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THE EXPANSION OF STEAM.

149

Properties of Satdrated Steam Continued.

Pressure inlbs. persquare inchabove thepressureof theatmosphere.

Temperaturein degrees ofFahrenheit.

Total Heatin degrees ofFahrenheit.

Cubic inchesof water toproducex cubic footof Steam,according toPambour.

Volume of Steam producedby 1 of water.

Weight of

1 cubic footof Steamin lbs.

Pambour.

Other

Authorities.

93

333'3

1215-6

6-32

273

251

2278

94

334o

1215-8

6-37

27I

249

2298

95

334-6

I 2 -0

6-42

269

247

2317

96

3353

1216*2

6-47

267

245

2334

97

33 6 -o

1216-4

6-52

265

243

2351

98

336-7

1216-6

6'57

263

24I

2370

99

337'4

1216-8

6 " Ö 2

261

239

2388

IOO

338 -o

1217*0

6-67

259

237

2406

IOI

338-6

1217*2

6-72

257

235

2426

102

339-3

1217-4

6-77

255

233

2446

103

339-9

1217-6

6-82

253

231

2465

104

34 o -5

1217-8

6-88

251

229

2484

105

34 i-i

I 2 l 8'0

6'93

249

227

2503

106

341-8

I 2 l 8'2

6-99

247

225

2524

107

342-4

1218-4

7-04

245

224

2545

108

343 '°

1218-6

7 *i 1

243

222

2566

IO9

343-6

12187

r 17

24I

221

2587

HO

344'2

1218-9

7-23

239

2 X 9

2608

111

344-8

1219*1

7' 26

238

217

2626

112

345-4

1219-3

7'32

236

215

2644

113

346-0

1219*4

7'38

234

214

2662

114

346-6

1219-6

7'45

232

212

2680

115

347-2

1219-8

7-48

231

211

2698

117

348-3

1220*2

T 57

228

208

2735

119

3495

1220-6

7-68

225

205

2771

121

350-6

1220*9

778

222

202

2807

123

351-8

1221*2

7-84

219

199

2846

125

352-9

1221*5

8*0

216

197

2885

127

354 -o

1221*9

8-11

213

194

*2922

I29

355 -o

1222*2

822

210

192

2959

131

356-1

1222*5

8-3

208

189

2996

133

357 ' 2

1222*9

8-42

205

187

-3033

135

358-3

1223*2

8-51

203

184

3070

145

363-4

1224-8

9-04

191

174

3263

155

368-2

1225*1

954

181

164

3443

165

372-9

1227*7

10*04

172

155

3623

175

377-5

1229*1

io -53

164

148

3800

185

3817

1230-3

11*0

157

141

3970

Note .According to Rankine and others, the relative volume of steam is less than hasbeen commonly assigned to it by Pambour, following the laws already explained; Pam-bour having treated steam as a permanent gas, instead of as being, what it is in actualpractice, highly saturated.