Initial Phase
Pierre began his voyage of scientific
researches at the age of 19. He carried out his first work on the calculation of the
wavelength of heat waves. At the beginning of his career, he worked as a laboratory
assistant to Professor P. Desains in the faculty of science. In 1880, he conducted his
first research in the determination of the wavelengths of infrared rays, using a novel
system of a thermocouple and a metallic wire grating. This process was entirely new at
that time, and it has since often been used in the study of this subject.
Following the work on wavelength rays, he
undertook an investigation on crystals in collaboration with his brother Jacques, who was
a preparator for Friedels laboratory of mineralogy at the Sorbonne. Their fruitful
collaboration led the two young physicists towards a great success, the discovery of
piezo-electricity. This unknown phenomenon consisted of an electric polarization produced
by the compression or the expansion of crystals in the direction of axis of symmetry. The
Curie brothers succeeded in carrying out a complete study of the new phenomenon :
"Some crystals, when compressed in
particular directions show positive and negative charges on their surfaces, the charges
being proportional to the pressure and disappearing when the pressure is withdrawn."
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After his theoretical and experimental researches, he verified Lippmanns prediction of a converse effect : the production of a piezo-electric crystal by an electric field. Applying this phenomenon, he formed a new apparatus, a piezo-electric quartz electrometer. This apparatus measures in absolute terms small quantities of electricity and also electric currents of low intensity. In experiments of radioactivity, Pierres discovery rendered great help. |
While experimenting piezo-electricity,
Pierre and Jacques were obliged to employ electrometric apparatus. In those days, the
quadrant electrometer was very well known, but they could not use it. So they developed a
new version, better adapted to their requirements. This instrument become popular in
France as the Curie electrometer the forerunner of modern quartz controls for
timepieces and radio transmitters.
Second Phase
In 1882, working as a supervisor at the
school of physics in Paris, Pierre carried out his own research. For a long period, he
studied buffered movements. These first years of independent research were arduous. It was
the second phase of his career, when he conducted fruitful research on crystals and
magnetism. He advanced theories of symmetry with regard to certain physical phenomena and
turned his attention to magnetism.
In 1885, he published his research papers
on the theoretical relations between crystallography and physics. Pierre, with his
brother, established the conditions of symmetry required for its production in crystals
and stated its notably simple quantitative laws as well as its absolute magnitude for
particular crystals. Pierre formulated the principle of symmetry, which states the
impossibility of bringing about a specific physical process in an environment lacking a
certain minimal dis-symmetry characteristic of the process. This principle became one of
the ultra-sensitive scientific scale, the Curie scale. Many eminent foreign scientists
including Roentgen, Kundt, Voigt and Riecke followed the new road opened by the Curie
brothers and made further investigations.
In 1894, he obtained his doctorate with a
thesis on the magnetic properties of materials. He undertook research on magnetism and
obtained a result of capital importance. He managed to perfect the analytical balance by
creating a periodic balance with direct reading of the last weights. Then he concentrated
on magnetism. He explained if there was any existence of some relation between the three
types of magnetism : Ferromagnetism, paramagnetism and diamagnetism. It led to the
discovery of a fundamental law, known as the Curies Law.
This law states : "The properties of
diamagnetic materials are generally independent of temperature but for paramagnetic
material the susceptibility is inversely proportional to the absolute temperature."
The temperature at which the transition
from ferromagnetism to paramagnetism takes place is known today as Curie point. Pierre
demonstrated the totally different character of diamagnetism and paramagnetism, which was
later explained theoretically by Paul Langevin. |