Drop (liquid)

Drop of water bouncing on a water surface subject to vibrations

The pendant drop test illustrated

Liquid forms drops because it exhibits surface tension.[1]

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.

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 ${\displaystyle \gamma }$.[2] Since the length of this boundary is the circumference of the tube, the force due to surface tension is given by

${\displaystyle \,F_{\gamma }=\pi d\gamma }$

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 (${\displaystyle F_{g}=mg}$) with the component of the surface tension in the vertical direction (${\displaystyle F_{\gamma }\sin \alpha }$) giving the formula

${\displaystyle \,mg=\pi d\gamma \sin \alpha }$

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, ${\displaystyle \gamma }$.

${\displaystyle \,mg=\pi d\gamma }$

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.[3][4]

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).

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 diameter; thus a 50 μm droplet represents a dose in 65 pl and a 500 μm drop represents a dose in 65 nanometers.

A droplet with a diameter of 3mm has a terminal velocity of approximately 8 m/s.[5] 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.[5]

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

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.[6][7]

Raindrops are not tear-shaped (Ⓐ); very small raindrops are almost spherical in shape (Ⓑ), while larger raindrops are flattened at the bottom (Ⓒ). As raindrops increase in size they encounter progressively more air resistance as they fall, making them begin to become unstable (Ⓓ); in the case of the largest raindrops, air resistance will be enough to split them into smaller raindrops (Ⓔ).

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.[9] Larger drops tend to be flatter on the bottom part due to the pressure of the gas they move through.[10] As a result, as drops get larger, a concave depression forms which leads to the eventual breakup of the drop.

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.[11]

The capillary length ${\displaystyle L_{c}}$ against radii of a droplet

Raindrop sizes typically range from 0.5 mm to 4 mm, with size distributions quickly decreasing past diameters larger than 2-2.5 mm.[12]

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.[13] 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.[9] 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.[14]

• 
  Blue dye being dropped in a saucer of milk
• 
  Impact of a drop of water
• 
  Backjet from drop impact
• Rain droplets impacting and dripping down
• 
  A drop of water hitting a metal surface and crown formation due to splashing of droplet
• 
  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
• 
  A drop of water on a leaf, hydrophobic effect, partial wetting
• 
  A triple backjet after impact
• 
  Photo of a raindrop on a fern frond
• 
  Detaching drop
• 
  Water droplets forming out of a shower head
• 
  A drop of water on an Asteraceae
• 
  Droplets of water refracting a small flower
• 
  A raindrop on a leaf
• 
  Water droplets on glass
• 
  Fountain water droplets as seen in very short exposure
• 
  Rain droplets on rose plant leaf

• Pitch drop experiment
• Rain
• Splash (fluid dynamics)
• Water droplet erosion
• Dribbling (teapot)

Wikimedia Commons has media related to Drops.

• Liquid Sculpture – pictures of drops
• Liquid Art – Galleries of fine art droplet photography (archived 19 March 2008)
• (Greatly varying) calculation of water waste from dripping tap: , (Archived 2009-08-13 at the Wayback Machine)