Investigate, assess and model the experimental evidence supporting the existence and properties of the electron

  • Cathode Rays: Streams of electrons emitted within an evacuated tube from a cathode to an anode.
  • Cathode Ray Tube: Also known as a discharge tube, a highly evacuated sealed-glass tube with two electrodes contained within it, through which cathode rays can travel.
  • Cathode rays were discovered in 1855 by German physicists Heinrich Geissler and Julius Plucker.
  • In 1875, William Crookes designed a number of different discharge tubes to study cathode rays.
  • There were two main groups of scientists who supported two different theories about cathode rays:
    • German physicists, such as Hertz and Lenard, who advocated an electromagnetic wave model.
    • English physicists, such as Crookes and Thomson, who advocated a charged particle model
  • In 1897, J. J. Thomson demonstrated that cathode rays were actually deflected by electric fields, which led to the acceptance of the charged particle model.

Thomson’s charge-to-mass experiment  

  • To find the charge/mass ratio of cathode rays (now known as electrons), J. J. Thomson performed two main steps:
    • Varying perpendicular magnetic and electric fields acting on a beam of cathode rays until the beam was not deflected, and then equating electric and magnetic force equations, determining the velocity of the cathode rays.
    • Applying the same strength magnetic field alone and determining the radius of the circle path travelled by the particles.
  • More specifically:
    • He directed a beam of cathode rays through perpendicular electric and magnetic fields.
    • He adjusted the strength of the electric field until the beam passed through the perpendicular fields without being deflected.
    • For this to occur, the forces exerted by the two field would be equal, which allowed the formation of a mathematical expression:
      • Fb = FE
      • qvB = qE
      • Hence , veb
    • Thus, the velocity of the cathode rays could be determined.
    • Then, the beam was passed through the same magnetic field alone and the radius of the curvature of the beam was measured.
    • Because the magnetic field exerts a centripetal force:
      • FC = FB
      • magnetic field
      • Hence, charge mass ratio
    • Thus, the charge/mass ratio could be determined.
  • Thomson confirmed the value found by passing the beam through the same electric field alone and measuring the radius of the curvature of the beam.
  • Thomson determined the charge/mass ratio to be 1.759 x 1011 C kg-1
  • As electrons produced by different cathodes had identical properties, Thomson concluded that electrons were a subatomic building block of all atoms.

Millikan’s oil drop experiment (ACSPH026)

  • In 1909 , Robert Millikan studied fine drops of oil within a uniform electric field to understand charge of a particle.
  • His setup is shown as above.
  • When the oil drops were sprayed , some of them drifted down to the region of uniform electric field.
  • As the oil drops entered the electric field, they were also momentarily exposed to X-rays so that the oil drops would get charged.
  • Once charged the electric field would act on the oil drops.
  • Two forces would be acting on the charged oil drop in this region:
    • Gravitational force :gravitational force
    • Electric Force :electric force
  • The electric field could be adjusted such that , and the oil drops move with constant velocity or are stationary.
    • this implies :
      • electric field adjustment
    • This motion of oil drop could be observed and verified with the help of a microscope.
  • To measure the mass of the oil drop, Millikan did the following:
    • allowed the oil drop to fall without electric field.
    • measured the terminal velocity
    • using equations of fluid mechanics, calculated radius and hence volume of the oil drop.
    • Using an oil of known density, and measured volume, calculated the mass of the drop.

Millikan observed that the charge appeared in quantised values. It was in multiple of a particular value.

He found the value to be 1.6 x 10-19 C, now understood as the charge of the electron.

He received a Nobel prize for this discovery in 1923.

Extract from Physics Stage 6 Syllabus © 2017 NSW Education Standards Authority (NESA)