BioG 1105-1106 at Cornell University
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Unit 1: Demos

Objective 1:

The Octet "Rule"

Objectives 2 and 3:

Electronegativity
Polarity and Chemical Bonds

Objective 7:

Wettability and Capillarity
Density of ice/water

Objective 8:

Hydrophobic, hydrophilic, and detergents
How does dry cleaning work?
Water as a Solvent

Objective 9:

Buffers (9c) (optional)

Objective 13:

Saturated v. unsaturated fats (13a)

Objective 17:

Protein structure

Objective 18:

Folding of long polypeptides in water
New research on Parkinson's disease emphasizes the importance of a protein's shape on its function

Optional Supplementary Material:

Caught on Tape: A different way to stay clean (and sticky)
Sticky Feet: On geckos and Spider-man

Wettability and Capillarity

Water molecules are attracted electrostatically to areas of charge on dissolved ions or polar molecules, and are also attracted to charged groups on a hydrophilic surface such as glass. Consequently, such surfaces are wettable, in the sense that water spreads over them and binds loosely to them. By contrast, hydrophobic surfaces, such as those of most plastics and waxes, lack surface charge and hence are not wettable; water on them will form isolated droplets, but will not spread out over the surface.

The readiness of water to bind to hydrophilic surfaces explains the phenomenon of capillarity audio—the tendency of aqueous liquids to rise in narrow tubes. If the end of a narrow glass tube is inserted below the surface of a volume of water, water will rise in the tube to a level well above the water level outside (see Figure). The reason is that glass is very hydrophilic, having many charged groups on its surface. The water molecules, electrostatically attracted to the glass, tend to creep upwards along the surface of the tube and to pull other water molecules (linked to them by hydrogen bonds) along with them. The water level stops rising when the pull of gravity just counteracts the electrostatic forces that contribute to capillarity. The larger the diameter of the tube, however, the smaller the percentage of waster molecules in direct contact with the glass and, correspondingly, the smaller the rise in the water in the tube. Even though the relatively few molecules in contact with the glass have a tendency to creep upward, they are held back by their cohesion via the network of hydrogen bonding with the rest of the water in the tube.

Capillarity is by no means restricted to glass tubes. Water will climb any charged surface. We are all familiar with the way it climbs up the fibers of paper towels and spread through the fibers of many kinds of cloth.

Water rises higher in a glass tube of small bore (left) than in one of large bore (center) because in the smaller tube a higher percentage of the water molecules are in direct contact with the glass and can form hydrogen bonds with charged groups on the glass. By contrast, water cannot “stick” to the surface of a plastic tube (right) because plastic is uncharged.

© BIOG 1105-1106