate ∆Tf ; ∆Tf = To- Tf 2 -Calculate MA from equation (2) and write it’s unit.

Experiment (6)

Surface Tension

Theory The molecules at the surface of a liquid are subject to the strong attractive forces of the interior molecules. A resultant force, whose direction is in a plane tangent to the surface at particular points, acts to make the liquid surface as small as possible. The magnitude of these force acting perpendicular to a unit length of a line in the surface is called the surface tension γ .

In the capillary –rise method, the liquid rises, because of its surface tension, in a capillary tube of small internal diameter immersed in it (provided that the liquid wets the tube) .

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The circular boundary line is located at some point above the meniscus and has a length 2 π r, where r is the inside tube radius. The force which causes the liquid to rise in the tube is 2 π r γ cosθ , where θ is the contact angle shown in Fig. 1 . At equilibrium the downward force mg due to gravity prevents the liquid from rising higher in the capillary. Here m is the mass of liquid in the capillary and g is the acceleration of gravity. For a liquid of density d rising to a height h in the capillary, this downward force is π r²hdg . At equilibrium this force is just balanced by the vertical force due to the surface tension , 2π r γ cosθ. For water and most organic liquids this contact angle is practically zero, this means that the surface of the liquid at the boundary is parallel with the wall of the capillary.

2π r γ = π r² hdg …………(1) γ = ½ hrdg …………….….(2)

Apparatus and chemicals Capillary tube, beaker, distilled water, organic liquid such as ethanol or acetone, traveling microscope, rubber tube.

Procedure

1- The capillary tube is cleaned.2- The capillary tube must be put in a beaker which contains 20ml of water

at 25ºC, then the water is raised slightly by gently blowing into the rubber tube and allowed to fall back to its equilibrium level.

3- The value of height of water (hH2O) inside the capillary tube will be read.4- Repeat the above procedure by using organic liquid instead of water, let is

be (hliq.).

10

ө

Fig.1

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Calculation

γ H2O = 72.14 dyn/cm 1. By h H2O we find (r)

γ H20 = h r d g /2 72.14 = ( h H2O× r × dH2O× 980)/2 r = ? cm

2. By r we find γliq.

γ liq = (h r d g)/2

γ liq = (hH2O × r ×dH2O × 980)/2

γ liq = ? dyn / cm

Experiment (7)

Heat of neutralization by calorimetry

Theory

In dilute solution strong acids and strong bases are completely dissociated to their ions. Furthermore, their salts are also completely dissociated in the solution. The neutralization of a strong acid by strong base may thus be written:

H+ + Cl- + Na+ + OH- NaCl + H2O

H+ + OH- H2O

The heat effect is therefore independent of the nature of the anion of the acid and the cation of the base. The heat of neutralization may be determined by simple calorimeter.

Apparatus and chemicals

Calorimeter, thermometer, stirrer, 0.1N KOH, 2N HCl

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Procedure

1- 100ml of 0.1N KOH is placed in a calorimeter, with confineous stirring record the temperature of the KOH solution every minute until 10min.

2- Add 16ml of 2N HCl to KOH solution and immediately record the temperature every minute until 10min.

Calculation

1- Plot a graph between temp.co and time then find ∆T

T2

Temp. oC T1

0 10 20 Time , min.

2- Calculate QQ = (m1s1 + m2s2) ∆T

m1, m2= mass of calorimeter (with thermometer and stirrer) and solution respectively.

s1, s2 = specific heat of glass and solution respectively (s1=0.16, s2=1)

3- Find the amount(weight) of KOH present in 100ml of 0.1N, let this be x

4- Calculate ∆H

Experiment (8)

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Heat of dissolution

Theory

Heat of dissolution can be defined as a quantity of heat which is formed during dissolving one mole of solute in a specific volume of a solvent.

Q = (m1s1 + m2s2) ∆T

Apparatus and chemicals

Calorimeter, thermometer, stirrer, KNO3

Procedure

1 -100ml of distilled water is placed in the calorimeter, with continuous stirring record the temperature of the water every minute until 10min.

2 -Add 3.5g of KNO3 to the water and immediately record the temperature , then take it every minute until 10min .

Calculation

1- Plot a graph between temp. oC and time then find ∆T

Temp oC

0 10 20

Time , min.

1- Calculate Q

13

T1

T2

Page 14: Stage 2 Physical Chem.experiment(1,2,3,4,5)111

Q = (m1s1 + m2s2) ∆T

2- Calculate ∆H

Where x is the weight of KNO3

Experiment (9)

Heat of solution from solubility Theory The variation of the solubility of a substance with temperature is given by the relation.

d lins ∆Hـــــــــــــــــــــــ = )1 --------------- (ــــــــــــــــ dT RT2

Where S is the solubility of the substance and ∆H is the heat of solution. This relation ship may be regarded as a from of the van't Hoff isochore . Assuming ∆H is constant between the temperasure T1 and T2 and integrating equation (1) between these limits

--------------- (2)

Where S1 is the solubility at the absolute temperature T1, and S2 is the solubility at the absolute temperature T2 .

If the solubility of a substance is determined at tow different temperature; its heat of solution may be calculated by application of equation (2). If more

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accurate data are required solubility may be determined at several different temperature and ∆H may be obtained from a plot of log S against 1/T .

Apparatus and chemicals Thermostats at 30, 40, 50,and 60 °C , benzoic aid potassium hydroxide (0.1N), pipette(25ml), ph .ph. indicator, cotton wool .

Procedure 1-250ml of KOH (0.1N) must be prepared. 2-1gm of benzoic acid is placed in a beaker which contains 100ml of hot water at about 70c.

3-The beaker is placed in the thermostat at 60c and leaving it for 15min. for thermal equilibrium. 4-A small piece of rubber tubing containing a cotton wool is attached to a 25ml pipette and 10ml of solution is withdrawn. (Note: the pipette may be wared before use in order to prevent the crystallization of the solutions at the higher temperature)

5-Put 10ml of solution in a conical flask which contain 30ml of hot water, then by using phenolphthalein as an indicator, titrate the solution with (0.1N) KOH and record the volume of KOH

6-Repeat these procedure from (3-5) by changing the temperature as (50,40 and 30°C).

Calculation

1-Culculate the concentration of benzoic acid at each temperature (S) (N.V)KOH =(N.V)b.q . →Nb.q=? = S

2-Plot between log S against 1/T

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log S

1/T

Experiment (10)Determination of solution composition by

Refraction Index

TheoryThe refractive index of a liquid can be determined by an Abbe′

refractometer. the ratio of the velocity of light in a vacuum to that in a medium, referred to the refractive index n, is readily determined by measuring the angles of incidence and refraction at an interface into a medium. The refractive index depends on the wavelength (of the light) and temperature, whish are usually specified with subscripts and superscripts, respectively. Thus nD

25 indicates a refractive index at 25co taken with the monochromatic yellow D light of the sodium arc. Measurements of refractive index are used to determine the concentration of solutions, to identify compounds, and to ascertain their purity. The specific refraction of a pure liquid is given by the formula

------------ (1)

Where n is the refractive index and d the density. The molar refraction R is given by the formula: R= r M ------------ (2)

Where M is the molecular weight. Molar refraction is an additive property; therefore, if it is determined for deferent members of a homologous series the contribution of the –CH2- group may be obtained. Molar refraction of mixture (Rm) can be calculated from the relation:

R m = X1 R1+ X2 R2 ------------- (3)

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Where X1 and X2 are mole fraction for component l and 2 , while R1 and R2 are molar refraction of component 1and 2 respectively.

Apparatus and chemicals Abbe′ retractometer, pipette, test tubes, dropper, ethanol, benzene

Procedure

1-Clean the prism, use a piece of cotton wool.

2-A few drops of the ethanol are placed on the ground – glass surface of the lower prism of the refractometer using dropper.

3- The prism box is closed and clamped. 4- The telescope is focused upon the cross hairs in the field by turnning the eyepiece. The edge of the dark band is brought to the intersection of the cross hairs and the compensator adjusted until the colored fringe disappears and a sharp – dark – white contrast is obtained .

5-The instrument is carefully adjusted until the intersection of the cross hairs and the dark edge of the band coincide.

6-The refractive index is read on the scale.

7-Take the refractive index for these mixtures and record the results in such a table:

No.of flasks 1 2 3 4 5 6 Sample

Ethanol(ml) 5 4 3 2 1 0 ?

Benzene(ml) 0 1 2 3 4 5 ?

n - - - - - - -

8-Take the refractive index of unknown (sample)

Calculation 1-Calculate the mole fraction for each test tube

nEthol

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XEthol = ــــــــــــــــــ nEthol + nBenz

Where X is mole fraction of ethanol ,n is number of moles .

2-Plot a graph between refractive index and mole fraction of ethanol

n

sample

X Ethol + X Benz = 1 :. X Benz = 1- X Ethol

X ethanol mole fraction of ethanol in the sample

3- Find the values of r, R and Rm by eq. 1, 2 and 3 respectively

Experiment (11)

An equilibrium constant by the distribution method

Theory

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The distribution coefficient, Kd of iodine between pure water and carbon tetrachloride,

can be determined by

Where C is the concentration of the iodine in organic and aqueous phase(determined by titration).

Then if instead of pure water, solution of potassium iodide is used as one of the phases, there will be an apparent increase in the solubility of the iodine which may be attributed to the rapidly reversible reaction KI + I2 → KI3

For which the apparent equilibrium constant is

The amount of free iodine in aqueous iodine solution cannot be determined by direct titration with standard thiosulfate solution, because as soon as the iodine is removed, the complex triiodide ion which is present dissociates to give more iodine. However, the concentration of unreacted iodine in this aqueous phase can be obtained by titrating the carbon tetrachloride layer and making use of the known distribution coefficient for iodine

(between the two pure liquids) .

The iodine combined with potassium iodide to from KI3 may be now determined, since the total iodine in the aqueous potassium iodide layer may be obtained by titration. The amount of iodide which was combined with the iodine can then be found. Since the original concentration of iodide is known, the amount of uncombined iodide may be obtained by difference.

Apparatus and chemicals Four conical flasks, 0.IN KI, I2, CCl4 , 0.1N Na2S2O3 , starch

Procedure

1- Prepare 250ml of 0.IN KI2- Add the solutions as arranged in this table:

No. of conical flask

Vol. of saturated soln. of I2 in CCl4

Vol. of H2O added(ml)

Vol. of 0.1N KI added(ml)

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(ml)

1 10 100 -

2 15 100 -

3 20 100 -

4 10 - 100

Then shake conicals well by shaker for 15min. 3-Leave the conical to separate to two layers; one of them is iodine dissolved in water, the other is iodine dissolved is CCl4 and separate two layers from each by separating funnel.4- Titrate 5ml of the organic phase for each conical with Na2 S2 O3 (0.I N).5-Titrate 50ml of the aqueous phase for each conical with Na2 S2 O3 (0.I N) by using starch as an indicator.

Calculation Find in each phase for first three conicals by:

Conical number 4 : - Let the total conc. of I2 in KI phase (aqueous) is equal to ,and can be find by:

- To find

Thus to calculate unreacted [I2] (free I2):

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To calculate [I2]reacted

To calculate [KI]unreacted

By substituting [I2] [KI] [KI3] in equation (1) Kc may be calculate

Experiment (12)

Phase diagram for a Binary system (phenol +Water)

Theory

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The phase diagram for a two- component system is the range of temperatures and compositions, in which they exist (solid and liquid) in equilibrium, defined by solids and liquids curves. There are three type of solution: 1-Miscible solutions: These solutions are completely miscible at any temperature, such as a solution of water and CH3COOH 2-Immiscible solutions: These are solutions which are not miscible with each other and not affected by temperature or any other factors, such as a solution of water and CCl4 .

3-Partially miscible solutions: These solutions are miscible at a definite temperature (they are affected by temperature), such as a solution of water and phenol.These are different phase diagram of binary system

Tc(max) Tc(max)

Temp.Temp. Temp. Tc(mini) Tc(mini)

Xc Xc

H2O Phenol H2O Isopropanol H2O Nicotine Composition Composition Composition

Where Tc is the critical temperature in which the two components are miscible, Xc is the critical composition in which the two components are miscible with each other.

Apparatus and Chemicals Thermostat bath, conical flask, Sensitive balance, thermometer, phenol, distilled water.

Procedure

1- Place 3g of phenol in a conical flask.

2- 1.5ml of water is added to the phenol, then placed in a thermostat bath and gently warmed until the solution become one phase at this time read the temperature (Ta), then cool the solution and with appearing the turbidity read the temperature (Tb).

3- Take the mean of temperature, and let it will be (T1).

4- Repeat the steps (2 and 3)by adding another four 1.5ml of water and let the temperature will be T2, T3, T4, T5 and the total added water will be 7.5ml.

5- Add 0.5ml of water and repeat steps 2 and 3, look if the temperature decreased add another 1.5ml of water five times, otherwise; if the temperature not decreased you must add another 0.5ml of water until the temperature decreasing, all temperatures must be recorded.

Calculation

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1-After taking the mean of temperatures, find %Wphenol at each addition like this:

2-Plot a diagram between the temperature and %WPhenol, then find the critical temperature and critical composition of the solution.

Tc

Temp.

Xc

%WPhenol

Experiment (13)

The radius of molecule from viscosity measurements

Theory The ratio of the viscosity η of a solution of large spherical particles to the viscosity of a pure solvent ηo is related to the fraction of the total volume of spheres per milliliter of solution by the expression , derived by Einstein ,

This equation may be rewritten:

Where r is the radius of the particle and C is the concentration of the particles in moles/L. Hence if η / ηo is plotted against C a straight line is obtained and r may be determined from the slope. The relative viscosity η / ηo may be determined using the relationship

In this equation t and to refer to the time of flow through the capillary of a given volume of the solution and pure solvent, respectively and d and do are the densities of the solution and pure solvent respectively.

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Apparatus and Chemicals Viscometer, stop watch, water, glycerol.

Procedure

1- The time of flow(to) of 50ml of water is determined by using the viscometer. 2- Prepare 100ml of 1M glycerol. 3- Dilute the glycerol solution to ( 0.2 , 0.4 , 0.6 , 0.8 M) and measure the time of flow(t)

for each dilution using the same volume as before, beginning from 0.2M solution.

Calculation

1- Results are recorded in such a table:

Conc. of glycerol soln.,

Mt, sec to ,sec

0.2

0.4

0.6

0.8

1.0

2- Find by

3- Plot a graph between η / ηo Vs. concentration

Slope = 6.3 × 1021 r3

r3 = ? η / ηo r = ?

Conc., M

Experiment (14)

Determination of molecular associationdegree of benzoic acid in benzene

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Theory

The addition of a solute to a solvent, in general, lowers the freezing point of the solvent. In this experiment the molecular weight of benzoic acid can be determined in benzene; this method is named cryoscopic method. Always the detected value (measured value)of molecular weight by this method is differ from that of the true value (actual value), due to the association of molecules, it means that two or more molecules were joined to from a big molecules . When the solute is dissociated to ions, each ion has it’s effect on increasing ∆T , and by this the measured molecular weight is decreased, thus dissociation degree can be found by

------------- (1)

Where is the dissociation degree Mo : true molecular weight of benzoic acid Mr : measured molecular weight of benzoic acid

n : number of dissociate ion of benzoic acid

While if the solute associated in solvent, the value of ∆T is decreased and the measured molecular weight is increased

Where is the association degree

Mo : true molecular weight of benzoic acid Mr : measured molecular weight of benzoic acid

n : mole numbers of solute( )

Apparatus and Chemicals

Freezing point apparatus, Beckman thermometer, benzene, benzoic acid, ice

Procedure

1- Add a known volume of benzene (10ml) is add to the center of the tube.2-The tube is cooled by slightly immersion in the ice bath and stirred continuously until the benzene starts to freeze, then read the temperature of the thermometer (To).3- Add 0.05g of benzoic acid and then record the freezing point of the solution (T1).

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4-Repeat step (3) three times, by adding 0.05g at each case to the same solution, then record the freezing point of each solution (T2, T3, T4) respectively.

Calculation

1- Find ∆ T in each case(∆ T1, ∆ T2, ∆ T3, ∆ T4) by ∆ T1 = To –T1

2- Calculate the concentration of each solution of benzoic acid in benzene. 3- (Note: W1 = 0.05g , W2 = 0.1g , W3= 0.15 , W4 = 0.2) 4- Plot a graph between the depression of the freezing point and concentration of the

substance.

∆ T

Slope = Kf benzene

Conc. of benzoic acid, M

5- Calculate the molecular weight ( ) for each solution

6-

7- Find

Experiment (15)Phase Diagram of three components

System

Theory According to the phase rule of Gibbs, the variance F (number of degree of freedom) of a system at equilibrium is equal to the number of components c

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minus the number of phases p plus 2 , provided that the equilibrium is influenced only by temperature , pressure and concentration. F=c– p + 2 The variation F is smallest number of independent variables required to completely fix the state of the system. This experiment is carried out at a constant temperature and pressure so that these are not variables. Thus eq. (1) becomes F = c– p And for a three – component system F=3 – p . Thus in a three – component system if only one liquid phase is present, F = 2 and the concentration of two of the chemical substances must be specified in order to describe the system completely. If two immiscible liquid phase are present in equilibrium, F=1 and the concentration of only one component needs to be specified. It is convenient to represent a three component system on a triangular diagram such as that illustrated in fig (1)

In an equilateral triangle, the sum of the perpendiculars from a given point to the three sides is a constant . The perpendicular distance from each apex, representing a pure compound , to the opposite side is divided to 100 equal parts , corresponding to percent , and labeled along the side at the right of the perpendicular .thus point (X) corresponding to a composition of 25 percent B, 25 percent C and 50 percent A . The components benzene and water are essentially immiscible hence two layers will be obtained on mixing .The third component ( ethanol ) , is soluble in each layer and on addition to a mixture of benzene and water distributes itself between these layers . The composition of the layers changes as more ethanol is added. Under these conditions, P equals 2 , and the system is completely defined by the composition . Thus if the points corresponding to these compositions are plotted, a smooth curve may be drawn indicating the limits of miscibility of water – benzene mixtures in ethanol as in Fig (2) B

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B

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Fig (2)

Apparatus and Chemicals

Five conical flask (25 ml ) , benzene , water , ethanol , 5ml pipette , burrette .

Procedure

1- Prepare the following mixtures

No. of Conical Flask

Vol.of water added(ml)

Vol.of Benzene(ml)

1 1 52 2 43 3 34 4 25 5 1

2- For conical number one , add ethanol slowly until the mixture converts from a turbid to a clear solution by vigorously shaking the mixture . The volume of ethanol which has been added is then recorded .

3- Repeat step 2 for each conical and record the volume of ethanol added.

Calculation

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1. By knowing the density of water,benzene and ethanol, calculate the weight of each component in the conical flask.

dwater= 1.00 g/mldBenzene= 0.87 g/mldEthanol= 0.79 g/mlwt = d × v

2. Calculate the %wt of each component in the conical flask.

3.Plot an equilateral triangle, each side equal to 10 cm. 4 .Put the datas on the diagram, and find the degree of freedom

at miscible region and immiscible region .

Experiment (16 )Fractional Distillation

Theory

The separation of liquids by distillation is one of the oldest operations of chemistry. The separation of two liquids which is obtained by a simple vaporization and condensation is not affective expect in the case of liquids with widely differing boiling points. Greater separation may be achieved by a series of simple distillation, but this is laborious. The same result is obtained by using a fractionating column through which the vapor is passed and brought into contact with part of the condensate flowing down the column. The less volatile components in the ascending vapor are condensed in such a column, and the more volatile components are boiled out of the descending liquid phase, so that the distillation through the column is equivalent to a number of successive simple distillations.

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The effectiveness of a distilling column is expressed in terms of the theoretical plate. The theoretical plate is a hypothetical section of column which produces a separation of components such that the vapor leaving the top of the section has the composition of the vapor which is in equilibrium with the liquid leaving the bottom of the section. The number of theoretical plates cannot be determined for the geometry of the distilling column; it is calculated from the separation effected with a liquid mixture for which the liquid – vapor equilibrium data are fully known.

Apparatus and chemicals

Abbe refractmeter, fractional column, 250 ml boiling flask, benzene and carbon tetra chloride.

Procedure

1-The distillation apparatus is shown in fig (3) 2-Place 40ml benzene and 10ml CCl4 in the boiling flask and

the mixture is boiled vigorously .3-After the distillation is take place, switch off the heater.4-Two samples are taken from the remained and distillate

respectively .

5-Perpare these solution No.of Conical

FlaskVol. of

benzene(ml)Vol. of

CCl4(ml)n

1 0 52 1 43 2 34 3 25 4 16 5 0

Remain - -Distilled - -

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6-Take the refractive index (n) for each solution, remained and distillated samples.

Calculation Calculate the mole fraction of CCl4 for each conical flask

Plot a graph between the refractive index of the solution and the mole fraction of CCl4

put the refractive index of the two samples(remained and distillated) on the graph, then detect the mole fraction of CCl4 for them as in this Fig. n

Plot between the following values:

mole fraction of CCl4 in

liquid13.64 21.73 29.44 40.57 52.50 62.20 72.20

mole fraction of CCl4 in

vapor15.82 27.15 36.15 47.50 57.10 63.80 73.30

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XCCl4 (in liquid)

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XCCl4(remained) XCCl4(distillate) XCCl4 in liquid

The theoretical plates can be found from the curve by this equation Number of theoretical plate = No of columns – 1

Experiment ( 17 )Determination of the molecular weight of a polymer

from viscosity measurements

Theory

Measurements of viscosities of high – polymer solutions offer an indirect method for determining molecular weight. The theoretical background for this method starts with Einstein's derivation ,

----------------(1)

where η is the viscosity of solution , ηo is the viscosity of the solvent. The quantity (η / ηo ) is of frequent – occurrence in the theory of viscosity and is known as the specific viscosity , ηsp . Because of the difficulty of knowing the fraction of the volume occupied by high – polymer molecules in solution and the fact that the reduced viscosity ηsp / c , is not independent of concentration , it is necessary to utilize the limiting viscosity number { η } defined by

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-------------------(2)

Where C is the concentration of the high – polymer in grams per ml . The limiting viscosity number is obtained by plotting the ratio of specific viscosity to the concentration against concentration for series solution and extra polting to zero concentration. For a series of samples of the same polymer in a given solvent and at a constant temperature the following empirical relation is obeyed quite well ----------------- (3) Here K and are constants which may be determined by measuring the intrinsic viscosities of a series of samples of a polymer for which the molecular weight have been measured by another method.

Apparatus and chemicals Viscometer , stop watch , 25ml volumetric flasks , 25ml conical flasks , poly styrene , toluene . Procedure

1- Solutions of poly styrene sample of unknown molecular weight ( 0.1gm , 0.2 gm , 0,3 gm , 0.4 gm , 0,5 gm ) are prepared in pure toluene .

2- The flow time in the viscometer is determined for toluene (to)3- The flow time for the solutions of polystyrene in toluene is determined (ti)

Calculation1. To calculate η / ηo , the bellow equation must be used

Let d/do =1 for easing

2- Plot a graph between ηsp / C and C

0.10.20.30.40.5

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K = 3.7×10-4

α = 0.62

C (M)

3-Find M by

Experiment (18)Determination of molecular weight by steam

distillation

Theory If two immiscible liquids such as bromo benzene and water are distilled from the same vesel, since one dose not affect the vapor pressure of the other, they will pass over in the ratio of their vapor pressures until one of them is completely distilled. Furthermore , the vapor pressure of the mixture will be equal to the sum of the vapor pressure of the individual components, i.e.

Ptotal =PBr-b+PW ……………..(1)

At the boiling point (PBr-b+PW) will then be equal to the atmospheric pressure. At this temperature the mixture distils in the molecular proportions PBr-b/PW . Hence if WBr-b and WW are the Weights in grams of bromo benzene and water in the distillate , then

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---------------(1)

Hence the molecular weight of bromo benzene can be found by the steam distillation method.

Apparatus and chemicals Steam distillation, thermometer , graduated cylinder , separating funnel , water and bromo benzene .

Procedure

1-Add 25ml bromo benzene and 100ml of water to the boiling flask, then operate the heater of the steam distillation apparatus .

2-When the mixture begin to distillate, recorde the temperature, and the steam distillation should proceed at the rate of about 1 drop per second .

3- Collect about 30ml of the distillate.

4-Distillation is stopped when the temperature commences to rise to the b.p. of water .

Calculation

1- Find the vapor pressure of water if you know that each increase or decrease by one degree centigrade in boiling point causes the change in vapor pressure about 27mmHg . Assume that the temp. of the mixture distillation=94oC 100- 94 = 6 oC 6 ×27= 162 mmHg 760 – 162 = 598mmHg

2- Calculate from knowing the density of each of them .

3-Find MwtBr-b by equation (1)

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