Fraction Collector Modifications

fraction collectors, such as the Techni- con photoelectric fraction collector (the design shown in the figure is for the. Technieon apparatus). The co...
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Fraction Collector Modifications Eugene A. Talley, Eastern Regional Research Laboratory, Agricultural Research Service, U. S. Department o f Agriculture, Philadelphia 18, Pa.

in fraction are useful during the ion exchange chromatography of amino acids ( 3 ) . A capillary inflow arm (Figure 1) has been substituted for the wider tube frequently employed with drop-counting fraction collectors, such as the Technicon photoelectric fraction collector (the design shown in the figure is for the Technicon apparatus). The columns n-ere fitted uith KO. 12 ball joints. The tubing betn-een these joints and the r e m support was of larger than capillary bize, but should be reasonably short; separation of peaks on the effluent curve was improved if this tubing was air filled rather than liquid filled during elution. The use of this capillary arm minimizes the uptake of ninhydrin-positive materials from the laboratory air and it improves the uniformity of dropping of the eluate. The bevel on the dropping tip can be omitted for large drops. (One of the revieivers suggests that the tip may be beveled by drawing it out n hile blowing into the capillary, thus preventing a significant reduction in bore n hile reducing the outside diameter of the tube.) With large diameter columns. t w o of the connecting tubes can be used in series, permitting a column to be disconnected for regeneration without changing the position of the column. The loner joint can be held by a pinch clamp. The upper joint, however, must be free to rotate in order to permit the shift from one row of the collector to the next. Lon, viscosity grease and a screw-type clamp (KO. C5155, Scientific Glass Apparatus Co.) with a rubber ring for cushioning, were used. Sections of split rubber tubing or tape may be necessary to make the clamps fit the capillary tubing. The second modification is the use of an extra counter to effect a change in the temperature of the water bath used to control the temperature of the columns. In using the IIoore and Stein ion exchange procedure for the determination of amino acids (S), the author found that increasing the flow rate considerably does not appreciably broaden the effluent peaks obtained. Recent developments (2, 4 ) also use increased flow rates. In the case of the 100-em. columns, if the flow rate is doubled, about 200 fractions are collected in 24 hours, which is about the HE TITO

DRIP

MODIFICATIOXS

Tcollecting equipment described

Figure 1.

Capillary in-

TIP

121 I

flow arm for use with the Technicon photoelectric fraction collector

CAPILLARY TUBING

I m m BORE’

GRIND

TIP

BALL‘ JOINT

capacity of the turntables of the fraction collectors used in this work. This is a convenient rate, except that the second temperature change is required a t a time when one is normally absent from the laboratory. An auxiliary counter has been used to switch the control contacts of the relay of the heating bath from one thermostat to another a t any given fraction number. This counter switch is a duplicate of the Microflex reset counter used in the drop-count attachment of the Technicon fraction collector. Thus it also may be used as a spare counter in an emergency. It is Eagle Signal Corp. KO.HZ40A6 with the standard operation sequence arrangement A242. It may be obtained as the open type for installation in a cabinet or as the enclosed type for use outside. This counter as obtained from the manufacturer contains a jumper across contacts L2 and 3 of its terminal block. This jumper must be removed when the counter is to be used in the Technicon drop-count attachment (the jumper across 3 and 4 must also be removed when the counter is used as a replacement drop counter) or for this application. The count coil of the counter must be supplied with a suitable electrical pulse each time a tube is changed, if it is to be used to snitch thermostats or other electrically operated apparatus when a definite number of tubes is filled. The Technicon drop-counting attachment is fitted with a two-wire Twistlock midget flush base (the direct reading counter outlet sholvn in the schematic diagram of the Technicon drop-count control) which furnishes a pulse every time a

drop is registered. By changing the internal wiring slightly, this can be used to furnish a pulse each time a tube is changed. Two wires (one to the multiplier socket and the other to the photoelectric relay chassis) are attached t o one terminal of the direct reading counter outlet. These wires are removed and connected together. The vacant terminal is then connected to terminal 1 of the counter in the dropcount attachment. This can be done rather simply by the use of a jumper from the vacated outlet terminal to contact 24 on the terminal block in the bottom of the drop-counting cabinet. After these changes are made, the multiplier socket is still operative, but the direct reading counter outlet now furnishes an electrical pulse only when the tubes are changed under the dropping tip insteitd of each time a drop is registered. Then a midget size two wire Twistlock cap such as Hubbell KO.7428, can be installed on a cord and used to connect to the count coil of the extra counter when it is being used. Several changes are made also in the auxiliary counter when it is used with the Technicon drop counter. For this application, it is safer to separate the clutch coil wiring from that of the count coil winding as described below. Then the clutch coil can be plugged directly into the line without danger of a short circuit. As furnished, both the count and the clutch coils are connected to terminal L1 of the terminal block of the counter. If the jumper between terminals A and B is removed, the wire from the count coil to L1 can be connected to terminal B. Then the snitch inside the counter and connected across VOL. 31, NO. 2, FEBRUARY 1959

317

trrniinals B and L2 will disconnect the count coil when the count is completed. The count coil is connected to the source of electric pulses (the direct reading counter outlet of the modified Technicon drop count attachment) through terminals M and L2. The clutch coil is connected through terminals L1 and A to the p o m r line in such a may that it may be disconnected easily. The swit.eh in the counter connected across terminals 4 and 2 is closed during the counting period and opens when the count is completed. The switch connected across terminals 1 and 3 has the opposite action. The items to be operated are connected accordingly. Fgr cuainple, for switching from 50" to 75" C. after 75 tubes are filled, the counter is set for 75 (the count will he correct as set for this application), the 50" C. thermostat is connected to terminal 2 and thr 75" C. thermostat to

terminal 1. Terminals 3 and 4, connrrtrd by a jumprr, are connected to our rrlay control terminal. The othrr side of the relay control line is connected to each of the thermostats. The counter as furnished is conditioncd to reset itself on low voltage. This nirans that the counter will reset itself to zcro count if there is a power interruption and then the sn-itching action will take place later than intended when action resumes. The counter is easily eonditioncd for nonreset on low voltage ( 1 ) . When this change is made, the counter will not rrset on power interruption and change the effective count. When starting, the clucrh coil is energized only while the counter is being srt and until the count is to begin and thcn is de-enerxized until one wishes to reset the eountrr again to zcro. If the conntrr is conditioned for reset on low roltagr, the

clutch coil most be energized t h m u ~ h o u t the entire counting period. To condition the rounter for use as a rcplnccmrnt for the counter in the, Technicon drop-countcr attachment, the entirr procedure dwcribcd in the last paragraph above and the first half of the prcrious parsgraph is reversrd. LITERATURE CITED

(1) Eagle

Signal Corp., >lolint., Ill., Micraflex IMl. llOC, 720. (Direct bulletin rcansstn to IC. F. IIavev.) (2) Hamiltod, 1'. E., AS.AL. C&;. 30, (3) Moon Chem. 192, 663-81 (1951).

(4)Spackman, I). H., Stein, IT. H., Moore, A,, Federelion Proc. 15, 358 (1856).

MENTION of trade names or companies in this paper docs not imply endorsement hy the Department of Agriculture over other? of qimilar nature not nientioned.

Electron Diffraction Study of Ferromagnetic Inclusion in Austenitic Stainless Steel Shigeto Yamaguchi and Yoshio Aoyama, Scientific Research Institute, 3 1 Kamifuii (Hongo), Tokyo, Japan HE EDGE of an electron beam is Tdefleeted by a magnetic field, eausing the Lorentz effect which is observable in the diffraction pattern obtained from a ferromagnetic substance. The edge of a razor (10 X 10 mm.), slightly polished electrically, was suitable for the electron transmission experiment [Yamaguchi, S., J . A p p l . Phys. 25, 811 (1954)l. The thickness of this edge was about 3000 A. Figure 1 shows the diffraction pattern of the ferromagnetic hard steel and that of the nonferromagnetic gold foil, which was photographed by means of double

piece of k e n i t i c stainless Steel (10 X 10 X 1 mm.) was shammed b r mechanical polishing. Here 'a strain-

induced transforination took plrrre a t the edge of the specimen, so that a comparatively thick layer of ferromagnetic ferrite (body-ccntrred lattice) is formrd. The frrroma7netic particles thus obtained in the specimen are magnetically oriented during the mechanical polishing. The edge of thc specimen and the gold foil w r e photographed by the same procrss as for Figures 1 and 2. In Figure 3, the rings of the specimen and those of gold are not concentric. The edge of the specimrn in Figure 3 was sharpcned by mechanical polishing. A satisfactorv strain-induced transformation from the original austenitic state to the ferritic state occurs in this process. The series of diffraction ring@

Figure 2. Gold and aluminum tiydroxide (boehmite); no Lorentz effect observed

Figure 3. Gold and stoinless steel. The specimen of austenitic stainless steel was polished mechonicolly; strong Lorentz effect observed T V a w Icngth, 0.0294 A.

n Figure 1. Diffraction patterns of gold and of hard steel os photographed b y double exposure. The rings due to the gold and those caused b y the steel a r e not concentric as a result of the . - . Lorenfz enect

ITave Imgth, 0.0292 A. Camera length, 485 mm. Po-itive enlnrged 3.2 times 318

ANALYTICAL CHEMISTRY