Experimental Determination of the Velocity of Light - Part 6
Library

Part 6

June 18

2

75

112.79

0.265

112.52

0.09

1.483

-0.120

257-43

28.158

0.99614

299860

P.M.

June 18

2

75

112.75

0.265

112.48

0.10

1.483

-0.120

257-43

28.158

0.99614

299970

P.M.

June 18

2

75

112.76

0.265

112.49

0.08

1.483

-0.120

257-43

28.158

0.99614

299950

P.M.

June 20

3

60

112.94

0.265

112.67

0.07

1.517

+0.063

257.65

28.172

0.99614

299880

A.M.

June 20

3

61

112.92

0.265

112.65

0.09

1.517

+0.048

257.63

28.172

0.99614

299910

A.M.

June 20

2

62

112.94

0.265

112.67

0.07

1.517

+0.036

257.62

28.172

0.99614

299850

A.M.

June 20

2

63

112.93

0.265

112.66

0.03

1.517

+0.024

257.61

28.172

0.99614

299870

A.M.

June 20

2

78

133.48

0.265

133.21

0.13

1.450

-0.156

257.36

33.345

0.99627

299840

P.M.

June 20

2

79

133.49

0.265

133.23

0.09

1.500

-0.168

257.40

33.345

0.99627

299840

P.M.

June 20

2

80

133.49

0.265

133.22

0.07

1.500

-0.180

257.39

33.345

0.99627

299850

P.M.

June 20

2

79

133.50

0.265

133.24

0.13

1.483

-0.168

257.39

33.345

0.99627

299840

P.M.

June 20

2

79

133.49

0.265

133.22

0.06

1.483

-0.168

257.38

33.345

0.99627

299840

P.M.

June 20

2

79

133.49

0.265

133.22

0.10

1.483

-0.168

257.38

33.345

0.99627

299840

P.M.

June 21

2

61

133.56

0.265

133.29

0.12

1.533

+0.048

257.65

33.332

0.99627

299890

A.M.

June 21

2

62

133.58

0.265

133.31

0.08

1.533

+0.036

257.64

33.332

0.99627

299810

A.M.

June 21

2

63

133.57

0.265

133.31

0.09

1.533

+0.024

257.63

33.332

0.99627

299810

A.M.

June 21

2

64

133.57

0.265

133.30

0.11

1.533

+0.012

257.61

33.332

0.99627

299820

A.M.

June 21

2

65

133.56

0.265

133.30

0.13

1.533

0.000

257.60

33.332

0.99627

299800

A.M.

June 21

3

80

133.48

0.265

133.21

0.06

1.533

-0.180

257.42

33.330

0.99627

299770

P.M.

June 21

3

81

133.46

0.265

133.19

0.10

1.500

-0.192

257.38

33.330

0.99627

299760

P.M.

June 21

3

82

133.46

0.265

133.20

0.05

1.500

-0.204

257.37

33.330

0.99627

299740

P.M.

June 21

3

82

133.46

0.265

133.20

0.08

1.517

-0.204

257.38

33.330

0.99627

299750

P.M.

June 21

3

81

133.46

0.265

133.19

0.08

1.500

-0.192

257.38

33.330

0.99627

299760

P.M.

June 23

3

89

133.43

0.265

133.16

0.08

1.542

-0.288

257.32

33.345

0.99627

299910

P.M.

June 23

3

89

133.42

0.265

133.15

0.06

1.550

-0.288

257.33

33.345

0.99627

299920

P.M.

June 23

3

90

133.43

0.265

133.17

0.09

1.550

-0.300

257.32

33.345

0.99627

299890

P.M.

June 23

3

90

133.43

0.265

133.16

0.07

1.533

-0.300

257.30

33.345

0.99627

299860

P.M.

June 23

3

90

133.42

0.265

133.16

0.07

1.517

-0.300

257.29

33.345

0.99627

299880

P.M.

June 24

3

72

133.47

0.265

133.20

0.15

1.517

-0.084

257.50

33.319

0.99627

299720

A.M.

June 24

3

73

133.44

0.265

133.17

0.04

1.517

-0.096

257.49

33.319

0.99627

299840

A.M.

June 24

3

74

133.42

0.265

133.16

0.11

1.517

-0.108

257.48

33.319

0.99627

299850

A.M.

June 24

3

75

133.42

0.265

133.16

0.06

1.517

-0.120

257.47

33.319

0.99627

299850

A.M.

June 24

3

76

133.44

0.265

133.18

0.10

1.517

-0.132

257.45

33.319

0.99627

299780

A.M.

June 26

2

86

133.42

0.265

133.15

0.05

1.508

-0.252

257.33

33.339

0.99627

299890

P.M.

June 26

2

86

133.44

0.265

133.17

0.08

1.508

-0.252

257.33

33.339

0.99627

299840

P.M.

June 27

3

73

133.49

0.265

133.22

0.11

1.483

-0.096

257.46

33.328

0.99627

299780

A.M.

June 27

3

74

133.47

0.265

133.20

0.06

1.483

-0.108

257.44

33.328

0.99627

299810

A.M.

June 27

3

75

133.47

0.265

133.21

0.09

1.483

-0.120

257.43

33.328

0.99627

299760

A.M.

June 27

3

75

133.45

0.265

133.19

0.09

1.467

-0.120

257.42

33.328

0.99627

299810

A.M.

June 27

3

76

133.47

0.265

133.20

0.08

1.483

-0.132

257.42

33.328

0.99627

299790

A.M.

June 27

3

76

133.45

0.265

133.19

0.10

1.483

-0.132

257.42

33.328

0.99627

299810

A.M.

June 30

2

85

35.32

135.00

99.68

0.05

1.500

-0.240

193.00

33.274

0.99645

299820

P.M. Mirror inverted.

June 30

2

86

35.34

135.00

99.67

0.06

1.508

-0.252

193.00

33.274

0.99645

299850

P.M. Mirror inverted.

June 30

2

86

35.34

135.00

99.66

0.10

1.508

-0.252

193.00

33.274

0.99645

299870

P.M. Mirror inverted.

June 30

2

86

35.34

135.00

99.66

0.09

1.517

-0.252

193.00

33.274

0.99645

299870

P.M. Mirror inverted.

July 1

2

83

02.17

135.145

132.98

0.07

1.500

-0.216

257.35

33.282

0.99627

299810

P.M. Mirror inverted.

July 1

2

84

02.15

135.145

133.00

0.09

1.500

-0.228

257.34

33.282

0.99627

299740

P.M. Mirror inverted.

July 1

2

86

02.14

135.145

133.01

0.06

1.467

-0.252

257.28

33.311

0.99627

299810

P.M. Mirror inverted.

July 1

2

86

02.14

135.145

133.00

0.08

1.467

-0.252

257.28

33.311

0.99627

299940

P.M. Mirror inverted.

July 2

3

86

99.85

0.400

99.45

0.05

1.450

-0.252

192.95

33.205

0.99606

299950

P.M. Mirror erect.

July 2

3

86

66.74

0.400

66.34

0.03

1.450

-0.252

128.63

33.205

0.99586

299800

P.M. Mirror erect.

July 2

3

86

50.16

0.400

47.96

0.07

1.467

-0.252

96.48

33.205

0.99580

299810

P.M. Mirror erect.

July 2

3

85

33.57

0.400

33.17

0.06

1.450

-0.240

64.32

33.205

0.99574

299870

P.M. Mirror erect.

In the last two sets of June 13, the micrometer was fixed at 113.41 and 112.14 respectively. The image was bisected by the cross-hair, and kept as nearly as possible in this place, meantime counting the number of seconds required for the image of the revolving mirror to complete 60 oscillations. In other words, instead of measuring the deflection, the speed of rotation was measured. In column 7 for these two sets, the numbers 11 and 6 are the differences between the greatest and the smallest number of seconds observed.

In finding the mean value of V from the table, the sets are all given the same weight. The difference between the result thus obtained and that from any system of weights is small, and may be neglected.

The following table gives the result of different groupings of sets of observations. Necessarily some of the groups include others:

Electric light (1 set) 299850 Set micrometer counting oscillations (2) 299840 Readings taken by Lieutenant Nazro (3) 299830 Readings taken by Mr. Clason (5) 299860 Mirror inverted (8) 299840 Speed of rotation, 192 (7) 299990 Speed of rotation, 128 (1) 299800 Speed of rotation, 96 (1) 299810 Speed of rotation, 64 (1) 299870 Radius, 28.5 feet (54) 299870 Radius, 33.3 feet (46) 299830 Highest temperature, 90 Fahr. (5) 299910 Mean of lowest temperatures, 60 Fahr. (7) 299800 Image, good (46) 299860 Image, fair (39) 299860 Image, poor (15) 299810 Frame, inclined (5) 299960 Greatest value 300070 Least value 299650 Mean value 299852 Average difference from mean 60 Value found for p 3.26 Probable error 5

Discussion of Errors.

The value of V depends on three quant.i.ties D, n, and f. These will now be considered in detail.

The Distance.

The distance between the two mirrors may be in error, either by an erroneous determination of the length of the steel tape used, or by a mistake in the measurement of the distance by the tape.

The first may be caused by an error in the copy of the standard yard, or in the comparison between the standard and the tape. An error in this copy, of .00036 inch, which, for such a copy, would be considered large, would produce an error of only .00001 in the final result. Supposing that the bisections of the divisions are correct to .0005 inch, which is a liberal estimate, the error caused by supposing the error in each yard to be in the same direction would be only .000014; or the total error of the tape, if both errors were in the same direction, would be 000024 of the whole length.

The calculated probable error of the five measurements of the distance was .000015; hence the total error due to D would be at most .00004. The tape has been sent to Professor Rogers, of Cambridge, for comparison, to confirm the result.

The Speed of Rotation.

This quant.i.ty depends on three conditions. It is affected, first, by an error in the rate of the standard; second, by an error in the count of the sound beats between the forks; and third, by a false estimate of the moment when the image of the revolving mirror is at rest, at which moment the deflection is measured.

The calculated probable error of the rate is .000016. If this rate should be questioned, the fork can be again rated and a simple correction applied. The fork is carefully kept at the Stevens Inst.i.tute, Hoboken, and comparisons were made with two other forks, in case it was lost or injured.

In counting the sound beats, experiments were tried to find if the vibrations of the standard were affected by the other fork, but no such effect could be detected. In each case the number of beats was counted correctly to .02, or less than .0001 part, and in the great number of comparisons made this source of error could be neglected.

The error due to an incorrect estimate of the exact time when the images of the revolving mirror came to rest was eliminated by making the measurement sometimes when the speed was slowly increasing, and sometimes when slowly decreasing. Further, this error would form part of the probable error deduced from the results of observations.

We may then conclude that the error, in the measurement of _n_, was less than .00002.

The Deflection.