of Venus fall in that part of the earth's orbit which we pass in the beginning of June and December transits always occur in those months. Tint transit of June 3d, 1769, excited great interest King George III. fitted out an expedition to Tahiti, under the command of the celebrated navigator Capt. James Cook. In order to make the angle as great as possible, and so increase the length of the chords, or paths of the planet across the sun, astronomers were sent to all the most favorable points of observation—St. Petersburg, Pekin, Lapland, California, etc. The result of these calculations fixed the solar parallax at 8.58". This was considered accurate until lately, but has now ceased to have any value. The next transits will happen, December 8 1874. "6 1882. June 7 2004. The first transit ever seen was witnessed by Horrox, a young amateur astronomer residing near Liverpool. TTia calculations fixed upon Sunday, Nov. 24,1639 (O. S.) He however commenced his watch of the sun on Saturday preceding. On the following day he resumed his observation at sunrise. The hour for church arriving, he repaired to service as usual. Heturning to his labor immediately afterward, he says: "At this time an opening in the clouds, which rendered the sun distinctly visible, seemed as if Divine Providence encouraged my aspirations; when—oh most gratifying spectacle! the object of so many earnest wishes—I perceived a new spot of perfectly round form that had just entered upon the left limb of the sun." . The transits of Mercury are more frequent; but owing to the nearness of the planet to the sun, they are of little value in deterrnining the solar parallax. The difficulty of determining the solar parallax accurately will be seen, when one is told that the correction from the old value of 8.58" to the new one of 8.94", is a change in the angle equal to that which the breadth of a human hair would make when seen at a distance of 125 feet. Yet this reduces the estimated distance of the sun from 95,293,000 miles, to 91,430,000 miles. 4. TO FIND THE LONGITUDE OP A PLACE.—(1.) The solar method.—If the sailor can see the sun, he watches it closely with his sextant; and when it ceases to rise any higher in the heavens it is apparent noon. By adding or subtracting the equation of time (as given in his almanac), he obtains the true or mean noon. He then compares the local time thus obtained, with the Greenwich time as kept by the ship's chronometer. The difference in time reduced to degrees, etc., gives the longitude. < (2.) The lunar method.—On account of the difficulty in obtaining a watch which will keep the exact Greenwich time through a long voyage, the moon is more generally relied upon than the chronometer. The Nautical Almanac* is always published, for the benefit of sailors, three years in advance. It gives the distance of the moon from the principal fixed stars which lie along its path, at every hour in the night. The sailor has only to determine with his sextant the moon's distance from any fixed star, and then by referring to his almanac find the corresponding Greenwich time. By comparing this with the local time, and reducing the difference to degrees, etc., he obtains the longitude. 5. TO FIND THE LATITUDE OF A PLACE.—(1.) By means of the sextant find the elevation of the pole above the horizon, and this gives the latitude directly. (2.) In the same manner, determine the height of the sun above the horizon at noon. The sun's declination for that day (as laid down in the almanac), added to or subtracted from this gives the height of the equinoctial above the horizon. Subtract this from 90°, and the remainder is the latitude. * It is pleasant to notice that the astronomer can predict with the utmost precision. He announces that on such a year, month, day, hour, and second, a celestial body will occupy a certain position in the heavens. At the time indicated we point our telescope to the place, and at the instant, true beyond the accuracy of any timepiece, the orb sweeps into view I A prediction of the Nautical Almanac is received with as much confidence as if it were a fact contained in a book of history. "On the trackless ocean, this book is the mariner's trusted friend and counsellor; daily and nightly its revelations bring safety to ships in all parts of the world. It is something more than a mere book. It is an everpresent manifestation of the order and harmony of the universe." 6. TO FIND THE CIBCUMFEBENCE OF THE EABTH.—If the earth were a perfect sphere, it is obvious that degrees of latitude would be of the same length wherever measured on its surface. Each would be -^ of the entire circumference. If, however, a person sets out from the equator, and travels along a meridian toward either pole, and when the polar star has risen in the heavens one degree above the horizon, he marks the spot, and then continues his journey, marking each degree in succession, he will find that the degrees are not of equal length, but increase gradually from the equator to the pole. If now the length of a degree be measured at different places, the rate of variation can be found, and then the average length be estimated. Measurements for this purpose have been made in Peru (almost exactly at the earth's equator), Lapland, England, France, India, Russia, etc. So great accuracy has been attained, that Airy and Bessel, who have solved the problem independently, differ in their estimate of the equatorial diameter but 77 yards, or only y^ • of a mile. 7. To FIND THE BELATIVE SIZE OF THE PLANETS.— The volumes of two globes are proportional to the cubes of their like dimensions. The diameter of Mercury is 2,962 miles, and that of the earth 7,925; then, The volume of Mercury : the volume of the earth :: 2962' : 7925». The same principle applied to the volume or bulk of the sun gives— The bulk of the sun : bulk of earth :: 854584" : T9S5». 8. TO FIND THE DIAMETER OF THE SUN.—(1.) A Very simple method is to hold up a circular piece of paper before the eye at such a distance as to exactly hide the entire disk of the sun. Then we have the proportion, Ai dlit. of paper dlik : dirt, of san-s dick :: diam. of paper d. : diam. son-s d. (2.) The apparent diameter of the sun, as seen from the earth, is about 32': the apparent diameter of the earth, as seen from the sun, is twice the solar parallax, or 17.88". Thence, the Ap. diam. of earth : ap. diam. of son :: real diam. of earth : real diam. of son. (3.) Knowing the apparent diameter of the sun, and its distance from the earth, the real diameter is found by Trigonometry. In figure 95, let S represent the earth, AB the radius of the sun, and ASB half the apparent diameter of the sun. We shall then have the proportion, AS : AB :: radius : sin. 16- (half mean diam. of sun). By a similar method the diameters of the planets are obtained. |