- Outline milestones in the development of modern atomic theory including Thomson, Millikan, and Rutherford experiments
- Describe the three subatomic particles (protons, neutrons, electrons) and define isotopes
Core Concepts & Principles
Electrons and Cathode Rays
In the late 1800s, J. J. Thomson used a cathode ray tube to discover that high-voltage electrical discharges in low-pressure gases produce a visible beam. This beam is deflected by electric and magnetic fields, showing it consists of negatively charged particles—electrons—that are fundamental constituents of all atoms and far less massive than atoms. Thomson calculated their charge-to-mass ratio.
Elementary Charge and Mass of the Electron
In 1909, Robert Millikan measured the charge on microscopic oil droplets, discovering that charges are always multiples of (the elementary charge of a single electron). Combining this with Thomson's charge-to-mass ratio yielded the mass of the electron ().
Early Atomic Models
Thomson proposed the "plum pudding" model (negative electrons embedded in a positive sphere), while Hantaro Nagaoka proposed a Saturn-like model (positive sphere surrounded by an electron ring). Both preceded the modern nuclear view.
Rutherford Scattering and the Nucleus
Ernest Rutherford, Hans Geiger, and Ernest Marsden fired high-speed alpha particles ( particles)—positively charged particles consisting of two protons and two neutrons—at thin gold foil. While most passed straight through (revealing that atoms are mostly empty space), a tiny fraction deflected sharply, showing that atoms contain a tiny, massive, positively charged nucleus. Rutherford later identified the proton as the hydrogen nucleus.
Isotopes and Neutrons
Frederick Soddy discovered isotopes—atoms of the same element that differ in mass due to varying numbers of neutrons. James Chadwick discovered uncharged neutrons in 1932, explaining why isotopes have essentially the same chemical properties (the same electron arrangement in neutral atoms) yet differ in mass.
Atoms are not indivisible; they consist of an extremely dense, positively charged nucleus (protons and neutrons) surrounded by a vast region of space containing low-mass electrons.
Problem-Solving Routines & Methods
- 1Use the measured electron charge magnitude and charge-to-mass ratio.
- 2Divide charge by charge-to-mass ratio: m = e / (e/m).
- 3Cancel coulombs to leave kilograms.
Combines Millikan's elementary charge with Thomson's charge-to-mass ratio.