Measurement of the magnetic exchange in a chlorobridged Cu (II

Harold C. Nelson, and Juan F. Villa. J. Chem. Educ. , 1980, 57 (5), p 385. DOI: 10.1021/ed057p385. Publication Date: May 1980. Cite this:J. Chem. Educ...
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Harold C. Nelson' Princeton University Princeton. NJ 08540 Juan F. Villa Herbert H. Lehman College City University of New York Bronx, NY 10468

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Measurement of the Magnetic Exchange in a Chlorobridged Cu(ll) Dimer Advanced inorganic experiment employing the Faraday magnetic susceptibility system

Magnetic exchange involves the coupling of electron spins through space (direct exchange) or through bridging groups (wperexchnnge) 111. Thc spins may couple in a parallcl or antiparallel fashion as shown in Figure 1. In rhr former nrraniement the material is said to be ferromagnetic while in the latter arrangement the material is said to be antiferromagnrtic. Measurement oi the drgree of the exchangr interacriun, W, in transition mrml dimers and, t o lesser ~ extent, trimers and tetramers have become active areas of research in recent years ( 2 4 ) . The value of W in copper(I1) dimers has been correlated with the metal-liaand-metal angle (3) as well as with specific delocalization mechanisms (4). Although a variable tem~eraturemaanetic susce~tibilitvmeasurement is not the onG means of measuring the-magnitude and sign of the exchange interaction, the method is the most accurate and the one most often employed, and can be used to obtain related magnetic variables (e.g., g and TIP, uide infra). However. there is no descriotion of an exoeriment desiened for such a determination dy students although the experiment mav he emoloved . . easilv and orofitablv. This Daoer - . is intended to supply such a description. Copper(I1) dimers provide theoretically simple models (5) and are pedagogically appealing since the exchange can be related to the two arrangements of the unpaired electron on each copper(I1) nucleus shown in Figure 1. Measurements have been made on systems having both types of arrangements; however, the parallel configuration of spins is relatively rare in copper(I1) dimers (6-9). Copper(I1) dimers containing brideine erouos . like the alkanoates or Schiff bases orovide a rather constant and similar type of orbital overladbetween the copper(I1) nuclei which is not influenced to any great extent by substituents with the result that within a particular series the magnitudes of the spin exchanges are very similar (2). Consequently, these types of copper(I1) dimers would not be very appealing experimentally to the students. A series of copper(I1) dimers that has been used with great success in both an undergraduate honors course and a graduate laboratory experiment are the halogen-bridged, copper(I1) guaninium dimers having the general formula: (Cu(guaninium)X&mH20, where X = CI, n = 2 and 0; X = Br, n = 0; X = F, n = 2; and guaninium is the protonated form of guanine, Figure 2. These complexes are prepared in virtually pure form and in a simple fashion (10, 11) and have been characterized spectroscopically (10-12). The hydrated, chlorobridged complex, shown in Figure 3 (13), will be the dimeric compound used in the magnetic exchange determination. The measurement of 25 is interesting and informative to the student in several ways. I t is an introduction to a field of research which is presently receiving great attention. It allows

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Figure 1.Possible spin coupling of two electronic spins located at two copper(l1) ions in a dimer. (a) triplet ground state, ZJposltive. (b) singlet ground state. ZJ negative.

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form ~ Dof neutral guanine.

Figure 3. Schemalrc of Me monohydrate dimer (13).

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CU

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C

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s m c m of the nichlarnguaniniumcopper(1l)

Volume 57, Number 5, May 1980 / 385

the determination of the nature of the dimeric ground state as well as the measurement of the strength of the interaction between the metal centers-the prim& objectives of the experiment. T h e student also has a means of checking his preparative techniques since monomeric impurities will yield lower values of W. In addition, the student is intrigued by the thought of working with a complex that contains a nucleic acid residue. Since euanine is a maior constituent of DNA. and since (:opper(ll)has been shown to have a pronounced effect on the rwersil~lcunwindine" of DNA 114-17). .. exnerimentine . with a coordination compound of copper(I1) containing a nncleic acid base invariablv eenerates aueries as to the role copper(ll) plays in the trn&kssion of &tic infnrmation. And, lastlv, this comolex contains a guanine ligand - having- a positive charge (13)-a relatively rare phenomenon in coordination chemistry. Experimental Synthesis

The stable, trichloroguaniniumcopper(I1)monohydrate dimer is synthesized according to methods previously outlined (10-12). A fourfold excess of CuC1~2Hz0(1.36 g) is dissolved in aqueous HC1 (2 M) with the formation of a light yellow solution. To this, guanine is added (0.3g) and themixturevigorouslystirred with heat untilall the guanine dissolves. Concentrated HC1 is added until the solution chances t o a dark green culor and then iq rvnpornted down LO m e third the volume 1211mil. lipon r d i n ~yellow , bnwn rryztnls appear whwh ran he ensdy f~ltered, m p 21It- 51r0 dec 1. Variable Temperature Bulk Magnetic Susceptibility Measurements The magnetic susceptibilitymeasurements can be obtained in the range 77*-3009K (18) using a Faraday balance setup and

HgCdSCN). as the standard (19). The most accurate values of W are obtained, however, from measurements made between 80' and 120°K.The Faraday setup used in our labratory is essentially that described by Busch et al(20) except that the BASF catalyst tower, drying tower, cryostat elevator, liquid nitrogen leveling device, and recorders are not utilized. Our eryostat (Air Products, PA) is permanently mounted on a horizontal arm and the electromagnet (Alpha Scientific, 4 in. water-cooled, adjustable-gap) is placed on a trolley and track. This placement allows in-field and out-of-field measurements to be performed inan easy fashion at magnetic fieldsof about 6000 G. Measurements made out-of-fieldare accompanied by shutdown of magnet power to assure zero magnetic field. The sample sunoort . used is a 50-50ouartz nvlon fiber as described bv Nelson and Villa (21 I. Snmplerizcsrnnge horn lII-.i~)mg andare intnduced into specially made l-icanlun ('I,.. ('A,, high purir). quarts buckets ~h X ;