A.U and G.C base pairs in synthetic RNAS have characteristic vacuum UV CD bands.

The vacuum UV CD spectra of GpC, CpG, GpG, poly[r(A)], poly[r(C)], poly[r(U)], poly[r(A-U)], poly[r(G).r(C)], poly[r(A).r(U)], and poly[r(A-U).r(A-U)] were measured down to at least 174 nm. These spectra, together with the published spectra of poly[r(G-C).r(G-C)], CMP, and GMP, were sufficient to estimate the CD changes upon base pairing for four double-stranded RNAs. The vacuum UV CD bands of poly[r(A)], poly[r(C)], and the dinucleotides GpC and CpG were temperature dependent, suggesting that they were due to intrastrand base stacking. The dinucleotide sequence isomers GpC and CpG had very different vacuum UV CD bands, indicating that the sequence can play a role in the vacuum UV CD of single-stranded RNA. The vacuum UV CD bands of the double-stranded (G.C)-containing RNAs, poly[r(G).r(C)] and poly[r(G-C).r(G-C)], were larger than the measured or estimated vacuum UV CD bands of their constituent single-stranded RNAs and were similar in having an exceptionally large positive band at about 185 nm and negative bands near 176 and 209 nm. These similarities were enhanced in difference-CD spectra, obtained by subtracting the CD spectra of the single strands from the CD spectra of the corresponding double strands. The (A.U)-containing double-stranded RNAs poly[r(A).r(U)] and poly[r(A-U).r(A-U)] were similar only in that their vacuum UV CD spectra had a large positive band at 177 nm. The spectrum of poly[r(A).r(U)] had a shoulder at 188 nm and a negative band at 206 nm, whereas the spectrum of poly[r(A-U).r(A-U)] had a positive band at 201 nm. On the other hand, difference spectra of both of the (A.U)-containing polymers had positive bands at about 177 and 201 nm. Thus, the difference-CD spectra revealed CD bands characteristic of A.U and G.C base pairing. (ABSTRACT TRUNCATED AT 250 WORDS)     

Mercury-induced transitions between right-handed and putative left-handed forms of poly[d(A-T).d(A-T)] and poly[d(G-C).d(G-C)]

Poly[d(A-T).d(A-T)] and poly[d(G-C).d(G-C)], each dissolved in 0.1 M NaClO4, 5 mM cacodylic acid buffer, pH 6.8, experience inversion of their circular dichroism (CD) spectrum subsequent to the addition of Hg(ClO4)2. Let r identical to [Hg(ClO4)2]added/[DNA-P]. The spectrum of the right-handed form of poly[d(A-T).d(A-T)] turns into that of a seemingly left-handed structure at r greater than or equal to 0.05 while a similar transition is noted with poly[d(G-C).(G-C)] at r greater than or equal to 0.12. The spectral changes are highly cooperative in the long-wavelength region above 250 nm. At r = 1.0, the spectra of the two polymers are more or less mirror images of their CD at r = 0. While most CD bands experience red-shifts upon the addition of Hg(ClO4)2, there are some that are blue-shifted. The CD changes are totally reversible when Hg(II) is removed from the nucleic acids by the addition of a strong complexing agent such as NaCN. This demonstrates that mercury keeps all base pairs in register.     

Interaction of transition metal ions with Z form poly d(A-C).poly d(G-T) and poly d(A-T) studied by I.R. spectroscopy.

Interactions between Ni2+, Co2+ and purine bases have been studied by I.R. spectroscopy in the case of double stranded regularly alternating purine-pyrimidine polynucleotides poly d(A-T), poly d(A-C).poly d(G-T) and poly d(G-C). The spectra of polynucleotide films have been recorded in hydration and salt content conditions which correspond to the obtention of the classical right-handed (A,B) and left-handed (Z) helical conformations. Selective deuteration of the 8C site of purines has been obtained and is used to detect interactions between the transition metal ions and the adenine or guanine bases. The spectral region between 1500 and 1250 cm-1 corresponding to base in-plane vibrations and involving also the glycosidic linkage torsion is discussed in detail. The selective interaction between the transition metal ion and the 7N site of the purine base is considered to be partly responsible for the stabilization of the base in a syn conformation, which favours the adoption by the polynucleotide (poly d(G-C), poly d(A-C).poly d(G-T) or poly d(A-T)) of a Z type conformation.     

Sequence-dependant polymorphism of DNA duplex in solutions

Raman spectra of six synthetic polydeoxyribonucleotide duplexes with different base sequences have been examined in aqueous solutions with different salt or nucleotide concentrations. Detailed conformational differences have been indicated between B and Z forms of poly[d(G-C)] X poly[d(G-C)], between B forms of poly[d(G-C)] X poly[d(G-C)] and poly[d(G-m5C)] X poly[d(G-m5C)], between A and B forms of poly(dG) X poly(dC), between B and "CsF" forms of poly[d(A-T)] X poly[d(A-T)], between B forms of poly[d(A-U)] X poly[d(A-U)] and poly[d(A-T)] X poly[d(A-T)], and between low- and high-salt (CsF) forms of poly(dA) X poly(dT). The Raman spectrum of calf-thymus DNA in aqueous solution was also observed and was compared with the Raman spectra of its fibers in A, B, and C forms.     

Evidence for Z-form RNA by vacuum UV circular dichroism.

Circular dichroism (CD) spectra in the vacuum UV region for different conformations of poly d(G-C) X poly d(G-C) and poly r(G-C) X poly r(G-C) are very characteristic. The CD of the RNA in the A-form (6 M NaClO4 and 22 degrees C) is very similar to that of the DNA in 80% alcohol where it is believed to be in the A-form. With the exception of the longest wavelength transition, the CD of the RNA in 6 M NaClO4 at 46 degrees C is similar to the CD of the DNA under conditions where it is believed to be in the Z-form (2 M NaClO4). This substantiates that poly r(G-C) X poly r(G-C) assumes a left-handed Z-conformation in 6 M NaClO4 above 35 degrees C. CD spectra for the left-handed Z-forms of both the RNA and DNA are characterized by an intense negative peak at 190-195 nm, a crossover at about 184 nm, and an intense positive peak below 180 nm. The right-handed A- and B-forms of RNA and DNA all have an intense positive peak in their CD spectra near 186 nm. The large difference in CD in the range 185-195 nm for right- and left-handed conformations of nucleic acids can be used to identify the sense of helix winding.     

Raison d'être and structural model for the B-Z transition of poly d(G-C).poly d(G-C)

In DNA oligonucleotides crystallized in the A form, the nucleotides adopt standard conformation except for steps 5'-CpG-3' where reduced base-pair twist and a sliding motion of the base pairs along their long axes causes pronounced interstrand guanine-guanine overlap. As a consequence, torsion angles alpha, beta and gamma are consistently trans, trans, trans instead of the common-gauche, trans, +gauche. This conformation significantly increases the intraresidue distance between the guanine base and the 5'-phosphate group. A molecular model of poly d(G-C).poly d(G-C) built with these structural characteristics in the A form, which we call A2-DNA, shows that rotation of the guanosine sugar into the syn orientation is easily achieved and pushes the base pair across the helix axis. If successive guanosines are changed this way, a smooth transformation occurs to the left-handed Z-DNA. We suggest that A- and A2-DNA forms of poly d(G-C).poly d(G-C) are metastable and that the actual transition is B in equilibrium (A in equilibrium A2) in equilibrium Z-DNA.     

Thermodynamics of left-handed helix formation

The thermodynamics of right- and left-handed helix formation by poly[d(G-C)] X poly[d(G-C)] and by poly-(dG-m5dC) X poly(dG-m5dC) were measured spectrophotometrically and calorimetrically. From the spectrophotometric measurements the thermal stabilities of the alternative helical conformations were evaluated as a function of counterion concentration. From the calorimetric measurements the enthalpies of either right-handed or left-handed helix formation were determined. The corresponding experimental delta H values are -8.6 and -11.2 kcal/mol base pairs for the two conformations in poly[dG-C)] X poly[d(G-C)], and -9.0 and -12.7 kcal/mol base pairs, respectively, for poly(dG-m5dC) X poly(dG-m5dC).     

Secondary structure of ovalbumin messenger RNA.

The secondary structure of highly purified ovalbumin mRNA was studied by automated thermal denaturation techniques and the data were subjected to computer processing. Comparative studies with 20 natural and synthetic model nucleic acids suggested that the secondary structure of ovalbumin mRNA possesses the following features: the extent of base pairing of ovalbumin mRNA is similar to that found in tRNAs or ribosomal RNAs; the secondary structure of ovalbumin mRNA is more thermolabile than any of the model compounds tested, including the copolymer poly(A-U); ovalbumin mRNA does not have extensive G-C rich stems as found in tRNAs or ribosomal RNAs; the base composition of the double-stranded regions reveals 54% G-C residues which was significantly higher than that noted in the whole molecule (approximately 41.5% G-C). The presence of 46% A-U pairs in short stems of about five base pairs would have a very large destabilizing effect on the secondary structure of ovalbumin mRNA. However, at 0.175 M monovalent cations and 36 degrees C most of the secondary structure of ovalbumin mRNA is preserved. These data suggest that the double-stranded regions in ovalbumin mRNA are of sufficient length to provide the necessary stability for maintaining the open loop regions in an appropriate conformation which may be required for the biological function of ovalbumin mRNA. Furthermore, the lability of the double-stranded regions in ovalbumin mRNA may also be important for the biological function of this mRNA.     

Thermodynamics of nucleic acid "shape readout" by an aminosugar

Recognition of nucleic acids is important for our understanding of nucleic acid structure as well as for our understanding of nucleic acid-protein interactions. In addition to the direct readout mechanisms of nucleic acids such as H-bonding, shape recognition of nucleic acids is being increasingly recognized as playing an equally important role in DNA recognition. Competition dialysis, UV, flourescent intercalator displacement (FID), computational docking, and calorimetry studies were conducted to study the interaction of neomycin with a variety of nucleic acid conformations (shapes). At pH 5.5, the results suggest the following. (1) Neomycin binds three RNA structures [16S A site rRNA, poly(rA)·poly(rA), and poly(rA)·poly(rU)] with high affinities (K(a) ~ 10(7) M(-1)). (2) The binding of neomycin to A-form GC-rich oligomer d(A(2)G(15)C(15)T(2))(2) has an affinity comparable to those of RNA structures. (3) The binding of neomycin to DNA·RNA hybrids shows a 3-fold variance that can be attributed to their structural differences [for poly(dA)·poly(rU), K(a) = 9.4 × 10(6) M(-1), and for poly(rA)·poly(dT), K(a) = 3.1 × 10(6) M(-1)]. (4) The interaction of neomycin with DNA triplex poly(dA)·2poly(dT) yields a binding affinity (K(a)) of 2.4 × 10(5) M(-1). (5) Poly(dA-dT)(2) shows the lowest association constant for all nucleic acids studied (K(a) < 10(5)). (6) Neomycin binds to G-quadruplexes with K(a) values of ~10(4)-10(5) M(-1). (7) Computational studies show that the decrease in major groove width in the B to A transition correlates with increasing neomycin affinity. Neomycin's affinity for various nucleic acid structures can be ranked as follows: RNAs and GC-rich d(A(2)G(15)C(15)T(2))(2) structures > poly(dA)·poly(rU) > poly(rA)·poly(dT) > T·A-T triplex, G-quadruplex, B-form AT-rich, or GC-rich DNA sequences. The results illustrate the first example of a small molecule-based "shape readout" of different nucleic acid conformations.     

Determination of base pairing in ribonucleic acid by Fourier-transform infrared spectrometry: yeast ribosomal 5S ribonucleic acid

Fourier-transform infrared (FT-IR) spectra of yeast ribosomal 5S RNA have been acquired at several temperatures between 30 and 90 degrees C. The difference spectrum between 90 (bases unstacked) and 30 degrees C (bases stacked) provides a measure of base stacking in the RNA. Calibration difference spectra corresponding to stacking of G-C or A-U pairs are obtained from "reference" FT-IR spectra of poly(rG) X poly(rC) minus 5'-GMP and 5'-CMP or poly(rA) X poly(rU) minus 5'-AMP and 5'-UMP. The best fit linear combination of the calibration G-C and A-U difference spectra to the 5S RNA (90-30 degrees C) difference spectrum leads to a total of 25 +/- 3 base pairs (17 G-C pairs + 8 A-U pairs) for the native yeast 5S RNA in the absence of Mg2+. In the presence of Mg2+, an additional six base pairs are detected by FT-IR (one G-C and five A-U). FT-IR melting curve midpoints show that A-U and G-C pairs melt together (65 and 63 degrees C) in the presence of Mg2+ but A-U pairs melt before G-C pairs (47 vs. 54 degrees C) in the absence of Mg2+.     

Study of conformation characteristics of polydeoxyribonucleotides with non-random base sequence by slow 1H----3H exchange

The rate constants of 1H----3H exchange between water and C8H-groups of purinic residues of alternating polynucleotides: poly[d(A-T)].poly[d(A-T)] (I), poly[d(G-C)].poly[d(G-C)] (II), poly[d(A-C)].poly[d(G-T)] (III) and homopolynucleotides: poly(dA).poly(dt) (IV), poly(dG).poly(dC) (V), as well as DNA E. coli, was determined in 0.15 M NaCl at 25 degrees C. The retardation of exchange observed at these conditions (compared to that of the B-form DNA) is in agreement with the model of B-alternating structure for the (I) and is attributed to the co-existence of B- and A-conformers for the (V) in solution. Absence of distinguishable differences in exchange rate constants for purinic residues of the (II), (III) and (IV) (compared to that of the B-form DNA) evidences that conformations of these polynucleotides in solution are similar to "canonical" B-form DNA and don't correlate with the model of "heteronomous" DNA which was proposed for (IV).     

Energetics of Z-DNA formation in poly d(A-T), poly d(G-C), and poly d(A-C) poly d(G-T).

The conformational change for the alternating purine-pyrimidine polydeoxyribonucleotides i.e. poly d(A-T), poly d(G-C), and poly d(A-C) poly d(G-T) from a right-handed conformation at room temperature to the left-handed Z-DNA like double helix at elevated temperatures has been studied by UV spectroscopy, Raman spectroscopy, and by adiabatic differential scanning microcalorimetry (DSC) in the presence of Na+ and Mg2+ or Ni2+ respectively as counterions. The differential UV spectra reveal through a hyperchromic shift at around 280nm and a hypochromic shift at 260nm that a conformational change to the left-handed conformation occurs. The Raman spectra clearly show characteristic changes, a drastic decrease of the band at 680cm-1 and the appearance of a new band at 628cm-1, due to the change of the purine bases to the syn conformation upon inversion of the helix-handedness. The course of the transition as function of temperature can be followed quantitatively by plotting the change in the excess heat capacity vs. temperature. The transition enthalpy delta H for the B- to Z-DNA transition per mole base pairs (mbp) amounts to 2.0 +/- 0.2kcal for poly d(G-C), to 4.0 +/- 0.4kcal for poly d(A-T), and to 3.1 +/- 0.3kcal for poly d(A-C) poly d(G-T). The enthalpy change due to the Z-DNA to coil transitions (per mole base pairs) amounts to 11kcal for poly d(G-C), 10.5kcal for poly d(A-T) and 11.3kcal for poly d(A-C) poly d(G-T).     

Determination of secondary structure in rabbit globin messenger RNA by thermal denaturation.

The secondary structure of highly purified globin messenger RNA has been investigated by alkaline hydrolysis, nuclease digestion, and thermal denaturation. The thermal denaturation properties of globin messenger have been compared to poly(U), poly (A), and a synthetic random sequence RNA copolymer. From these studies it is concluded that globin mRNA contains considerable secondary structure and that the amount of helical structure is greater than that which occurs with a random sequence polyribonucleotide. Globin mRNA contains, by comparison to the secondary structures of native DNA, tRNAs, or 18S rRNA, helices with involve 55-62% of the bases or 58-68% if a correction is made for the 3'-terminal poly(A) segment. The helices of globin mRNA appear to be unique as differences in the NaCl stabilization of this RNA have been noted when compared to other naturally ooccurring and synthetic RNAs. Comparison of the hyperchromicity maxima, obtained at 260 and 280 nm for globin mRNA and 18S rRNA, indicates that the helices of the two RNAs contain similar numbers of G-C base pairs. Differential analysis of NaCl stabilization curves indicate three discrete thermally denaturable helix types in globin mRNA.     

Amine group of guanine enhances the binding of norfloxacin antibiotics to DNA.

The binding mode of norfloxacin, a quinolone antibacterial agent, in the synthetic polynucleotides poly[d(G-C)2], poly[d(I-C)2] and poly[d(A-T)2] was studied using polarized light spectroscopy, fluorescence spectroscopy and melting profiles. The absorption, circular and linear dichroism properties of norfloxacin are essentially the same for all the complexes, and the angle of electric transition dipole moment I and II of norfloxacin relative to the DNA helix axis is measured as 68-75 degrees for all complexes. These similarities indicate that the binding mode of norfloxacin is similar for all the polynucleotides. The decrease in the linear dichroism (LD) magnitude at 260 nm upon binding norfloxacin, which is strongest for the norfloxacin-poly[d(G-C)2] complex, and the identical melting temperature of poly[d(A-T)2] and poly[d(I-C)2] in the presence and absence of norfloxacin rule out the possibility of classic intercalation and minor groove binding. However, the characteristics of the fluorescence emission spectra of norfloxacin bound to poly[d(A-T)2] and to poly[d(I-C)2] are similar but are different to that of norfloxacin bound to poly[d(G-C)2]. As the amine group of the guanine base protrudes to the minor groove, this result strongly suggests that norfloxacin binds in the minor groove of B-form DNA in a nonclassic manner.     

The solution structure of d(G(4)T(4)G(3))(2): a bimolecular G-quadruplex with a novel fold

The G-rich 11-mer oligonucleotide d(G(4)T(4)G(3)) forms a bimolecular G-quadruplex in the presence of sodium ions with a topology that is distinct from the folds of the closely related and well-characterized sequences d(G(4)T(4)G(4)) and d(G(3)T(4)G(3)). The solution structure of d(G(4)T(4)G(3))(2) has been determined using a combination of NMR spectroscopy and restrained molecular dynamics calculations. d(G(4)T(4)G(3))(2) forms an asymmetric dimeric fold-back structure consisting of three stacked G-quartets. The two T(4) loops that span diagonally across the outer faces of the G-quartets assume different conformations. The glycosidic torsion angle conformations of the guanine bases are 5'-syn-anti-syn-anti-(T(4) loop)-anti-syn-anti in one strand and 5'-syn-anti-syn-anti-(T(4) loop)-syn-anti-syn in the other strand. The guanine bases of the two outer G-quartets exhibit a clockwise donor-acceptor hydrogen-bonding directionality, while those of the middle G-quartet exhibit the anti-clockwise directionality. The topology of this G-quadruplex, like other bimolecular fold-back structures with diagonal loops, places each strand of the G-quartet region next to a neighboring parallel and an anti-parallel strand. The two guanine residues not involved in G-quartet formation, G4 and G12 (i.e. the fourth guanine base of one strand and the first guanine base of the other strand), adopt distinct conformations. G4 is stacked on top of an adjacent G-quartet, and this base-stacking continues along with the bases of the loop residues T5 and T6. G12 is orientated away from the core of G-quartets; stacked on the T7 base and apparently involved in hydrogen-bonding interactions with the phosphodiester group of this same residue. The cation-dependent folding of the d(G(4)T(4)G(3))(2) quadruplex structure is distinct from that observed for similar sequences. While both d(G(4)T(4)G(4)) and d(G(3)T(4)G(3)) form bimolecular, diagonally looped G-quadruplex structures in the presence of Na(+), K(+) and NH(4)(+), we have observed this folding to be favored for d(G(4)T(4)G(3)) in the presence of Na(+), but not in the presence of K(+) or NH(4)(+). The structure of d(G(4)T(4)G(3))(2) exhibits a "slipped-loop" element that is similar to what has been proposed for structural intermediates in the folding pathway of some G-quadruplexes, and therefore provides support for the feasibility of these proposed transient structures in G-quadruplex formation.     

Reversible helix/coil transitions of left-handed Z-DNA structures. Comparison of the thermodynamic properties of poly(dG).poly(dC), poly[d(G-C)].poly[d(G-C)], and poly(dG-m5dC).poly(dG-m5dC)

In contrast to poly(dG).poly(dC), which remains in the B-DNA conformation under all experimental conditions the polynucleotides with the strictly alternating guanine/cytosine or guanine/5'-methylcytosine sequences can change from the classical right-handed B-DNA structure to the left-handed Z-DNA structure when certain experimental conditions such as ionic strength or solvent composition are fulfilled. Up to now the investigation of the helix/coil transition of left-handed DNA structures was not possible because the transition temperature exceeds 98 degrees C. By applying moderate external pressure to the surface of the aqueous polymer solution in the sample cell the boiling point of the solvent water is shifted up the temperature scale without shifting the transition temperature, so that we can measure the helix/coil transition of the polynucleotides at all experimental conditions applied. It can thus be shown that the Z-DNA/coil transition is cooperative and reversible. The Tm is 125 degrees C for poly(dG-m5dC).poly(dG-m5dC) in 2mM Mg2+, 50mM Na+, pH 7.2 and 115 degrees c for poly[d(G-C)].poly[d(G-C)] in 3.04M Na+. The transition enthalpy per base pair was determined by the help of an adiabatic scanning microcalorimeter.     

Porphyrin and metalloporphyrin binding to DNA polymers: rate and equilibrium binding studies

Interactions of meso-tetrakis(4-N-methylpyridiniumyl)porphyrin [TMpyP(4)] with poly[d(G-C)].poly[d(G-C)] [poly[d(G-C)2] and poly[d(A-T)].poly[d(A-T)] [poly[d(A-T)2] were studied by equilibrium dialysis and stopped-flow dissociation kinetics as a function of [Na+]. Metalloderivatives of TMpyP(4), NiTMpyP(4), and ZnTMpyP(4) were also investigated. The apparent equilibrium binding constants (Kobs) were approximately the same for TMpyP(4) binding to either poly[d(G-C)2] or poly[d(A-T)2] and decreased with increasing [Na+]. The slopes of the plots of log Kobs vs log [Na+] were similar, with values close to -2.7. Contrary to implications in previously reported studies, these data do not indicate that TMpyP(4) prefers to bind to GC sites at low ionic strength and to AT sites at high ionic strength. In contrast, binding of ZnTMpyP(4) to these two polymers is very different. Comparisons of Kobs values at 0.065 M [Na+] indicate that ZnTMpyP(4) binding to AT sites is approximately 200 times more favorable than binding to GC sites, a finding in agreement with previous qualitative observations. Although the binding of the Zn species to the GC polymer was too weak for us to assess the salt effect, the plot of log Kobs vs log [Na+] gave a slope of -2.0 for ZnTMpyP(4) binding to poly[d(A-T)2]. Application of condensation theory for polyelectrolytes suggests similar charge interactions for ZnTMpyP(4) and for TMpyP(4) binding to poly[d(A-T)2]. Likewise, the rates of dissociation from poly[d(A-T)2] were similar for TMpyP(4) and ZnTMpyP(4) [and also NiTMpyP(4)]. However, whereas TMpyP(4) [and NiTMpyP(4)] dissociation from poly[d(G-C)2] was measurable, that for ZnTMpyP(4) was too fast to measure.(ABSTRACT TRUNCATED AT 250 WORDS)     

Cytoplasmic CUG RNA Foci Are Insufficient to Elicit Key DM1 Features

The genetic basis of myotonic dystrophy type I (DM1) is the expansion of a CTG tract located in the 3′ untranslated region of DMPK. Expression of mutant RNAs encoding expanded CUG repeats plays a central role in the development of cardiac disease in DM1. Expanded CUG tracts form both nuclear and cytoplasmic aggregates, yet the relative significance of such aggregates in eliciting DM1 pathology is unclear. To test the pathophysiology of CUG repeat encoding RNAs, we developed and analyzed mice with cardiac-specific expression of a beta-galactosidase cassette in which a (CTG)₄₀₀ repeat tract was positioned 3′ of the termination codon and 5′ of the bovine growth hormone polyadenylation signal. In these animals CUG aggregates form exclusively in the cytoplasm of cardiac cells. A key pathological consequence of expanded CUG repeat RNA expression in DM1 is aberrant RNA splicing. Abnormal splicing results from the functional inactivation of MBNL1, which is hypothesized to occur due to MBNL1 sequestration in CUG foci or from elevated levels of CUG-BP1. We therefore tested the ability of cytoplasmic CUG foci to elicit these changes. Aggregation of CUG RNAs within the cytoplasm results both in Mbnl1 sequestration and in approximately a two fold increase in both nuclear and cytoplasmic Cug-bp1 levels. Significantly, despite these changes RNA splice defects were not observed and functional analysis revealed only subtle cardiac dysfunction, characterized by conduction defects that primarily manifest under anesthesia. Using a human myoblast culture system we show that this transgene, when expressed at similar levels to a second transgene, which encodes expanded CTG tracts and facilitates both nuclear focus formation and aberrant splicing, does not elicit aberrant splicing. Thus the lack of toxicity of cytoplasmic CUG foci does not appear to be a consequence of low expression levels. Our results therefore demonstrate that the cellular location of CUG RNA aggregates is an important variable that influences toxicity and support the hypothesis that small molecules that increase the rate of transport of the mutant DMPK RNA from the nucleus into the cytoplasm may significantly improve DM1 pathology.