In the 1930’s, the Physics Laboratory of the Faculty of Science of the University of Porto would buy, from Adam Hilger, Ltd., London, a constant deviation spectrometer. The ultimate purpose was to set up a spectroscopy laboratory for teaching and research. This model’s robust construction (the telescope and the collimator are rigidly fixed) makes it adequate for student’s practice.
To sweep across the spectrum, all it takes is to rotate the high quality, constant deviation prism – known as Pellin‐Broca prism. Spectra in the 390‐900 nm interval are observed, either directly, or through photographic recording, or even by using a thermopile and associated galvanometer, when working in the infra‐red range. The wavelength of the line under observation is read straight on a drum, which is fixed to the prism’s rotation mechanism.
Details of the construction and operation of this spectrometer are explored, against the background of present day spectrometers, automatic and computerized, thereby offering a deeper understanding of spectroscopic analysis: for instance, the use of the raies ultimes powder, a mixture of 50 chemical elements whose emission spectra provide a way of calibrating the instrument.
The practice of spectroscopy goes as far back as the 17th century, when Isaac Newton investigated the spectrum produced by the dispersion of sunlight by an optical prism and concluded that visible light is nothing more than the non-uniform mixture of different, more or less refrangible, radiations (fig. 1). The term “spectrum” was coined by Newton himself. In 1802, the British physicist Thomas Young evaluated, for the first time, the wavelength and frequency of each color of the solar spectrum, by applying his wave theory of light to the phenomenon of interference in thin films1: 424 and 675 nm (originally in inches) were then yielded as the lower and upper wavelength boundaries for visible light. In the same year, William Hyde Wollaston, a British chemist, also observed for the first time some of the dark lines that cross the whole of the visible spectrum of sunlight, which he considered to be the limits of the different colours2.
Twelve years later, the optician Joseph Fraunhofer created a device to observe the dark (absorption) lines in the Sun’s spectrum (today known as “Fraunhofer lines”), where an illuminated slit and a lens were placed before the prism3 (fig. 2a). His device was later transformed by two German scientists, the physicist Gustav Kirchhoff and the chemist Robert Bunsen, into a much handier and more precise observation and measurement instrument, the spectroscope4 (fig. 2b). Working together, they demonstrated that each chemical element has a unique spectrum, and established spectroscopy as a powerful method of analysis. Therefore, they are regarded as the founders of modern spectroscopy.
As a result of these contributions, the science of spectroscopy evolved rapidly: the leading optical instrument manufacturers of the 19th century rushed to produce new and diverse spectroscopes, put on display in the 1862 International Exhibition, held in London5.
Meanwhile, the appearance of photography offered the possibility of recording the observations permanently (the first photograph of a spectrum can be traced down to 1842, when the French physicist Alexandre-Edmond Becquerel placed a daguerreotype plate in front of a solar spectrum to record its image6): spectrographs came forward, where spectra can be recorded and studied at a later time, as well as spectrometers, for accurate measurement of the wavelength.
The first decades of the 20th century saw the increasing development of spectroscopy, which became very important, not only in chemical analysis but also in the understanding of the atomic structure. Existent experimental procedures were refined, new methods and techniques were created; the acknowledgement of spectroscopy as a fundamental resource in the metallurgical industry led to the manufacture of high standard instruments in response to market demands. Prisms were replaced by diffraction gratings, for linearity. The improvements in grating fabrication, mechanical stability, elimination of stray light and temperature control led to today’s large spectrometers that can achieve wavelength resolution below 0.1 picometer. For spectral details, the Scanning Fabry-Pérot Interferometer can reach resolutions below 1 femtometer.
THE HILGER CONSTANT DEVIATION WAVELENGTH SPECTROMETER
In the early 1930’s, the Physics Laboratory of the Faculty of Science of the University of Porto would buy, from Adam Hilger, Ltd., London, a constant deviation wavelength spectrometer (though the precise date of this acquisition is still unknown, it has been found that the spectrometer’s accessories are marked down in an Adam Hilger, Ltd. catalogue published in 1930). Spectrometer and accessories are presently in the collection of scientific instruments of the Museum of Science of the Faculty of Science, with a range of accessories which, according to the trade catalogue7, were adequate for general spectrum analysis. The firm’s logotype, as well as a reference number, is engraved both in the spectrometer and in all its accessories. Many components – such as screws, hollow tubes, etc. – are made of brass and finished by a distinct dark red varnish.
Adam Hilger was a company founded by two German precision optical instrument makers technicians, Adam e Otto Hilger. In 1902, Frank Twyman was appointed General Manager; he was an engineer, who had been working with Otto Hilger since 1898, on the development of spectroscopic instruments. Twyman would spend the next ten years developing methods for spectrochemical analysis and designing new devices, thereby becoming an authority in the industrial application of spectrochemistry8.
In academic laboratories, spectroscopy was chiefly used as a means of teaching optics, and associated instruments were deliberately made with as much room for adjustment as possible so that the students might learn the working principle of the instrument rather than use it as a research tool9. For this reason, and given that this spectrometer is intended to work in the visible and near UV - when most spectral lines lie in the UV range - we believe that teaching may have been the main purpose of this acquisition, though the intention of initiating research in spectroscopy should not be excluded. However, as far as we know, no scientific work has been done in this period, in connection with spectroscopy.
The constant deviation spectrometer was first designed, in 1904, by Frank Twyman, using the so-called Pellin-Broca prism. This is a visual instrument, in which the telescope and the collimator are rigidly fixed; all it takes to sweep through the spectrum is to rotate the prism, which makes it adequate for student’s practice11 (fig. 4a).
According to the catalogue, the 1926 design results from several improvements, following the identification of a few faults in earlier models. It is worth mentioning the cover that completely envelops the prism table and the sweeping gear, and fully adjusts to the collimator and telescope, protecting all optical elements from dust and fumes generated during operation. It also reduces any unwanted light and spurious reflections, creating a field background with extreme blackness, so that the faintest lines can be observed. The prism is stabilized by a process that resulted from research carried out by the British Scientific Instrument Research Association, whereby both tarnishing and clouding of the surfaces are very greatly retarded, enabling its use for many years without the need for cleaning12.
Either the telescope or the collimator comprise a tube rigidly screwed to the spectrometer’s body, in whose interior another tube slides back and forth and can be drawn out altogether; the alignment of these tubes is guaranteed by construction with the highest precision. An objective glass inside the telescope can be focused by a side screw attached to a scale seen through a small window, to enable repetition. The telescope and the collimator, at right angles to each other, are aligned with the two solid and heavy feet of the base, which makes the spectrometer stable and space saving.
The instrument owned by the Museum of Science of the Faculty of Science (fig. 4b), with the catalogue reference D78, shows signs of wear, keeping however most of the accessories bought at the time; the optical prism is in excellent condition. The full set may have cost a little more than 100 sterling pounds (an estimation has been made using the costs listed in the 1930 catalogue, given that no invoice has been found).
The constant deviation prism
The dispersive element of the spectrometer is a constant deviation prism (or Pellin-Broca prism), with a refractive index of 1.74 for the D-line (fig. 5). This prism was first introduced in 1899, by André Broca and Ph. Pellin13: its configuration equals the combination of two 30° and one 45° prisms, for which the sought minimum deviation condition occurs at 90° for radiation of any wavelength. To pass through the spectrum, all it takes is to rotate the table sustaining the prism by means of a micrometric screw. A duralumin drum (fig. 6) is fixed to this screw, bearing a helical scale, from 390 to 900 nm (the unit that has been used through the entire catalogue is the angström).The wavelength of the line under observation is directly read off the scale, without the observer having to quit the eyepiece; the wavelength scale is over 1 meter long, which enables high precision readings, particularly when small wavelengths are concerned. The smallest division is 1 nm, however, it is possible, in the blue and violet ranges, to read an extra figure through estimation.
Accessories for the telescope
This spectrometer has originally a shutter eyepiece, suited for observation in the visible range (fig. 7), with a positive eyepiece, sliding shutters in the focal plane and a metal pointer. The two shutters can be shifted in from either side to cover any part of the field of vision, thereby obscuring bright spectral lines so that feebler ones in the proximity can be observed. The metal pointer’s point is ground extremely fine, polished bright and illuminated from above by a small swivel mirror. A slide with light filters gives the pointer any desired color, to provide comfort and increase accuracy in reading, particularly in the violet range of the spectrum; it also has the advantage of removing parallax almost entirely. The position of this pointer can be adjusted laterally by two screws.
This eyepiece can be replaced by the symmetrical slit mount (fig. 8), mounted on a tube to fit the telescope, with a recess in a block into which a thermopile fits, thereby increasing the spectrometer’s sensitivity in the infrared portion of the spectrum. There is an eyepiece for observation of the slit and thermopile, the width of the slit being adjusted by a large milled ring, divided down to 0.001 inch.
Accessories for the collimator
The collimator of the spectrometer has a slit (fig. 9) with fine screw adjustment and associated divided drumhead (missing); the jaws of the slit are made of untarnishable metal, with screws for correcting want of parallelism. A comparison prism allows the approach of two spectra. A sliding diaphragm with three apertures (Hartmann diaphragm) can be used for spectrum photography, giving the spectra in close juxtaposition.
The symmetrical slit (fig. 10), is another type of slit, adjustable by a large milled ring, with division readings down to 0.001 inch. The maximum slit length to be used is 11 mm, which can be increased to 20 mm by removing a diaphragm usually screwed in from the front.
If the telescope is replaced by a photographic camera, the spectrometer turns into a spectrograph. The 1930’s acquisition included such a camera (Fig. 11). Made entirely of metal, it records the whole of the visible spectrum across the larger dimension of a “quarter plate”. The camera is designed to work in conjunction with the object glass of the telescope, with which it forms an optical system based on the telephoto principle, showing an equivalent focal length of 21 inch (53.3 cm). It can be set in position very quickly by removing the telescope draw tube: accuracy of alignment is assured by the geometric fitting. Focusing is achieved by the object glass of the telescope, and readings repeated by means of the scale and index mentioned above. Though the focal length is 21 inch, the front edge of the camera extends only 3 inches (7.6 cm) beyond the position normally occupied by the eyepiece. By means of a rack and pinion adjustment, one plate can take several exposures.
The procedure by which a substance is led to emit radiation, suitable for its spectroscopic analysis, falls into four classes: flame, electric arc discharge, spark discharge and vacuum tube discharge. The flame spectrum can be obtained from some metals or their salts, by placing a small amount of a substance or of its strong solution in a Bunsen flame. This method is mainly adequate for alkaline or alkaline-earth metals. The electric arc came to be one of the preferred methods when direct current with voltage from 150 to 220 V became available; however, with alternate current or lower voltages, spectra can be created by using carbon electrodes. It is thus possible to obtain spectra from metals, metallic alloys, powders, precipitates, dry residues from solutions, etc. To produce spectra from spark discharge, a small transformer with a 15,000 V output on open circuit is needed.
The Physics Laboratory of the Faculty of Science also bought from Adam Hilger, Ltd., a Gramont Arc and Spark Stand (fig. 12), an electrode holder designed by Arnaud de Gramont14, with all exposed metal parts made of stainless steel and insulation in non-inflammable zylonite (a trade name for cellulose acetate), safe enough for tensions up to 20,000 V. This design allows any desired position of the arc or spark to be attained. With this electrode holder, metal or carbon electrodes with section diameter from 4 to 10 mm can be used, as well as small specimens of metal or other conductive materials, held by spring clips, and non-conductive powders (slags, glasses, precipitates, residues from solutions, etc.) held in small platinum cups. An adjustable pointer on a swinging arm can be fitted to the stand and is of assistance in setting the height of the arc or spark gap: this becomes important when two or more sets of electrodes have to be interchanged in one series of exposures.
The spark is excited by a transformer, which includes an autotransformer running on A.C.: high voltages are obtained by suitable tappings on the auto-transformer. For sparking between electrodes, a 0.006 μF condenser is connected in parallel with the spark gap (fig. 13). These devices were supplied by Adam Hilger, Ltd., though manufactured by other firms, under their specifications (the condenser, for instance, shows the logotype Dubilier).
The Physics Laboratory also owned a Hitchen apparatus (meanwhile gone missing), to enable the observation of spectra produced by sparks from liquids and solutions, with the accuracy already achieved for metallic alloys. It was a sparking vessel for liquids (fig. 14), designed to work with the Gramont arc and spark stand, showing advantage over other existing vessels for the same purpose (by Hartley, Pollok and Leonard)15. We favour the hypothesis that it may also have been supplied by Adam Hilger, Ltd., given that one of its inventors, Frank Twyman, was considered to be at the time one of the leading experts in spectroscopy and, as said previously, was the firm’s General Manager.
To examine the absorption spectra of liquids and solutions, an adjustable thickness absorption tube, designed by Edward Baly16, was also bought by the Physics Laboratory and can still be seen in the collection (fig. 15). It consists of two glass tubes, which fit loosely one inside the other, the outer tube being about 1 inch wide and 5 inches long. Both tubes have one end with flange ground flat and square to the axis, upon which a circular quartz plate is cemented. A bulb shaped container is sealed to the side of the outer tube, to take aside the solution when the thickness of layer is decreased by pushing the inner tube. The outer tube has a millimeter scale etched upon it, for readings of the thickness of liquid. A broad rubber band is slipped over the junction in order to keep it watertight. The cell is filled up with the liquid or solution under observation: over the same exposure time, various spectra can be recorded for different thicknesses of a solution with a given concentration, or for the same thickness of solutions with different concentrations. The required attachments to place the Baly cell in front of the collimator tube were also bought at the time.
Two chemists reputedly made major contributions to spectral analysis: Walter Hartley e Arnaud de Gramont. Hartley, an English scientist and pioneer in the field, had, by 1882, investigated the proportions of certain metals whose presence in a compound was made evident by the appearance of their lines in the spectrum. His work was continued by Pollok and Leonard. They distinguished the lines of each particular metal by Greek letters, which denoted the persistence of the spectrum line as the amount of metal in presence was reduced17:
Pollok’s nomenclature for the sensitive spectrum lines of metals in solution.
|τ||Seen with the metal, but not with strong solutions|
|σ||Seen with strong solutions, but not with 1% solutions|
|φ||Seen with 1% solutions, but not with 0.1% solutions|
|χ||Seen with 0.1% solutions, but not with 0.01% solutions|
|ψ||Seen with 0.01% solutions, but not with 0.001% solutions|
|ω||Seen with 0.001% solutions|
This way, W. Hartley and his co-workers laid the foundations for quantitative spectral analysis, dealing essentially with solutions. De Gramont (Arnaud de Gramont published in 1923, together with F. Lecoq De Boisbaudran, Analyse Spectral Appliquée aux Recherches de Chimie Minérale, in two text volumes and one atlas of drawings, to be found in the Library of the current Department of Physics and Astronomy) followed the same line of thought, working chiefly with metals in solid state. Hartley and co-worker’s sensitive lines were named by him as “les raies sensibles”; lines that persisted even with the smallest amounts of metals in solution he called “les raies ultimes”. This expression may have first been used by de Gramont in 190718. He established a limit for the appearance of the whole spectrum (“limite d’apparition total”), above which all the lines of an element would be present, and below which the lines would be vanishing. The lines to persist the last make up the “raies ultimes”, to be identified in order to quantify small amounts of an element. In the 1907 publication, de Gramont listed the wavelengths of the “raies ultimes” for various metals. These lines are not necessarily the strongest lines in the spark spectrum of the element, but show in its arc spectrum, where they are generally of great intensity; they are generally also present in the spectra of very hot flames.
Adam Hilger, Ltd. also supplied spectroscopically standardized substances, such as R.U. powder (after “Raies ultimes”), of which he was the sole supplier; this powder had been developed by J. W. Ryde e H. G. Jenkins at the Research Laboratories of the General Electric Company, Ltd., Wembley, UK19, consisting of traces of fifty elements incorporated in a suitable base material (zinc, magnesium and calcium oxides). The quantity of each element had been carefully adjusted so that the arc spectrum showed, on the average, about seven lines per element. In making a spectroscopic analysis, the arc spectrum of ten to twenty milligrams of the R.U. powder was overlapped to the spectrum of the material to be examined, as a comparison spectrum. All the elements present as impurities in the substance under examination would produce lines coincident with the corresponding lines in the R.U. spectrum. Therefore, the identification of the elements present in the material could be made promptly, without wavelength determinations.
Along the 1930’s, in order to make the use of the Hilger spectrometer more versatile, a few accessories would be manufactured locally: a Zeiss-type optical bench with fitting carriages, an electric arc with electrodes at a right angle, a Gramont arc and spark stand and a magnesium lamp with clockwork.
In 1964, the Physics Laboratory bought another constant deviation wavelength spectrometer from Hilger & Watts (Adam Hilger, Ltd. had amalgamated with E. R. Watts in 1948)20, together with a grooved iron bar for mounting accessories, a photographic camera with slides taking “quarter plates”, and a Ramsden eyepiece.
Nowadays most laboratories have computer controlled spectrometers, and most students never get the possibility to look directly at a line spectrum, to appreciate the color hues and relative brightness of the lines. We consider that, in laboratory practices, a direct view spectrometer, or a spectroscope, in parallel with a computer controlled one, is a must. Students can better grasp the limitations of the instrument with a simpler version close at hand. The teaching practice along the years has convinced us that this approach is important (as a side remark, it should be said that the direct view spectrometer allowed a university student to discover, a few years ago, that he had a lesser form of color blindness). Following suit with this belief, the spectrometer supplied by Hilger & Watts in 1964 is still used in spectrometry teaching classes, along with two computer assisted small spectrometers, providing different spectral ranges (fig. 17). In addition to the benefits already pointed out, students are shown that “size actually matters”, for obtaining better resolution.
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