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The purpose of Robert Millikan's oil-drop experiment (1909) was to measure the electric charge of the electron. He did this by carefully balancing the gravitational and electric forces on tiny charged droplets of oil suspended between two metal electrodes. Knowing the electric field, the charge on the droplet could be determined. Repeating the experiment for many droplets, he found that the values measured were always multiples of the same number. He interpreted this as the charge on a single electron: 1.602 × 10−19 coulombs (SI unit for electric charge). In 1923, Millikan won the Nobel Prize for physics in part because of this experiment. This experiment has since been repeated by generations of physics students, although it is rather expensive and difficult to do properly.
Experimental procedure The apparatus The diagram shows a simplified version of Millikan's set up. A uniform electric field is provided by a pair of horizontal parallel plates with a high potential difference between them. A charged drop of oil is allowed to drift in between them. By varying the potential, the drop can be made to rise, or fall acordingly. The plates are held together by a ring of insulating material (not shown in the diagram). There are two holes cut into the ring. A bright light source is shone through one of the holes, and focused on the region where the oil drops drift between the plates. A low-powered microscope is inserted through the other hole. The oil drops reflect the light and look like bright points on a dark field of view through the microscope. The microscope has a graduated scale in the eyepiece which allows for the velocity of the drop to be measured by timing how long it takes to travel from one division to another. The oil used is the type that is usually used in vacuum apparatus. This is because this type of oil has an extremely low vapour pressure. Ordinary oil would evaporate away under the heat of the light source and so the mass of the oil drop would not remain constant over the course of the experiment. Some oil drops will pick up a charge through friction with the nozzle as they are sprayed, but more can be charged by allowing an ionising radiation source (such as an x ray tube) Method Initially the oil drops are allowed to fall between the plates with the electric field turned off. They very quickly reach a terminal velocity because of friction with the air in the chamber. The field then turned on and, if it is large enough, some of the drops (the charged ones) will start to rise. (This is because the upwards electric force FE is greater for them than the downwards gravitational force W). A likely looking drop is selected and kept in the middle of the field of view by alternately switching off the voltage until all the other drops have fallen. The experiment is then continued with this one drop. The drop is allowed to fall and its terminal velocity v1 in the absence of an electric field is calculated. The drag force acting on the drop can then be worked out using Stokes' law: where v1 is the terminal velocity (i.e. velocity in the absence of an electric field) of the falling drop, η is the viscosity of the air, and r is the radius of the drop. The weight W is the volume V multiplied by the density ρ and the acceleration due to gravity g. However what is needed is the apparent weight. The apparent weight in air is the true weight minus the upthrust (which equals the weight of air displaced by the oil drop). For a perfectly spherical droplet the apparent weight can be written as: ho - ho_) , Now at terminal velocity the oil drop is not accelerating. So the total force acting on it must be zero. So the two forces F and W must cancel one another out. implies: Once r is calculated, W can easily be worked out. Now the field is turned back on. where q is the charge on the oil drop and E is the electric field between the plates. For parallel plates where V is the potential difference and d is the distance between the plates. One conceivable way to work out q would be to adjust V until the oil drop remained steady. Then we could equate FE with W. But in practice this is extremely difficult to do precisely. A more practical approach is to turn V up slightly so that the oil drop rises with a new terminal velocity v2. Then Millikans experiment and cargo cult science Richard Feynman said in a commencement lecture he gave at Caltech in 1974
However, according to this webpage the value as of 1991 for the charge on the electron is less than 1% higher than the value obtained by Millikan in 1913. | ||||||||
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