Table of Equivalent Velocities.

Miles
per
Hour.
Feet
per
Second.
Feet
per
Minute.
Metres
per
Minute.
Metres
per
Second.
1,1·58826·8 ·447
2,2·917653·6 ·894
3,4·426480·51·341
4,5·9352107·31·788
5,7·3440134·12·235
6,8·8528160·92·682
8,11·7704214·63·576
10,14·7880268·24·470
15,22 1,320402·36·705
20,29·41,760536·48·940
25,36·72,200670·511·176
30,44 2,640804·613·411
35,51·33,080938·815·646
40,58·73,5201,072·917·881
45,66 3,9601,207 20·116
50,73·44,4001,341·122·352
60,88 5,2801,609·226·822
70,102·76,1601,877·531·292
80,117·27,0402,145·835·763
90,132 7,9202,414 40·233
100,146·78,8002,682·244·704
110,161·29,6802,950·249·174
120,176 10,5603,218·453·644
130,191 11,4403,486·658·115
140,205·312,3203,755·162·585
150,220 13,2004,023·367·056

To convert feet per minute into
metres per second, multiply by ·00508.

Table Showing Velocity and Thrust Corresponding with Various Horse-Powers.

Velocity
in Miles
per Hour.
Horse-Power.
1102030405060708090100
Thrust in Pounds.
1,375 3,750 7,500 11,250 15,000 18,750 22,500 26,250 30,000 33,750 37,500
5,75 750 1,500 2,250 3,000 3,750 4,500 5,250 6,000 6,750 7,500
10,37·5375 750 1,125 1,500 1,875 2,250 2,625 3,000 3,375 3,750
15,25 250 500 750 1,000 1,250 1,500 1,750 2,000 2,250 2,500
20,18·8187·5375 562·5750 937·51,125 1,312·51,500 1,687·51,875
25,15 150 300 450 600 750 900 1,050 1,200 1,350 1,500
30,12·5125 250 375 500 625 750 875 1,000 1,125 1,250
35,10·7107·1214·3321·4428·6535·7642·8750 857·1964·31,071·4
40,9·493·8187·5281·3375 468·8562·5656·3750 843·8937·5
45,8·383·3166·7250 333·3416·7500 583·3666·7750 833·3
50,7·575 150 225 300 375 450 525 600 675 750
60,6·362·5125 187·5250 312·5375 437·5500 562·5625
70,5·453·6107·1160·7214·3267·9321·4375 428·6482·1535·7
80,4·746·993·8140·6187·5234·4281·3328·2375 421·9468·8
90,4·241·783·3125 166·7208·3250 291·7333·3375 416·7
100,3·7537·575 112·5150 187·5225 262·5300 337·5375

Fig. 72b.—When an aeroplane is driven through the air, it encounters stationary air and leaves it with a downward trend. With a thick curved aeroplane, as shown, the air follows both the top and the bottom surfaces, and the direction that the air takes is the resultant of these two streams of air. It will be seen that the air takes the same direction that it would take if the plane were flat, and raised from a to c, which would be substantially the same as shown at f, h, g. It has, however, been found by actual experiment that the curved plane is preferable, because the lifting effect is more evenly distributed, and the drift is less in proportion to the lift.