Keywords
secondary interaction,
hydrodynamic volume
But before we talk more about molecular weights, let's first let's ask a question:
For one, polymers move very slowly, or at least, they move a lot more slowly than do small molecules. It makes sense that the faster molecules in a liquid move, the more easily the liquid will flow. So when we dissolve a polymer in a solvent, their slow motion makes the whole solution more viscous.
To understand, it helps to think about a fabulous three-day holiday weekend. You're leaving town for the holiday, going on a road trip with a few of your favorite co-conspirators. You pile into your sleek, fast convertible and hit the highway, in search of adventure. But soon after merging into the fast lane you notice that your pulse is slowing a good deal. The wind that had been blowing furiously through your rebelliously wild hair has diminished to gentle summer breeze as your velocity drops. Your engine bogs down, and you have to shift down into fourth, then third, in order to keep your engine revved at these incredibly slow speeds. "How slow?" your mind wonders in frustration, as you glance at your speedometer, which now reads a paltry forty-five miles per hour!
Far ahead, in front of a long line of equally slow moving sleek convertibles, all of them in third gear, you spot a large spare tire cover which reads, "The Happy Hattson Family, Forestdale, Wisconsin". Attached to that spare tire cover is a monstrous and menacing motor home, covered in bumper stickers chronicling its many journeys to vacation heavens like Gatlinburg, Tennessee and Branson, Missouri. The motor home, filled with Happy Hattsons, is chugging away at a pace that would make a snail blush. With bitter resignation you come to accept the fact that you will be a bit late getting to your destination.
That's how it is with polymers and small molecules. The big giant motor home moving slowly in the fast lane slows down ALL the traffic on the highway. In the same way, slow moving polymers get in the way of the fast moving solvent molecules when they try to flow. So the whole solution moves more slowly, and becomes more viscous.
What's worse is that the polymer molecules do more than just block the motion of the small molecules. They also slow them down through intermolecular forces. If there are any attractive secondary interactions between the polymer and solvent molecules, the small solvent molecules can become bound to the polymer. When this happens they move with the polymer more or less, and of course, they have to move at the polymer's slow speeds. It might help to think of a small asteroid, hurtling through space, and being captured by the gravity of a large planet and becoming a satellite. In the same way, a solvent molecule coming too close to the polymer molecule will get captured and become a "satellite" of the polymer molecule.
For most every polymer there's a definite relationship between molecular weight and viscosity. So, measure the viscosity, and we can get the molecular weight. And that's just what we're going to talk about next, measuring the viscosity of a polymer solution.
So now we know how to measure the time it takes for the solution level to drop, called an efflux time, I'll tell you some more details. We don't just do one measurement. We measure efflux times for solutions of our polymer solution at varying concentrations. We also, for comparison measure the efflux time of the pure solvent, with no polymer dissolved in it.
So what do we do with these numbers? The first thing we do is we give a name to one of them. We give a name to the efflux time of the pure solvent. We call it t0. Then we start to do some number crunching. The first thing we do is calculate the viscosity of the polymer solutions to the viscosity of the pure solvent. We do this by taking the efflux time of the polymer solution at a given concentration (we call this t) and dividing it by t0, the efflux time for the pure solvent. This gives us what we call the relative viscosity. We use the Greek letter h to denote the relative viscosity.
When we make this plot, we call the slope of the plot k'. We also
extrapolate back to zero concentration, and call the y-intercept
the
intrinsic viscosity. (The intrinsic viscosity is a hypothetical
construct. As viscosity varies with concentration, the intrinsic
viscosity is the hypothetical viscosity at a hypothetical "zero
concentration".) Think about this. If you can remember
your high school algebra you might notice that this gives us an equation
in slope intercept form. You know, the old y = mx + b, where
Of course, k'[n]2 is our m, the slope of the
line; and [n] is our b, the y-intercept. The intrinsic
viscosity is an important number, because it's the one that will tell us
the molecular weight, momentarily.
But first, you may want to take a break and go get a snack, or a drink of
water, or something right now.
Are you back? Obviously, or else you wouldn't be reading this. Before
we go and calculate our molecular weight from the intrinsic viscosity, I
must tell you a second way to calculate the intrinsic viscosity. Remember
the old relative viscosity? I told you we'd be using it, and that's just
what we're going to do right now. Let's take the natural logarithm of the
relative viscosity, and let's divide that number by the concentration of
the solution we measured. This gives us a number we call the inherent
viscosity.
Now just like the reduced viscosity, there's a different inherent
viscosity for each concentration you measure. So, we can make a plot of
inherent viscosity on the y-axis, and concentration on the
x-axis. Then we get a plot that looks like this:
Again, [n] is our slope intercept, but our slope this time is
different, it's k'' [n]2. Yes, our plot is once
again a line described by an equation is slope intercept form. Want to
see it? Here it is:
Now we usually figure up our intrinsic viscosity using both methods. If
they agree, then we know we've done everything right. We usually put the
plots from both methods together to get a plot that looks like this, with
the two lines meeting at their common intercept:
Another way to
tell if you've done everything right is that k' - k'' should equal
0.5
This is called the Mark-Houwink equation. M is what we call
the viscosity average molecular weight (at last1) and K' and
a are the Mark-Houwink constants. There is a specific set
of Mark-Houwink constants for every polymer-solvent combination. So you
have to know these for your polymer-solvent combination in order to get an
accurate measure of molecular weight. This means that you can't get a
good measure if you're measuring a polymer that you've just invented and
there are no calculated Mark-Houwink constants available. But it still
can give you a qualitative idea of whether molecular weight is high or
low. The mere fact that you get an intrinsic viscosity can tell you a
lot, too. Sometimes that's the only way you can tell that what you
have made is indeed a polymer.
One last note: You have to use dilute solutions to do this kind of
experiment. If the solutions are too concentrated, the polymer molecules
might get close enough together to interact with each other. This
causes the viscosity to increase in ways that our equations here don't
describe very well, so accurate measurements can't be made. That's why
this technique is called dilute solution viscometry.
Want to know some other ways of measuring molecular weight? Visit these
pages!
We've done an awful lot of number crunching here, but we still
haven't gotten a molecular weight. Are we ever going to?
Okay, okay, be patient. I had to go around just now because we need the
intrinsic viscosity [n] to calculate molecular weight. We calculate it
with a simple little equation:
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