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Osmotic pressure measurements can be used to determine the molecular weights of large molecules such as proteins. For a solution of large molecules to qualify as "dilute," its molar concentration must be very low and hence the osmotic pressure can be too small to measure accurately. For this reason, the usual procedure is to measure the osmotic pressure at a variety of concentrations, then extrapolate the results to the limit of zero concentration. Here are some data for the protein hemoglobin dissolved in water at 3oC:

Concentration (grams/liter)h (cm)
5.62.0
16.66.5
32.512.8
43.417.6
54.022.6

The quantity his the equilibrium difference in fluid level between the solution and the pure solvent,. From these measurements, determine the approximate molecular weight of hemoglobin (in grams per mole).

An experimental arrangement for measuring osmotic pressure. Solvent flows across the membrane from left to right until the difference in fluid level,h, is just enough to supply the osmotic pressure.

Short Answer

Expert verified

The approximate molecular weight is 66.3kg/mol.

Step by step solution

01

Step 1. Given Information

We are given a table,

02

Step 2. The osmotic pressure 

For dilute solutions, the osmotic pressure can be approximated as,

π=nRTV

π=nRTV=cRTM

Therefore,

M=cRTπ

Here the number density of the solute nVin moles/liter is replaced by cM, cis the concentration of the solute in (grams/liter) and Mis its molecular weight (in grams/mole). But in this experiment the osmotic pressure is balanced by the difference in the fluid level hso for each solute concentration, one can calculate the osmotic pressure by the following formula,

π=ρgh

Substitute ρghfor πin the equation M=cRTπ

π=nRTV=cRTM

Use the density of water ρ=1g/cm3. The table given below shows the value of the osmotic pressure for each solute condition and the corresponding estimated value of the molecular weight from the following relation,

03

Step 3. Consider the following table,

The table is as follows,

Concentration
grams/liter=kg/m3
hcm
πN/m2
Mkg/mole
5.62.0196.265.5
16.60.5637.659.7
32.512.81255.759.4
43.417.61726.657.7
54.022.62217.155.9
04

Step 4. Graph of concentration versus molecular mass

The graph of concentration versus molecular mass is as follows,

05

Step 5. Approximated Molecular Weight

The molecular weight estimated from each measurement is plotted versus the concentration. As the equation that relates osmotic pressure to the concentration of solutes is most accurate in the limit of very dilute solution, one should extrapolate the results to zero concentration. If apparently one bad point at c=16.6g/Lis ignored, the molecular weight is M=66.3kg/mol. Therefore, the approximate molecular weight is66.3kg/mol

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Most popular questions from this chapter

For a magnetic system held at constant TT and HH (see Problem 5.17 ), the quantity that is minimized is the magnetic analogue of the Gibbs free energy, which obeys the thermodynamic identity

Phase diagrams for two magnetic systems are shown in Figure 5.14 ; the vertical axis on each of these figures is μ0Hμ0H (a) Derive an analogue of the Clausius-Clapeyron relation for the slope of a phase boundary in the HH - TT plane. Write your equation in terms of the difference in entropy between the two phases. (b) Discuss the application of your equation to the ferromagnet phase diagram in Figure 5.14. (c) In a type-I superconductor, surface currents flow in such a way as to completely cancel the magnetic field (B, not H)(B, not H) inside. Assuming that MM is negligible when the material is in its normal (non-superconducting) state, discuss the application of your equation to the superconductor phase diagram in Figure 5.14.5.14. Which phase has the greater entropy? What happens to the difference in entropy between the phases at each end of the phase boundary?

Because osmotic pressures can be quite large, you may wonder whether the approximation made in equation5.74is valid in practice: Is μ0really a linear function of Pto the required accuracy? Answer this question by discussing whether the derivative of this function changes significantly, over the relevant pressure range, in realistic examples.

μ0T,P2μ0T,P1+P2-P1μ0P......equation(5.74)

Repeat the preceding problem with T/TC=0.8

Use the data at the back of this book to verify the values of Hand G quoted above for the lead-acid reaction 5.13.

Use a Maxwell relation from the previous problem and the third law of thermodynamics to prove that the thermal expansion coefficient (defined in Problem 1.7) must be zero at T=0.

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