EE Academic Genealogy Project
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Gustav R. Kirchhoff
|Franz Ernst Neumann|
|Carl Friedrich Gauss|
Gustav Robert Kirchhoff (12 March 1824 – 17 October 1887) was a German physicist who contributed to the fundamental understanding of electrical circuits, spectroscopy, and the emission of black-body radiation by heated objects.
He coined the term “black body” radiation in 1862, and two different sets of concepts (one in circuit theory, and one in thermodynamics) are named “Kirchhoff’s laws” after him; there is also a Kirchhoff’s Law in thermochemistry. The Bunsen–Kirchhoff Award for spectroscopy is named after him and his colleague, Robert Bunsen.
Kirchhoff formulated his circuit laws, which are now ubiquitous in electrical engineering, in 1845, while still a student. He completed this study as a seminar exercise; it later became his doctoral dissertation. In 1857 he calculated that an electric signal in a resistanceless wire travels along the wire at the speed of light. He proposed his law of thermal radiation in 1859, and gave a proof in 1861. He was called to the University of Heidelberg in 1854, where he collaborated in spectroscopic work with Robert Bunsen. Together Kirchhoff and Bunsen discovered caesium and rubidium in 1861. At Heidelberg he ran a mathematico-physical seminar, modelled on Neumann’s, with the mathematician Leo Koenigsberger. Among those who attended this seminar were Arthur Schuster and Sofia Kovalevskaya. In 1875 Kirchhoff accepted the first chair specifically dedicated to theoretical physics at Berlin.
In 1862 he was awarded the Rumford Medal for his researches on the fixed lines of the solar spectrum, and on the inversion of the bright lines in the spectra of artificial light.
He contributed greatly to the field of spectroscopy by formalizing three laws that describe the spectral composition of light emitted by incandescent objects, building substantially on the discoveries of David Alter and Anders Jonas Angstrom (see also: spectrum analysis).
He also contributed to optics, carefully solving Maxwell’s equations to provide a solid foundation for Huygens’ principle (and correct it in the process).
William L. Robb
Prof. Physics and Electrical Engineering
|Post-Doctoral Fellow, 1892, ETH Zurich|
|Ph.D., 1883, University of Berlin||Hermann von Helmholtz|
|M.S., 1881, University of Berlin||Gustav R. Kirchhoff|
William Lispenard Robb, (1861-1933) received a B.A. degree from Columbia University. He continued his post-graduate studies in Germany under von Helmholtz and Kirchoff, and received his Ph.D. at the University of Berlin. He went to Rensselaer as a Professor of Physics and Electrical Engineering in 1902 by Director P. C. Ricketts, who was then embarking on a program of broadening the scope of the Institute curriculum. Dr. Robb introduced, organized, and heeded the course and department of electrical engineering until his death in 1933.
Dr. Robb was the first of that group of newcomers who helped to broaden and revitalize science and engineering at Rensselaer. His exacting and somewhat gruff manner and method as a teacher and administrator only partly concealed the essential integrity of the man, who represented the concept of “no nonsense” education.
[Information courtesy of Rensselaer Polytechnic Institute Archives. Special thanks to Ms. Jenifer Monger of RPI.]
Heinrich R. Hertz
|Hermann von Helmholtz|
|Gustav R. Kirchhoff|
Heinrich Rudolf Hertz (22 February 1857 – 1 January 1894) was a German physicist who clarified and expanded James Clerk Maxwell’s electromagnetic theory of light, which was first demonstrated by David Edward Hughes using non-rigorous trial and error procedures. Hertz is distinguished from Maxwell and Hughes because he was the first to conclusively prove the existence of electromagnetic waves by engineering instruments to transmit and receive radio pulses using experimental procedures that ruled out all other known wireless phenomena. The scientific unit of frequency – cycles per second – was named the “hertz” in his honor.
While studying at the Gelehrtenschule des Johanneums in Hamburg, Heinrich Rudolf Hertz showed an aptitude for sciences as well as languages, learning Arabic and Sanskrit. He studied sciences and engineering in the German cities of Dresden, Munich and Berlin, where he studied under Gustav R. Kirchhoff and Hermann von Helmholtz.
In 1880, Hertz obtained his PhD from the University of Berlin; and remained for post-doctoral study under Hermann von Helmholtz. In 1883, Hertz took a post as a lecturer in theoretical physics at the University of Kiel. In 1885, Hertz became a full professor at the University of Karlsruhe where he discovered electromagnetic waves.
The most dramatic prediction of Maxwell’s theory of electromagnetism, published in 1865, was the existence of electromagnetic waves moving at the speed of light, and the conclusion that light itself was just such a wave. This challenged experimentalists to generate and detect electromagnetic radiation using some form of electrical apparatus.
The first successful radio transmission was made by David Edward Hughes in 1879, but it would not be conclusively proven to have been electromagnetic waves until the experiments of Heinrich Hertz in 1886. For the Hertz radio wave transmitter, he used a high voltage induction coil, a condenser (capacitor, Leyden jar) and a spark gap—whose poles on either side are formed by spheres of 2 cm radius—to cause a spark discharge between the spark gap’s poles oscillating at a frequency determined by the values of the capacitor and the induction coil.
To prove there really was radiation emitted, it had to be detected. Hertz used a piece of copper wire, 1 mm thick, bent into a circle of a diameter of 7.5 cm, with a small brass sphere on one end, and the other end of the wire was pointed, with the point near the sphere. He bought a screw mechanism so that the point could be moved very close to the sphere in a controlled fashion. This “receiver” was designed so that current oscillating back and forth in the wire would have a natural period close to that of the “transmitter” described above. The presence of oscillating charge in the receiver would be signaled by sparks across the (tiny) gap between the point and the sphere (typically, this gap was hundredths of a millimeter).
In more advanced experiments, Hertz measured the velocity of electromagnetic radiation and found it to be the same as the light’s velocity. He also showed that the nature of radio waves’ reflection and refraction was the same as those of light and established beyond any doubt that light is a form of electromagnetic radiation obeying the Maxwell equations.
Hertz’s experiments triggered broad interest in radio research that eventually produced commercially successful wireless telegraph, audio radio, and later television.
He died of Wegener’s granulomatosis at the age of 36 in Bonn, Germany in 1894.
In 1930 the International Electrotechnical Commission (IEC) honored Hertz by naming the unit of frequency—one cycle per second—the “hertz”.