Drop (liquid)

Surface tension

Liquid forms drops because it exhibits surface tension.

A simple way to form a drop is to allow liquid to flow slowly from the lower end of a vertical tube of small diameter. The surface tension of the liquid causes the liquid to hang from the tube, forming a pendant. When the drop exceeds a certain size it is no longer stable and detaches itself. The falling liquid is also a drop held together by surface tension.

Viscosity and pitch drop experiments

Main article: Viscosity, Pitch drop experiment

Some substances that appear to be solid, can be shown to instead be extremely viscous liquids, because they form drops and display droplet behavior. In the famous pitch drop experiments, pitch – a substance somewhat like solid bitumen – is shown to be a liquid in this way. Pitch in a funnel slowly forms droplets, each droplet taking about 10 years to form and break off.

Pendant drop test

In the pendant drop test, a drop of liquid is suspended from the end of a tube or by any surface by surface tension. The force due to surface tension is proportional to the length of the boundary between the liquid and the tube, with the proportionality constant usually denoted \gamma.{{cite book

: ,F_{\gamma} = \pi d \gamma

where d is the tube diameter.

The mass m of the drop hanging from the end of the tube can be found by equating the force due to gravity (F_{g} = mg) with the component of the surface tension in the vertical direction (F_{\gamma} \sin \alpha) giving the formula

: ,mg = \pi d \gamma \sin \alpha

where α is the angle of contact with the tube's front surface, and g is the acceleration due to gravity.

The limit of this formula, as α goes to 90°, gives the maximum weight of a pendant drop for a liquid with a given surface tension, \gamma.

: ,mg = \pi d \gamma

This relationship is the basis of a convenient method of measuring surface tension, commonly used in the petroleum industry. More sophisticated methods are available to take account of the developing shape of the pendant as the drop grows. These methods are used if the surface tension is unknown.{{Cite journal |archive-url=https://web.archive.org/web/20081217040101/http://www.firsttenangstroms.com/pdfdocs/STPaper.pdf |archive-date=2008-12-17 | access-date = 2008-11-05}}{{cite journal

Drop adhesion to a solid

The drop adhesion to a solid can be divided into two categories: lateral adhesion and normal adhesion. Lateral adhesion resembles friction (though tribologically lateral adhesion is a more accurate term) and refers to the force required to slide a drop on the surface, namely the force to detach the drop from its position on the surface only to translate it to another position on the surface. Normal adhesion is the adhesion required to detach a drop from the surface in the normal direction, namely the force to cause the drop to fly off from the surface. The measurement of both adhesion forms can be done with the Centrifugal Adhesion Balance (CAB). The CAB uses a combination of centrifugal and gravitational forces to obtain any ratio of lateral and normal forces. For example, it can apply a normal force at zero lateral force for the drop to fly off away from the surface in the normal direction or it can induce a lateral force at zero normal force (simulating zero gravity).

Droplet

The term droplet is a diminutive form of 'drop' – and as a guide is typically used for liquid particles of less than 500 μm diameter. In spray application, droplets are usually described by their perceived size (i.e., diameter) whereas the dose (or number of infective particles in the case of biopesticides) is a function of their volume. This increases by a cubic function relative to diameter3/6000 to convert μm into picolitres)--; thus, a 50 μm droplet represents a dose in 65 pl and a 500 μm drop represents a dose in 65 nanolitres.

Speed

A droplet with a diameter of 3 mm has a terminal velocity of approximately 8 m/s. Drops smaller than 1 mm in diameter will attain 95% of their terminal velocity within 2 m. But above this size the distance to get to terminal velocity increases sharply. An example is a drop with a diameter of 2 mm that may achieve this at 5.6 m.

Optics

Due to the different refractive index of water and air, refraction and reflection occur on the surfaces of raindrops, leading to rainbow formation.

Sound

The major source of sound when a droplet hits a liquid surface is the resonance of excited bubbles trapped underwater. These oscillating bubbles are responsible for most liquid sounds, such as running water or splashes, as they actually consist of many drop-liquid collisions.{{cite journal | author-link = Andrea Prosperetti

"Dripping tap" noise prevention

Reducing the surface tension of a body of liquid makes possible to reduce or prevent noise due to droplets falling into it. This would involve adding soap, detergent or a similar substance to water. The reduced surface tension reduces the noise from dripping.

Shape

The classic shape associated with a drop (with a pointy end in its upper side) comes from the observation of a droplet clinging to a surface. The shape of a drop falling through a gas is actually more or less spherical for drops less than 2 mm in diameter.{{cite journal

Capillary length

The capillary length is a length scaling factor that relates gravity, density, and surface tension, and is directly responsible for the shape a droplet for a specific fluid will take. The capillary length stems from the Laplace pressure, using the radius of the droplet.

Using the capillary length we can define microdrops and macrodrops. Microdrops are droplets with radius smaller than the capillary length, where the shape of the droplet is governed by surface tension and they form a more or less spherical cap shape. If a droplet has a radius larger than the capillary length, they are known as macrodrops and the gravitational forces will dominate. Macrodrops will be 'flattened' by gravity and the height of the droplet will be reduced.

Size

Raindrop sizes typically range from 0.5 mm to 4 mm, with size distributions quickly decreasing past diameters larger than 2–2.5 mm.{{Cite book

Scientists traditionally thought that the variation in the size of raindrops was due to collisions on the way down to the ground. In 2009, French researchers succeeded in showing that the distribution of sizes is due to the drops' interaction with air, which deforms larger drops and causes them to fragment into smaller drops, effectively limiting the largest raindrops to about 6 mm diameter.

• However, drops up to 10 mm (equivalent in volume to a sphere of radius 4.5 mm) are theoretically stable and could be levitated in a wind tunnel. The largest recorded raindrop was 8.8 mm in diameter, located at the base of a cumulus congestus cloud in the vicinity of Kwajalein Atoll in July 1999. A raindrop of identical size was detected over northern Brazil in September 1995.{{cite journal

Standardized droplet sizes in medicine

In medicine, this property is used to create droppers and IV infusion sets which have a standardized diameter, in such a way that 1 millilitre is equivalent to 20 drops. When smaller amounts are necessary (such as paediatrics), microdroppers or paediatric infusion sets are used, in which 1 millilitre = 60 microdrops.

Gallery

Image:Blue Droplet.jpg|Blue dye being dropped in a saucer of milk Image:2006-02-13 Drop-impact.jpg|Impact of a drop of water Image:2006-01-28 drop-impact backjet.jpg|Backjet from drop impact File:Rain drops - Japan -2016 July 20.webm|Rain droplets impacting and dripping down File:Milk Drop Coronet, 1957.jpg|Edgerton's ultra-high-speed photograph of the splash of a drop of milk forming a small crown Image:Post-splash with droplets.jpg|A drop of water hitting a wet metal surface and ejecting more droplets, which become water globules and skim across the surface of the water Image:Water drop on a leaf.jpg|A drop of water on a leaf, hydrophobic effect, partial wetting Image:Water droplet backjet.JPG|A triple backjet after impact Image:Raindrop on a fern frond.jpg|Photo of a raindrop on a fern frond Image:2006-01-21 Detaching drop.jpg|Detaching drop Image:Showerheadandwaterdroplets.jpg|Water droplets forming out of a shower head Image:Asteraceae03.JPG|A drop of water on an Asteraceae Image:A small flower refracted in rain droplets.jpg|Droplets of water refracting a small flower Image:Water Drop on rose leaf.JPG|A raindrop on a leaf Image:Water_Droplets_Background.JPG|Water droplets on glass Image:Fountain water droplets.jpg|Fountain water droplets as seen in very short exposure Image:Water drops on rose leaf.jpg|Rain droplets on rose plant leaf File:RainDrops1.jpg|Rain water flux from a canopy. Among the forces that govern drop formation: surface tension, cohesion, Van der Waals force, Plateau–Rayleigh instability.

References

References

1. Luck, Steve. (1998). "The American Desk Encyclopedia". [[Oxford University Press]], USA.
2. (2005-10-04). "Numerical model for the fall speed of raindrops in a waterfall simulator".
3. Rankin, Ryan C.. (June 2005). "Bubble Resonance".
4. Thompson, Rachel. (25 June 2018). "Scientists have finally come up with a solution for the world's most annoying household sound".
5. "Water Drop Shape".
6. Berthier, Jean. (2010). "Microfluidics for biotechnology". Artech House.
7. "Millilitre".