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  1 Int  |           art came together in his work on esthetics, and he had
  2 I    |           understand the forces at work in the world in which he
  3 I    |     regards the kind of scientific work. I then endeavoured to show
  4 I    |             what we call amount of work in the mechanical sense
  5 I    |           of the word.~The idea of work for machines, or natural
  6 I    |      concerned. In speaking of the work of machines and of natural
  7 I    |            of the hard and intense work of thinking, which tries
  8 I    |    intelligence is met with in the work of machines, of course is
  9 I    |      assigned to the instrument at work.~Now, the external work
 10 I    |            work.~Now, the external work of man is of the most varied
 11 I    |        used on it, and the kind of work produced. But both the arm
 12 I    |          is incapable of doing any work; the moving force of the
 13 I    |           of the muscle must be at work in it, and these must obey
 14 I    |            and weaving frames, the work of which rivals that of
 15 I    |           of the muscles.~Now, the work of the smith requires a
 16 I    |          we speak of the amount of work of a machine. We have nothing
 17 I    |           of becoming exhausted by work is also met with in the
 18 I    |            when their capacity for work is spent, there is a possibility
 19 I    |            understand by amount of work; but we must endeavour,
 20 I    |           to measure the amount of work. This we can do better by
 21 I    |      activity can be restored.~The work which the weight has to
 22 I    |             must be continually at work. Such a one is the weight.~
 23 I    |          measure for the amount of work. Let us assume that a clock
 24 I    |          others, ten times as much work is performed for ten pounds
 25 I    |           fall being the same, the work increases directly as the
 26 I    |         therefore do twice as much work as when it can only run
 27 I    |         weight being the same, the work increases as the height
 28 I    |            off all as a measure of work, at any rate, in the present
 29 I    |         for measuring magnitude or work is a foot pound - that is,
 30 I    |             that is, the amount of work which a pound raised through
 31 I    |          may apply this measure of work to all kinds of machines,
 32 I    |            had performed a certain work, Hence it is that the measurement
 33 I    |            that the measurement of work by foot pounds is universally
 34 I    |            that case be simpler to work the machine by the direct
 35 I    |          levels, it may be used to work other wheels. But when it
 36 I    |           one man must necessarily work four times as long as the
 37 I    |           the total expenditure of work is the same, whether four
 38 I    |             whether four labourers work for a quarter of an hour
 39 I    |           labour, we introduce the work of a weight, and hang to
 40 I    |          also, you will observe no work has been gained, for while
 41 I    |            through one inch is, as work, equivalent to the product
 42 I    |             but that the amount of work is never thereby increased.~
 43 I(1) |           the technical measure of work; to convert it into scientific
 44 II   |      motive force, and can produce work, is called vis viva. The
 45 II   |      velocity has been lost by the work which they have performed.~
 46 II   |           mechanics, of performing work. This would also be the
 47 II   |           mass. It is equal to the work, expressed in foot-pounds,
 48 II   |        weight goes from a to m the work of the raised weight is
 49 II   |           viva is changed into the work of a raised weight. Thus
 50 II   |            raised weight. Thus the work which the arm originally
 51 II   |       spring can, however, perform work; it gradually expends this
 52 II   |       stretch the cord my arm must work for a few seconds; this
 53 II   |            for a few seconds; this work is imparted to the arrow
 54 II   |    extremely short time the entire work which the arm had communicated
 55 II   |     several days. In both cases no work is produced which my arm
 56 II   |          already seen is a form of work.~In this case, then, I have
 57 II   |          case, then, I have gained work which my arm has not performed.
 58 II   |       under the influence of which work has been gained.~Elastic
 59 II   |        cases liquid is raised, and work thereby produced.~The same
 60 II   |           the machine, and furnish work.~You all know how powerful
 61 II   |           the further capacity for work of the natural forces is
 62 II   |     diminished or exhausted by the work which has been performed.
 63 II   |         namely, that to mechanical work - had not been accurately
 64 II   |          endeavoured to deduce the work which heat performs, by
 65 II   |           the capacity of heat for work, which even now, though
 66 II   |         equivalent of a mechanical work; so long as this velocity
 67 II   |     apparently also the mechanical work which this velocity could
 68 II   |      processes in which mechanical work is destroyed, and heat produced
 69 II(2)|           technical measure of the work we must divide it by the
 70 III  |          foot pounds the amount of work which is destroyed by the
 71 III  |     produced by the consumption of work, a definite quantity of
 72 III  |             a definite quantity of work is required to produce that
 73 III  |        centigrade. The quantity of work necessary for this is, according
 74 III  |          experiments, equal to the work which a gramme would perform
 75 III  |         relations between heat and work were also found in the reverse
 76 III  |            process - that is, when work was produced by heat. In
 77 III  |      producing large quantities of work, as in the case of the steam
 78 III  |         does it. Gas thus performs work, and this work is produced
 79 III  |            performs work, and this work is produced at the cost
 80 III  |           compressed, and how much work is necessary for their compression;
 81 III  | equivalence of heat and mechanical work in friction, as close an
 82 III  |        into a definite quantity of work; this quantity of work can
 83 III  |          of work; this quantity of work can also be retransformed
 84 III  |        form in which a quantity of work may appear.~These facts
 85 III  |    transformed into other forms of work, or results afresh from
 86 III  |           forces which can produce work - I mean the chemical. We
 87 III  |          the ultimate cause of the work which gunpowder and the
 88 III  |      carbon and of oxygen performs work just as much as that which
 89 III  |         just as the same amount of work is produced when a weight
 90 III  |      longer produce either heat or work any more than a fallen weight
 91 III  |        than a fallen weight can do work if it has not been again
 92 III  |          once more the capacity of work which they had before they
 93 III  |        carbon for oxygen, performs work in combustion, which appears
 94 III  |       before, but its capacity for work is lost. Hence the two elements
 95 III  |            for it its capacity for work.~We here become acquainted
 96 III  |    acquainted with a new source of work, the electric current which
 97 III  |       affinity which is capable of work, it is here lost. The electrical
 98 III  |          this case, we can restore work which has been lost, but
 99 III  |       turns the wheel produces the work which is required for separating
100 III  |          raised weight can produce work, but in doing so it must
101 III  |            but it can no longer do work.~A stretched spring can
102 III  |            stretched spring can do work, but in so doing it becomes
103 III  |            of a moving mass can do work, but in doing so it comes
104 III  |          to rest. Heat can perform work; it is destroyed in the
105 III  |        Chemical forces can perform work, but they exhaust themselves
106 III  |    Electrical currents can perform work, but to keep them up we
107 III  |            that their capacity for work is exhausted in the degree
108 III  |        which they actually perform work.~We have seen, further,
109 III  |        fell without performing any work, it either acquired velocity
110 III  |  electrical currents or mechanical work.~We have seen that heat
111 III  |           heat may be changed into work; there are apparatus (thermo-electric
112 III  |          whenever the capacity for work of one natural force is
113 III  |          force which is capable of work. The connections between
114 III  |   accustomed to measure mechanical work, and how the equivalent
115 III  |          and how the equivalent in work of heat may be found. The
116 III  |           found. The equivalent in work of chemical processes is
117 III  |       relations, the equivalent in work of the other natural forces
118 III  |   expressed in terms of mechanical work.~If, now, a certain quantity
119 III  |     certain quantity of mechanical work is lost, there is obtained,
120 III  |           an equivalent of heat or work; so that in all these interchanges
121 III  |          all the forces capable of work in the whole universe remains
122 III  |   practical interests of technical work, we have been led up to
123 III  |  understood a machine which was to work continuously without the
124 III  |           the expenditure of fuel. Work is wealth. A machine which
125 III  |        machine which could produce work from nothing was as good
126 IV   |            the great operations at work in the life of the earth