Echallens, just taken from Savoy, but in 1798 Morat was incorporated with (finally annexed in 1814) the canton of Fribourg, the other bailiwicks being then given to the canton of Léman (later of Vaud). In the 16th century the original democratic government gradually gave place to the oligarchy of the patrician families. Though this government caused much discontent it continued till it was overthrown on the French occupation of 1798.
From 1803 (Act of Mediation) to 1814, Fribourg was one of the six cantons of the Swiss Confederation. But, on the fall of the new régime, in 1814, the old patrician rule was partly restored, as 108 of the 144 seats in the cantonal legislature were assigned to members of the patrician families. In 1831 the Radicals gained the power and secured the adoption of a more liberal constitution. In 1846 Fribourg (where the Conservatives had regained power in 1837) joined the Sonderbund and, in 1847, saw the Federal troops before its walls, and had to surrender to them. The Radicals now came back to power, and again revised the cantonal constitution in a liberal sense. The Catholic and Conservative party made several attempts to recover their supremacy, but their chiefs were driven into exile. In 1856 the Conservatives regained the upper hand at the general cantonal election, secured the adoption in 1857 of a new cantonal constitution, and have ever since maintained their rule, which some dub “clerical,” while others describe it as “anti-radical.”
Authorities.—Archives de la Société d’histoire du Canton de F., from 1850; F. Buomberger, Bevölkerungs- u. Vermögensstatistik in d. Stadt u. Landschaft F. um die Mitte d. 15ten Jahrhunderts (Bern, 1900); A. Daguet, Histoire de la ville et de la seigneurie de F., to 1481 (Fribourg, 1889); A. Dellion, Dictionnaire historique et statistique des paroisses catholiques du C. de F. (12 vols., Fribourg, 1884–1903); Freiburger Geschichtsblätter, from 1894; Fribourg artistique (fine plates), from 1890; E. Heyck, Geschichte der Herzoge von Zähringen (Freiburg i. Br., 1891); F. Kuenlin, Der K. Freiburg (St Gall and Bern, 1834); Mémorial de F. (6 vols., 1854–1859); Recueil diplomatique du Cant. de F. (original documents) (8 vols., Fribourg, 1839–1877); F. E. Welti, Beiträge zur Geschichte des älteren Stadtrechtes von Freiburg im Uechtland (Bern, 1908); J. Zemp, L’Art de la ville de Fribourg au moyen âge (Fribourg, 1905); J. Zimmerli, Die deutsch-französische Sprachgrenze in d. Schweiz (Basel and Geneva, 1895), vol. ii., pp. 72 seq.; Les Alpes fribourgeoises (Lausanne, 1908). (W. A. B. C.)
FRICTION (from Lat. fricare, to rub), in physical and mechanical
science, the term given to the resistance which every material
surface presents to the sliding of any other such surface upon it.
This resistance is due to the roughness of the surfaces; the
minute projections upon each enter more or less into the minute
depressions on the other, and when motion occurs these roughnesses
must either be worn off, or continually lifted out of the
hollows into which they have fallen, or both, the resistance to
motion being in either case quite perceptible and measurable.
Friction is preferably spoken of as “resistance” rather than “force,” for a reason exactly the same as that which induces us to treat stress rather as molecular resistance (to change of form) than as force, and which may be stated thus: although friction can be utilized as a moving force at will, and is continually so used, yet it cannot be a primary moving force; it can transmit or modify motion already existing, but cannot in the first instance cause it. For this some external force, not friction, is required. The analogy with stress appears complete; the motion of the “driving link” of a machine is communicated to all the other parts, modified or unchanged as the case may be, by the stresses in those parts; but the actual setting in motion of the driving link itself cannot come about by stress, but must have for its production force obtained directly from the expenditure of some form of energy. It is important, however, that the use of the term “resistance” should not be allowed to mislead. Friction resists the motion of one surface upon another, but it may and frequently does confer the motion of the one upon the other, and in this way causes, instead of resists, the motion of the latter. This may be made more clear, perhaps, by an illustration. Suppose we have a leather strap A passing over a fixed cylindrical drum B, and let a pulling force or effort be applied to the strap. The force applied to A can act on B only at the surfaces of contact between them. There it becomes an effort tending either to move A upon B, or to move the body B itself, according to the frictional conditions. In the absence of friction it would simply cause A to slide on B, so that we may call it an effort tending to make A slide on B. The friction is the resistance offered by the surface of B to any such motion. But the value of this resistance is not in any way a function of the effort itself,—it depends chiefly upon the pressure normal to the surfaces and the nature of the surfaces. It may therefore be either less or greater than the effort. If less, A slides over B, the rate of motion being determined by the excess of the effort over the resistance (friction). But if the latter be greater no sliding can occur, i.e. A cannot, under the action of the supposed force, move upon B. The effort between the surfaces exists, however, exactly as before,—and it must now tend to cause the motion of B. But the body B is fixed,—or, in other words, we suppose its resistance to motion greater than any effort which can tend to move it,—hence no motion takes place. It must be specially noticed, however, that it is not the friction between A and B that has prevented motion, this only prevented A moving on B,—it is the force which keeps B stationary, whatever that may be, which has finally prevented any motion taking place. This can be easily seen. Suppose B not to be fixed, but to be capable of moving against some third body C (which might, e.g., contain cylindrical bearings, if B were a drum with its shaft), itself fixed,—and further, suppose the frictional resistance between B and C to be the only resistance to B’s motion. Then if this be less than the effort of A upon B, as it of course may be, this effort will cause the motion of B. Thus friction causes motion, for had there been no frictional resistance between the surfaces of A and of B, the latter body would have remained stationary, and A only would have moved. In the case supposed, therefore, the friction between A and B is a necessary condition of B receiving any motion from the external force applied to A.
Without entering here on the mathematical treatment of the subject of friction, some general conclusions may be pointed out which have been arrived at as the results of experiment. The “laws” first enunciated by C. A. Coulomb (1781), and afterwards confirmed by A. J. Morin (1830–1834), have been found to hold good within very wide limits. These are: (1) that the friction is proportional to the normal pressure between the surfaces of contact, and therefore independent of the area of those surfaces, and (2) that it is independent of the velocity with which the surfaces slide one on the other. For many practical purposes these statements are sufficiently accurate, and they do in fact sensibly represent the results of experiment for the pressures and at the velocities most commonly occurring. Assuming the correctness of these, friction is generally measured in terms simply of the total pressure between the surfaces, by multiplying it by a “coefficient of friction” depending on the material of the surfaces and their state as to smoothness and lubrication. But beyond certain limits the “laws” stated are certainly incorrect, and are to be regarded as mere practical rules, of extensive application certainly, but without any pretension to be looked at as really general laws. Both at very high and very low pressures the coefficient of friction is affected by the intensity of pressure, and, just as with velocity, it can only be regarded as independent of the intensity and proportional simply to the total load within more or less definite limits.
Coulomb pointed out long ago that the resistance of a body to be set in motion was in many cases much greater than the resistance which it offered to continued motion; and since his time writers have always distinguished the “friction of rest,” or static friction, from the “friction of motion,” or kinetic friction. He showed also that the value of the former depended often both upon the intensity of the pressure and upon the length of time during which contact had lasted, both of which facts quite agree with what we should expect from our knowledge of the physical nature, already mentioned, of the causes of friction. It seems not unreasonable to expect that the influence of time upon friction should show itself in a comparison of very slow with very rapid motion, as well as in a comparison of starting (i.e. motion after a long time of rest) with continued
