# Indirect measurement

For stars beyond a distance of 1,000 parsecs (parallactic angle 0.001″), the trigonometric method is in general not sufficiently accurate, and other methods must be used to determine their distances.

The parallax can be derived from the apparent magnitude of the star if there are any means of knowing the absolute magnitude of the star—i.e., the magnitude the star would have at the standard distance of 10 parsecs. For many stars a reasonable estimate can be made from their spectral types or their proper motions. The formula connecting the absolute magnitude, *M*, and the apparent magnitude, *m*, with parallax, *p*, is

expressing the condition that the light received from a star varies inversely as the square of the distance.

Some groups of stars, such as the Hyades cluster in Taurus and the Ursa Major cluster, have proper motions converging toward a definite point on the celestial sphere and are called moving clusters. The apparent convergence is due to the effect of perspective on parallel motions. Once the direction toward the convergent point is known, and the proper and radial motion of a member star is known, the parallax can be determined from the geometry.

One method of indirect measurement involves the determination of mean, or average, stellar parallaxes. The solar system is moving through space with a velocity of 13.4 km (8.3 miles) per second, carrying it three times Earth’s distance from the Sun in one year. This produces a general drift in the angular movement of the stars away from the apex, or point in the sky to which the movement is directed. Were the stars at rest, this would give a ready means of determining their individual distances. As the stars are all moving, the method gives the average distance of a group of stars examined, on the assumption that their peculiar motions are eliminated. In this way the mean parallaxes of stars of successive apparent magnitudes, of different galactic latitudes, and of different spectral types are obtained. Thus the mean parallax of fifth magnitude stars (i.e., of stars just visible to the naked eye) is 0.018″, and of the 10th magnitude stars (i.e., of stars each giving about 1/100 of the light of a star of the fifth magnitude) is 0.0027″.

Stellar parallaxes are also deduced from spectroscopic observations. The spectra of nearly all stars can be grouped into a small number of classes, which form a continuous sequence depending on the effective (surface) temperatures of the stars. The Henry Draper (HD) stellar classification, which is of this kind, uses the letters O–B–A–F–G–K–M–L–T to denote classes with temperatures descending from about 50,000 K for class O to about 800 K for class T. The HD system has been generally adopted, usually in combination with a decimal subdivision for refined work.

Empirical studies show that the spectra of the stars also include important clues to their true luminosities. In 1914 Walter Adams and Arnold Kohlschütter established the spectroscopic differences between giant and dwarf stars of the same spectral type and laid the foundation for the determination of spectroscopic parallaxes. These differences, depending upon the intrinsic brightness of the star, allow an estimate of its absolute magnitude, and the parallax can then be deduced by means of the equation (2) given above. This method has been applied to most of the brighter stars in the Northern Hemisphere, using stars of known parallax as standards.

A two-dimensional classification system of stellar spectra, which has been universally adopted, has greatly improved the accuracy of spectroscopic parallaxes. The system, called the MK system, assigns a precise system of Draper classes and five luminosity classes, using the Roman numerals I to V. The system divides the majority of stars into supergiants, bright giants, subgiants, and main sequence (dwarf) stars, depending upon their intrinsic brightness, as determined from the spectral lines most sensitive to this property. The luminosity classes are then calibrated in terms of absolute magnitude.

The colours of the stars can also be used as indicators of their absolute magnitude, as first shown by Ejnar Hertzsprung in 1905 and 1907. A measure of the colour of a star is the difference in brightness, measured in magnitudes, in two selected wavelength bands of its spectrum. Initially the difference between the visual and the photographic magnitude of a star was defined as the colour of its light and called its colour index. A comparison between the colour index and the spectral classification of a star has made it possible to develop a quantitative method of measuring a star’s absolute magnitude. Several photometric systems have been developed. The most widely used system is the two-dimensional quantitative classification method based upon photoelectric measurements in three wavelength bands in the ultraviolet, blue, and yellow (or visual) regions of the spectrum, hence called the *UBV* system. The system of the two colour indices *U-B* and *B-V* is calibrated in terms of spectral class and luminosity class on the MK system, based upon a set of standard stars. The relationship between the two indices in the *UBV* system and the absolute magnitudes for the main-sequence stars is of particular interest. By means of this relationship and the inverse square law, it is possible to determine the distances to galactic clusters from photoelectric observations of main-sequence stars in these clusters. In other words, such photometric parallaxes are obtained from a comparison of the observed apparent magnitudes of the stars and the absolute magnitudes inferred from their spectral types.

If the relative orbit of a visual binary system is known, the following relation connects the combined mass, *M*, of the two stars, expressed in the Sun’s mass as unit; the orbital period, P, expressed in years, the semimajor axis of the relative orbit; *a*, expressed in seconds of arc; and the parallax *p**:* *p* = *a*/^{3}Square root of√*M*P^{2}. Both *a* and P are known, but not *M*; it will be noted that an error in the value of *M* gives rise to a much smaller error in *p*. Thus, for instance, increasing *M* by a factor of 8 only halves the value of *p*. The value of *p* obtained by assuming the combined mass to be equal to the mass of the Sun is called the hypothetical parallax.

In many visual pairs the complete orbit has not been observed. If *s* denotes the apparent distance in seconds of arc and ω the relative motion in seconds of arc per year, a hypothetical parallax can be derived from the formula *p* = 0.418 ^{3}Square root of√*s*ω^{2}. By use of the relationship between mass and luminosity of a star, it is possible, knowing the spectral type of the star, to derive a correcting factor that will give a more accurate value of the parallax. Parallaxes so determined are called dynamical parallaxes.