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An Encyclopaedia of civil engineering : historical, theoretical and practical : illustrated by upwards of three thousend engravings on wood by R. Branston / by E. Cresy
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Chap. XIX.

ATMOSPHERE AS A MOVING POWER.

1221

of cylinders which extended the whole length of the sails, and were put in motion by asystem of wheel work connected with the shaft in the following manner; — a ring of iron about4 inches wide and | of an inch thick, was attached to the main shaft, and concentric with it, ashort distance behind the whip : a bevelled wheel without arms is made to revolve easilyupon the circumference of the ring, and a spur-wheel without arms turns upon four pinsin the back of the same. The whole machinery revolves with the shaft, and when thequantity of canvas spread is too great, a lever fastened to the bracings, and weighed soas to hang vertically, is brought into a horizontal position by means of a string attached tothe end within the mill ; in this position it engages a stud upon the spur-wheel, and pre-vents its motion : a bevelled wheel then gives motion to the four small pinions, and withthem the cylinders, which continue to wind up the cloth, until the miller from within letsgo the string, and the lever is disengaged from the stud.

On the relative Effects of Hint/mill Sails, according to Smeaton and Coulomb .— The velocityof windmill sails, whether unloaded or loaded, producing a maximum effect, is nearlyas the velocity of the wind, their shape and position being similar. The load at themaximum is somewhat less than as the square of the velocity of the wind, the shape andposition of the sails being the same. The effects of the same sails at a maximum are nearly,but somewhat less than, as the cubes of the velocity of the wind. The load of the samesails at the maximum is nearly as the squares, and their effects as the cubes of the numbersof turns in a given time : when sails are loaded, so as to produce a maximum effectat a given velocity, and the velocity of the wind increases, the load continuing the same,the increase of effect, when that of the velocity of the wind is small, will be nearly as thesquares of those velocities : when the velocity of the wind is double, the effects will henearly as 10 to 27 \ ; when the velocities compared are more than double that where thegiven load produces a maximum, the effects increase nearly in the simple ratio of thevelocity of the wind. In sails where the figures and positions are similar, and the velocityof the wind the same, the number of turns in a given time will he reciprocally as theradius or length of the sail: the load at a maximum overcome by sails of a similar figureand position, at a given distance from the centre of motion, will be as the cube of theladitis.

The effects of sails of similar figure and position are as the squares of the radius: thevelocities of the extremities of Dutch sails, as well as of the enlarged sails, in all their usualpositions when unloaded, or even loaded to a maximum, are considerably quicker than thevelocity of the wind.

Number ofAle Gallonsdelivered onan OvershotWheel 10 ft.in diameterevery minute.

Diameter ofthe Cylindersof the com*mon SteamEngine ininches.

Diameter ofthe C> Underof the im-proved SteamEngine ininches.

Number ofHorses em-ployed 9jworking hrs.per day,andmoving at therate oCi milesper hour.

Numberof menworking12 hoursper day.

Radius ofDutch Sailsin their com-mon poMiionin feet.

Radius ofDutch Sails intheir bestposition infeet.

Radius ofMr.smeaton ’senlarged Sailsin feet.

Height towhich theseditlerentpowers willraise 1000 lbs.avoirdupois

minu'e.

230

8-

6 12

1

5

21 -24

17-89

15 65

13

390

9-5

7-8

2

10

30 04

25 30

22-13

26

528

10-5

8 2

3

15

36-80

30-98

27-1 1

39

GCO

11-5

8-8

4

20

42-48

35-78

31 -30

52

790

12-5

9-35

5

25

47-50

40 00

35-(’0

65

970

14-0

10-55

6

30

52-03

43-82

38-34

78

1170

15-4

11*75

7

35

56 -90

47-33

41-41

90

1350

16-8

12-8

8

40

60 09

50-60

44-27

104

1445

17-3

13-6

9

45

63-73

53-66

46-96

117

1584

18-5

14*2

10

50

67 17

56-57

49-50

130

1740

19-4

14-8

11

55

70 46

59-33

51'91

143

1900

20-2

15*2

12

60

73-59

61-97

54-22

156

2100

21-0

16-2

13

65

76*59

64 5

56 -43

169

2300

22 0

17-0

14

70

79-49

66-94

58-57

182

2500

23-1

17-8

15

75

82-27

6928

60-62

195

2686

23-9

18-3

16

80

84-97

71 55

62 61

208

2870

24-7

19 0

17

85

87-07

73 32

64-16

221

3055

25-5

19-6

18

90

901 3

75-90

67-41

234

3240

26-2

201

19

95

92-60

77-98

68 23

247

3240

27 0

20-7

20

100

95*00

80-00

7000

2 r 0

3750

28-5

22-2

22

I 10

99-64

83-90

73-42

2S6

4000

29-8

23 0

24

120

104 06

87-63

76-68

312

4460

31-1

23-9

26

130

108 -32

91 22

79-81

338

4850

32-4

24-7

28

140

112-20

94-66

82-82

364

5250

33-6

25-5

30

150

1 1635

97-98

85-73

390

4 i 3