Chemists -- France -- Biography; Curie, Pierre, 1859-1906; Physicists -- France -- Biography
In recalling this period in the life of Pierre Curie, between 1883 and
1895, we can appreciate the great progress the young physicist had made
while acting as Chief of Laboratory. He had succeeded during this time
in organizing an entirely new teaching service; he had published an
important series of theoretical memoirs, as well as the results of
experimental research of the first order. In addition, he had
constructed new apparatus of great perfection--and all this in spite of
very insufficient accommodations and resources. This achievement
suggests the distance he had traveled since the doubts and hesitations
of his early youth in learning to discipline his methods of work, and to
derive from them the full advantage of his exceptional capacities.
He enjoyed a growing esteem in France, and in foreign countries. He was
listened to with interest at the meetings of the learned societies
(Society of Physics, Society of Mineralogy, Society of Electricians),
where he was in the habit of presenting his communications and where he
joined readily in the discussion of various scientific questions.
Among foreign scholars who already at this time appreciated him highly,
I can name, in the first place, the illustrious English physicist, Lord
Kelvin, who joined with him in a certain scientific discussion, and who
often expressed for him, from that time on, both esteem and sympathy.
During one of his visits to Paris, Lord Kelvin was present at a meeting
of the Society of Physics when Pierre Curie made a statement regarding
the construction and the use of standard condensers with guard ring. In
this statement he recommended the use of an apparatus which involved the
charging of the central part of the guard ring plate by a galvanic cell
and in uniting the guard ring with the earth. One uses then, as a
measure, the charge induced on the second plate. Even though the
resulting disposition of lines of the field be complex, the charge
induced can be calculated by a theorem of electrostatics, with the same
simple formula as is used for an ordinary apparatus in a uniform field,
and one has the benefit of a better isolation. Lord Kelvin believed at
first that this reasoning was inexact. Despite his great repute and his
advanced age, he went the following day to the laboratory to find the
young Director. Here he discussed the matter with him before the
blackboard. He was completely convinced, and seemed even delighted to
concede the point to his companion.[5]
Public-domain text, read in full here on John Shaqi.
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