Great has been the fame of the lodestone and of amber in the
writings of the learned: many philosophers cite the lodestone and also amber
whenever, in explaining mysteries and things beyond man’s understanding by
means of the lodestone as a sort of Delphic sword and as an illustration of all
sorts of things. Medical men also (at the bidding of Galen), in proving that purgative medicines exercise attraction
through likeness of substance and kinship of juices (a silly error and
gratuitous!), bring in as a witness the lodestone, a substance of great
authority and of noteworthy efficiency, and a body of no common order. Thus in
very many affairs persons who plead for a cause the merits of which they cannot
set forth, bring in as masked advocates the lodestone and the amber. But all
these, besides sharing the general misapprehension, are ignorant that the
causes of the lodestone’s movements are very different from those which give to
amber its properties; hence they easily fall into errors, and by their own imaginings
are led farther and farther astray. For in other bodies is seen a considerable
power of attraction, differing from that of the lodestone, in amber, for
example. Of this substance a few words must be said, to show the nature of the
attachment of bodies to it, and to point out the vast difference between this
and the magnetic actions; for people still continue in ignorance, and deem that
inclination of bodies to amber to be an attraction, and comparable to the
magnetic coition.
There are no lines of force!
— William Gilbert (1540-1603), De Magnete
[All About Magnets], 1600
One loadstone appears to attract another in the natural
position; but in the opposite position, repels it and brings it to rights.
— William Gilbert (1540-1603), De Magnete
[All About Magnets], 1600.
But when I tried all these things, I found them to be false:
for not onely breathing and belching upon the Loadstone after eating of
Garlick, did not stop its vertues: but when it was all anoynted over with the
juice of the Garlick, it did perform its office as well as if it had never been
touched with it.
— William Gilbert (1540-1603), De Magnete [All About Magnets], 1600
Take the stone on which you have designated the poles, N and
S, and put it in its vessel so that it may float …
— William Gilbert (1540-1603), De Magnete
[All About Magnets], 1600
Lines of force can cross space, like gravity and
electricity. So space has a magnetic relation of its own, and one that we
should probably find hereafter to be of the utmost importance in natural
phenomena.
— Michael Faraday (1791 – 1867), lecture to the Royal Society, about 1850,
For the complete determination of the magnetic force of the
earth in a given place three elements are required: the declination, or the
angle between the plane in which the magnet lies and a meridian; the
inclination of its direction to the horizontal plane; and in the third place,
the intensity…
The method which was used in this investigation consists in
the observation of the time in which the same magnetic needle makes the same
number of oscillations in different places, or of the number of oscillations
made in the same interval of time. The intensity is set proportional to the
square of the number of oscillations in a given time.
— Johann Karl Friedrich Gauss (1777 – 1855), writing in 1841.
At the centre of the card is a metal thimble holding a jewel
with a conical hole, which rests on the supporting pivot. A jewel such as a
small ruby is used for pivots in the compass, in the best watches, and in the
best pivoted electrical instruments, because it is very hard and does not wear
out. Underneath the card is fixed not one magnet, but eight, held by an
arrangement of threads which makes the north point of the card point to the
magnetic north.
— E. N. da C. Andrade and Julian Huxley, Forces
at Work, Blackwell, 1934.
In January 1981 … we undertook an expedition to New Zealand
and Tasmania to search for magnetotactic bacteria and to test the hypothesis.
The sites were chosen because they are ecologically diverse and share many
physical characteristics with New England, such as absolute latitude, magnetic
field strength and climate. Moreover, the magnetic inclination in New Zealand
and Tasmania has the same absolute value as it has in New England, although it
has the opposite sign.
— Richard Blakemore and Richard B. Frankel, ‘Magnetic navigation in bacteria’, Scientific American December 1981.
[They] had been set together, side by side, to work on the
problem of deducing the characteristics of German magnetic mines laid at sea,
especially the sensitivity and polarity of the firing mechanism. The data from
which the characteristics were to be deduced were the reports of our
minesweepers as they exploded the mines, with the positions of the explosions
being reported as ranges and bearings from the minesweepers.
— R. V. Jones, Most Secret War,
Hamish Hamilton, 1978.
Field reversals, occurring roughly every million years, are
the most dramatic of the wide range of phenomena exhibited by the earth’s
magnetic field. And the next reversal on Earth may not be so far away: if the
current rate of decay of the Earth’s dipole component is maintained, it will
vanish in less than 2000 years’ time.
— Jeremy Bloxham, ‘Evidence for asymmetry and fluctuation’, Nature, 322: 13, 1986
I am the Knower of the field in everyone, Arjuna. Knowledge
of the field and its Knower is true knowledge.
— Bhagavad Gita, 13:2, in the
translation of Eknath Easwaran, Arkana Books, 1985.
We know that the magnet loves the lodestone, but we do not
know whether the lodestone also loves the magnet or is attracted to it against
its will.
— Unknown Arabic physicist, 12th century.
If the experiments are completed within a short time, and if
the needle which is used is made of hardened steel and carefully magnetised, no
considerable loss of its power need be feared …
— Karl Friedrich Gauss (1777 – 1855), writing in 1841.
In treating of magnetism, a distinction is made between permanent and variable magnets; we regard, for example, a magnet of hard steel as
a permanent magnet, and a magnet of soft iron as a variable one. Were the
distinction between the two classes perfect (which is, however, as little the
case as that between conductors and insulators in electricity), the magnetism
of a permanent magnet could only investigated through its effects, while that of the variable magnet might be investigated
through its causes as well as its effects. At all events, even though the
distinction is not perfect, the variable magnet is more favourable to a
complete examination of the nature of magnetism than the permanent one …
Now it is known that the investigation of the magnetism of a
magnet through its effects (produced
on other bodies) leads us to the knowledge of the ideal distribution of the magnetic fluid on the surface of a
magnet, regarding which Gauss has proved, that as far as the explanation of
phenomena is concerned, it answers completely to the true internal condition of the magnet. In many investigations it is
a great advantage to find a way furnished by the ideal distribution towards the
simple and complete union of all the observed actions, without the necessity of
making any hypothesis regarding the interior of the body; more particularly
when the causes of these actions remain unknown and are still to be
investigated.
— Wilhelm Eduard Weber (1804 – 1891) Poggendorff’s Annalen, lxxxvii, translated in the Scientific memoirs, edited by Tyndall and Francis, 1853.
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