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"Droplet" and "raindrop" redirect here. For other uses, see and.

Water drops falling from a tap.
Surface tension prevents the droplet from being cut by a knife

A drop or droplet is a small column of, bounded completely or almost completely by. A drop van damme dating history may form when liquid accumulates at the lower end of van damme dating history a tube or other surface boundary, producing a hanging drop called a drop. Drops may also be formed by the of van damme dating history a or by of a larger mass of liquid.

One drop equals 50 mm^3, then 1 cubic centimetre = 20 drops


Surface tension[]

Drop of water dancing on a water surface subject to vibrations
The pendant drop test illustrated.

Liquid forms drops because the liquid exhibits.

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.

Pendant drop test[]

In the pendant drop test, a drop of liquid is suspended from the end of a tube by. 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 γ {\displaystyle \gamma } . Since the length of this boundary is the circumference of the tube, the force due to surface tension is given by

F γ = π d γ {\displaystyle \,F_{\gamma }=\pi d\gamma } single tanzkurse baden bei wien

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

m g = π d γ sin ⁡ α {\displaystyle \,mg=\pi d\gamma \sin \alpha }

where α is the with the tube, 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, γ {\displaystyle \gamma } .

m g = π d γ {\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.

In, and IV infusion sets have a, in such a way that 1 is equivalent to 20. And, for the cases when smaller amounts are necessary (such as paediatrics), microdroppers or paediatric infusion sets are used, in which 1 millilitre = 60 microdrops.

Drop adhesion to a solid[]

The drop to a solid can be divided to two categories: lateral adhesion and normal adhesion. Lateral adhesion resembles friction (though 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 (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 ).


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, droplets are usually described by their perceived size (i.e., diameter) whereas the dose (or number of infective particles in the case of ) is a function of their volume. This increases by relative to diameter; thus a 50 µm droplet represents a dose in 65 pl and a 500 µm drop represents a dose in 65 nanolitres.

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.

Due to the different of and, and occur on the surfaces of, leading to formation.

The major source of sound when a droplet hits a liquid surface is the 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.

The shapes of raindrops, depending on their sizes.

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 2mm in diameter. Larger drops tend to be flatter on the bottom part due to the pressure of the gas they move through. As a result, as drops get larger, a concave depression forms which leads to the eventual breakup of the drop.

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

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 in the vicinity of in July 1999. A raindrop of identical size was detected over northern Brazil in September 1995.


See also[]


  1. Luck, Steve (1998-10-22).. Oxford University Press, USA.  . 
  2. Cutnell, John D.; Kenneth W. Johnson (2006). Essentials of Physics. Wiley Publishing. 
  3. Roger P. Woodward, Ph.D. (PDF). First Ten Angstroms. Retrieved 2008-11-05. 
  4. F.K.Hansen; G. Rodsrun (1991). "Surface tension by pendant drop. A fast standard instrument using computer image analysis". Colloid and Interface Science. 141: 1–12. :. :. 
  5. ^ (PDF). 2005-10-04. p. 2. Archived from (PDF) on 2013-07-31. Retrieved 2013-06-28. 
  6. ; Oguz, Hasan N. (1993). (PDF). Annual Review of Fluid Mechanics. 25: 577–602. :. :. Retrieved 2006-12-09. 
  7. Rankin, Ryan C. (June 2005).. The Physics of Bubbles, Antibubbles, and all That. Retrieved 2006-12-09. 
  8. ^ Pruppacher, H. R.; Pitter, R. L. (1971). "A Semi-Empirical Determination of the Shape of Cloud and Rain Drops". Journal of the Atmospheric Sciences. 28: 86–94. :. :. 
  9. . Retrieved 2008-03-08. 
  10. McFarquhar, Greg (2010). "Raindrop Size Distribution and Evolution". Geophysical Monograph Series. 191. :. :. 
  11. Emmanuel Villermaux, Benjamin Bossa (September 2009). (PDF). Nature Physics. 5 (9): 697–702. :. :.. 
  12. Hobbs, Peter V.; Rangno, Arthur L. (July 2004). "Super-large raindrops". Geophysical Research Letters. 31. :. :. 

External links[]

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