Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D.,...

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Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04
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Transcript of Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D.,...

Page 1: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Surface Tension

Spring 2004 BIOEN 301

Extra bonus lecture!

WILL NOT BE ON FINAL!

F. Reitz, Ph.D., 6/2/04

Page 2: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

more bugs that think they’re all that and a bag of chips: the Water Strider

http://www-math.mit.edu/~dhu/Striderweb/striderweb.html

Page 3: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Water striders are light (like ants) thus don’t “break” surface

http://encarta.msn.com/encnet/refpages/RefMedia.aspx?refid=461560390

• Ooh! Look at me! I have hydrophobic feet and I weigh less than Fritz does! I’m soooo great!

Page 4: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Even a piece of steel can do this trick if it is small (steel ~ 8x water)

http://www.sita-messtechnik.de/englisch/oberfl/

Page 5: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

4 H2O molecules

separated in space from each otherhave partial + and – charges

what would they do???

but what’s surface tension, really?

Page 6: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

4 H2O molecules

they clump together

+ and – charges snuggle up close

potential energy of system has dropped

Page 7: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Surface Tension

http://hyperphysics.phy-astr.gsu.edu/hbase/surten.html

water in bulk has many binding partners

water at surface has less, has exposed charges left over

potential energy of water at surface is higher

deforming droplet to increase surface area takes work

Page 8: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Surface Tension

E = FX, energy = force * distance

dE = F dX F = dE/dX

e.g. spring energy = ½ kx2, dE/dX = kx = F

Page 9: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Surface Tension

creating surface area in 20C water droplet takes

73 ergs/cm^2 droplet thus

seems springy if mg << l it

dominates and you can walk on water (Vogel pp 72, 104-109)

Page 10: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Surface Tension

surface area in 20C water costs

73 ergs/cm2

= “ ”

Page 11: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Surface Tension

surface area in 20C water costs

73 ergs/cm2

F = dE/dX

can get from F in this apparatus

if film is w by w cm, how much area has been created?

Page 12: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Surface Tension

2 W2

Page 13: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Surface Tension

2 W2

(front and back side)

Page 14: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

OK so remember this? (steel ~ 8x water)

http://www.sita-messtechnik.de/englisch/oberfl/

Page 15: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Floating without floating – The SECRET OF THE STRIDERS REVEALED!!! = 73 ergs/cm2 = 73 dyne-cm/cm2 = 73 dynes/cm 73 dynes/cm is also like a tear strength if we stacked poker chips on water it might look like below area of chip doesn’t matter so much as the edge (vertical

contributions) lift = perimeter * * sin wait, why sin ? why not pull them all at 90 degrees?

Page 16: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Floating without floating -

is constant of water / air interface, so can’t just “choose” to pull less

surface fails when tension along perimeter of chips exceeds 73 dynes/cm

after that, the water does something else more energetically profitable –

Page 17: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Incidentally – Scaling tie-in - Why droplets are droplet-sized -

mass increases faster than length or area, so above about 1 cm diameter, water droplet mg > l, so more likely to get torn apart by its own weight

Page 18: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Floating without floating - anyway so if the outlines of your feet are long enough for L to

add up to more than your weight (and your contact angle is high) you too can walk on water

Page 19: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

“and your contact angle is high”? need to push off water, not have it wick up onto you contact angle is a measure of hydrophobicity among other things “other things”?...

Page 20: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Contact Angles

here’s a droplet on a surface -

Page 21: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Contact Angle

here’s a slice of it –

tangent to droplet edge is “contact angle”

why is theta theta?

Page 22: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Contact Angle

balance of forces

surface tension pulls up

gravity & adhesion pulls down

what are the other two?

Page 23: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Remember this?

http://hyperphysics.phy-astr.gsu.edu/hbase/surten.html

water at surface has less binding partners

energy at surface is higher

Page 24: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

What if -

http://hyperphysics.phy-astr.gsu.edu/hbase/surten.html

what if the circles are aluminum atoms in a solid?

what if the space above it is liquid ethanol?

Page 25: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Contact Angle

F = dE/dX

surface/air & surface/water interfaces also have “surface tension”, in ergs/cm2

moving water edge back and forth incurs energy costs/profits

but units of F are energy/distance, not area?! what’s the deal?

Page 26: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Contact Angle

problem is 3-D

surface tension is force per length

each dL of perimeter contributes dL force

F = dE/dX => dL

dE = dL dX = dA

back to ergs/cm2

Page 27: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Obtuse contact Angles

hydrophobic surface

“gravity & adhesion” is now “gravity & repulsion”

if no gravity, drop leaves

Page 28: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Contact Angle

why doesn’t drop pull or push itself along the surface?

it did when initially set down, it distorted itself until equilibrium reached

edge equilibrium is one thing

equilibrium between (roundness) & gravity (flatness) & surface coverage (adhesion/repulsion) is another factor...

Page 29: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

surface adhesion energy

Page 30: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

surface adhesion energy

The water at this surface is at a lower potential energy than the bulk water, so deformations that increase this surface area are favorable and spontaneous

Page 31: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Same thing as drop on surface, different geometry

so fluid scoots along the surface until equilibrium reachedlike water rising in a tube until forces add to mg (gravity) = r2 h gsurface tension trying to pull water up tube rather than round up a beadequivalently - surface energies are being minimized

dE = F dX = dL dX = dA

Page 32: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Capillary action

the fluid meets the glass at an angle which depends on the glass properties

the surface tension in the tube acts around the perimeter 2 r

if surface tension is T, total vertical force is 2 r T cos equating forces gives

h = 2 T cos / (r g)

Page 33: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

An example from nature - xylem

channels in plants that draw up water

Page 34: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Current record holder for world’s tallest tree

“Stratosphere Giant”, sequoia, 112.6 m tall

this is a formidable water head

can surface tension really bring water from the roots up to the top?

Page 35: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

And the answer is…

xylem contact angle ~ 50°

vessel diameters go down to ~ 30 microns

h = 2 T cos / (r g)

if T = 73 dyne/cm, r = 15 microns, = 1 g/cm3, g = 981 cm/s2, h = ??? …

drumroll please -

Page 36: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

h = 87 cm

ahem

apparently osmotic effects (root pressure, evaporation) dominate

Page 37: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Back to this -

http://hyperphysics.phy-astr.gsu.edu/hbase/surten.html

water at surface has less binding partners

potential energy of water at surface is higher

what if we do this…

Page 38: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Hmm… what molecule is that?how does surface water energy change?what happens to surface tension?

Page 39: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

Soap! this particular detergent molecule is SDS (sodium dodecyl sulfate, minus the Na+)

water happy, SDS happy

tension reduced

Page 40: Surface Tension Spring 2004 BIOEN 301 Extra bonus lecture! WILL NOT BE ON FINAL! F. Reitz, Ph.D., 6/2/04.

We now have COMPLETE POWER OVER WATER STRIDERS!!!

simply add soap and they’re SCREWED!

HA HA!

and so it is that we have the last laugh