1
ger RNA from that carrying the mdx4cv mutation. As shown in Fig. 1b, c, a 58 primer specific to the wild-type sequence allowed amplification of a 240-base-pair fragment encompassing exons 53 and 54 of mRNA extracted from muscle tissue of con- trol C57Bl/6 and all transplanted animals, but not from mRNA from mock-transplanted mdx4cv mice. All PCR reactions were internally normalized by simultaneous amplification of a 378-base- pair fragment encompassing exons 33–36. Our results indicate that repair by bone- marrow-derived cells never exceeds 1% of total muscle fibres during the lifespan of transplanted mdx mice. Transplantation of total bone marrow, or even of highly enriched stem-cell fractions from bone marrow 2 , therefore has a very limited impact on muscle-cell replacement, and no amelio- rating effect on murine muscular dystrophy. This might be explained by poor recruitment of bone-marrow cells to the dystrophic mus- cle, or by bone-marrow-derived cells having no selective advantage over resident myo- genic precursors, which regenerate muscle throughout life in mdx mice. We do not address strategies for over- coming these limitations here, although they are likely to be the focus of future research. It should be stressed that the mdx mouse model does not reproduce the clinical picture of Duchenne’s muscular dystrophy in humans, in which muscle degeneration gives rise to fibrosis rather than to repair 5 , so it remains possible that dystrophin-producing cells derived from bone marrow might be subject to positive selection in a human context. Giuliana Ferrari*, Anna Stornaiuolo†, Fulvio Mavilio*‡ *H. San Raffaele-Telethon Institute for Gene Therapy, and GenEra SpA, Via Olgettina 58, 20132 Milano, Italy e-mail: [email protected] Department of Biomedical Sciences, University of Modena School of Medicine, 41100 Modena, Italy 1. Ferrari, G. et al. Science 279, 1528–1530 (1998). 2. Gussoni, E. et al. Nature 401, 390–394 (1999). 3. Bittner, R. E. et al. Anat. Embryol. 199, 391–396 (1999). 4. Danko, I. et al. Pediatr. Res. 32, 128–131 (1992). 5. Emery, A. E. H. Duchenne Muscular Dystrophy 2nd edn (Oxford Univ. Press, Oxford, 1993). Microclimate Formation of ozone by fireworks O zone is a secondary pollutant and greenhouse gas that is formed from molecular oxygen in the presence of sunlight and nitrogen oxides. The extent of production also depends on the presence of volatile hydrocarbons, carbon monoxide and methane 1–6 . But we have discovered a surprising source of ozone which is gen- erated in spontaneous bursts even in the absence of sunlight and nitrogen oxides — namely, the exuberant mass of colour- emitting sparklers that are lit during the Diwali festivities, which take place every year during October and November in Delhi, India. The underlying process of ozone formation resembles that induced by ultraviolet radiation in the stratosphere 7,8 . We undertook a routine, real-time monitoring of the concentrations of NO x (NO and NO 2 ), O 3 and other microclimatic factors at a known pollutant-receptor site 9 in Delhi in order to determine the effects of burning unprecedented numbers of fire- works on the local environment during the festive period in November 1999. We found that during the festival period the ozone concentration peaked at around noon and fell to negligible levels after sunset. On Diwali night (7 November), a small build-up of O 3 (951 parts per billion by volume) was detected between 20:40 and 02:30 hours (results not shown). During this period, no correlation was found between NO x concentration and O 3 forma- tion, indicating that the ozone was unlikely to have been generated in reactions involv- ing ambient NO x . This observation was sur- prisingly different from night-time O 3 measurements obtained on the other dates, when no O 3 formation was detected. Further experiments carried out under different climatic conditions showed that there is a linear regression between the total amount of inflammable material present in sparklers and the cumulative O 3 formed (correlation, 0.993). There was no change in ambient NO x concentration before, brief communications NATURE | VOL 411 | 28 JUNE 2001 | www.nature.com 1015 during or after these experiments (Fig. 1). Sparklers depend on a combination of different metal salts to generate their colour and sparkle 10 — these include potassium perchlorate, sulphur, strontium nitrate, bar- ium nitrate, sodium oxalate, calomel, alu- minium and manganese. When burnt, a significant proportion of the light emitted by these constituents has a wavelength below 240 nm (ref. 11). The radiative ener- gy of these emissions is sufficient to dissoci- ate atmospheric molecular oxygen into atomic oxygen, enabling the reaction O 2 &OO 3 to take place. This proposed mechanism could explain the formation of bursts of O 3 without the participation of NO x , and is therefore similar to the process of ultraviolet-radiation-induced formation of O 3 in the stratosphere 7,8 . Arun K. Attri, Ujjwal Kumar, V. K. Jain School of Environmental Sciences, Jawaharlal Nehru University, New Delhi 110 067, India e-mail: [email protected] 1. Ramanathan, V., Singh, H. B., Ciceron, R. J. & Kiehl, J. T. J. Geophys. Res. 90, 5547–5566 (1985). 2. Lacis, A. A., Weubbles, D. J. & Logan, J. A. J. Geophys. Res. 95, 9971–9981 (1990). 3. Wang, W. C. & Sze, N. D. Nature 286, 589–590 (1980). 4. Crutzen, P. J. & Zimmermann, P. H. Tellus 43A–B, 136–151(1991). 5. Walcek, C. J. & Yuan, H.-H. J. Appl. Meteorol. 34, 1056–1069 (1995). 6. Johnson, D. W. et al. Nature 353, 617–621 (1991). 7. Chapman, S. R. Meteorol. Soc. Mem. 3, 103–125 (1930). 8. Brausser, G. P. et al. J. Geophys. Res. 95, 5639–5655 (1990). 9. Singh, A. et al. Atmos. Environ. 31, 3421–3427 (1997). 10. Holmes, H. H. in The Encyclopedia Americana Int. edn, Vol. 11, 263–265 (American Corp., New York, 1983). 11.Reader, J. & Corliss, C. H. in CRC Handbook of Chemistry and Physics 63rd edn (eds Weast, R. C. & Astle, M. J.) E205–E368 (CRC, Florida, 1982–83). Figure 1 Ambient concen- tration (parts per billion by volume) of O 3 (red circles), NO (green) and NO 2 (blue) in the environment as a func- tion of time after lighting colour-emitting ‘pencil’ sparklers. a–d, Values correspond to the simulta- neous burning of one, three, four and six sparklers, respectively; vertical black lines indicate the duration of burning for the sparklers (starting at 0 s). O 3 begins to accumulate in each case at around 100 s; this time lag corresponds to the volume of air in the assembly of the Teflon tube and manifold attached to the O 3 and NO x analysers. During the exper- iments, the open end of the Teflon tube leading to the analysers was kept 900 cm away from the sparklers. The average weight of inflammable material (initial weight minus weight after burning) was 9.1550.85 g per sparkler. The burn time varied from 26 s for one sparkler to a maximum of 42 s for six; this variation was due to differences in the weight of the burning mixture. O 3 formation was independent of microclimatic factors such as temperature and humidity of the ambient air. The concentrations of NO and NO 2 did not change during the O 3 burst. Further details are available from the authors. 25 15 5 –5 595 395 195 –5 1,995 1,495 995 495 –5 1,195 995 795 595 395 195 –5 0 100 200 300 400 500 0 100 200 300 400 500 Time (s) Concentration (p.p.b.v.) a b c d O 3 O 3 O 3 O 3 NO 2 NO Concentration (p.p.b.v.) Time (s) © 2001 Macmillan Magazines Ltd

document

  • Upload
    v-k

  • View
    212

  • Download
    0

Embed Size (px)

Citation preview

ger RNA from that carrying the mdx4cvmutation. As shown in Fig. 1b, c, a 58primer specific to the wild-type sequenceallowed amplification of a 240-base-pairfragment encompassing exons 53 and 54 ofmRNA extracted from muscle tissue of con-trol C57Bl/6 and all transplanted animals, but not from mRNA from mock-transplanted mdx4cv mice. All PCRreactions were internally normalized bysimultaneous amplification of a 378-base-pair fragment encompassing exons 33–36.

Our results indicate that repair by bone-marrow-derived cells never exceeds 1% oftotal muscle fibres during the lifespan oftransplanted mdx mice. Transplantation oftotal bone marrow, or even of highlyenriched stem-cell fractions from bone marrow2, therefore has a very limited impacton muscle-cell replacement, and no amelio-rating effect on murine muscular dystrophy.This might be explained by poor recruitmentof bone-marrow cells to the dystrophic mus-cle, or by bone-marrow-derived cells havingno selective advantage over resident myo-genic precursors, which regenerate muscle throughout life in mdx mice.

We do not address strategies for over-coming these limitations here, althoughthey are likely to be the focus of futureresearch. It should be stressed that the mdxmouse model does not reproduce the clinical picture of Duchenne’s musculardystrophy in humans, in which muscledegeneration gives rise to fibrosis ratherthan to repair5, so it remains possible thatdystrophin-producing cells derived frombone marrow might be subject to positiveselection in a human context.Giuliana Ferrari*, Anna Stornaiuolo†,Fulvio Mavilio*‡*H. San Raffaele-Telethon Institute for GeneTherapy, and †GenEra SpA, Via Olgettina 58,20132 Milano, Italye-mail: [email protected]‡Department of Biomedical Sciences, University ofModena School of Medicine, 41100 Modena, Italy1. Ferrari, G. et al. Science 279, 1528–1530 (1998).

2. Gussoni, E. et al. Nature 401, 390–394 (1999).

3. Bittner, R. E. et al. Anat. Embryol. 199, 391–396 (1999).

4. Danko, I. et al. Pediatr. Res. 32, 128–131 (1992).

5. Emery, A. E. H. Duchenne Muscular Dystrophy 2nd edn (Oxford

Univ. Press, Oxford, 1993).

Microclimate

Formation of ozone by fireworks

Ozone is a secondary pollutant andgreenhouse gas that is formed frommolecular oxygen in the presence of

sunlight and nitrogen oxides. The extent ofproduction also depends on the presence ofvolatile hydrocarbons, carbon monoxideand methane1–6. But we have discovered asurprising source of ozone which is gen-erated in spontaneous bursts even in the

absence of sunlight and nitrogen oxides —namely, the exuberant mass of colour-emitting sparklers that are lit during theDiwali festivities, which take place everyyear during October and November inDelhi, India. The underlying process ofozone formation resembles that induced byultraviolet radiation in the stratosphere7,8.

We undertook a routine, real-time monitoring of the concentrations of NOx

(NO and NO2), O3 and other microclimaticfactors at a known pollutant-receptor site9

in Delhi in order to determine the effects ofburning unprecedented numbers of fire-works on the local environment during thefestive period in November 1999. We foundthat during the festival period the ozoneconcentration peaked at around noon andfell to negligible levels after sunset.

On Diwali night (7 November), a smallbuild-up of O3 (951 parts per billion byvolume) was detected between 20:40 and02:30 hours (results not shown). Duringthis period, no correlation was foundbetween NOx concentration and O3 forma-tion, indicating that the ozone was unlikelyto have been generated in reactions involv-ing ambient NOx. This observation was sur-prisingly different from night-time O3

measurements obtained on the other dates,when no O3 formation was detected.

Further experiments carried out underdifferent climatic conditions showed thatthere is a linear regression between the totalamount of inflammable material present insparklers and the cumulative O3 formed(correlation, 0.993). There was no changein ambient NOx concentration before,

brief communications

NATURE | VOL 411 | 28 JUNE 2001 | www.nature.com 1015

during or after these experiments (Fig. 1).Sparklers depend on a combination of

different metal salts to generate their colourand sparkle10 — these include potassiumperchlorate, sulphur, strontium nitrate, bar-ium nitrate, sodium oxalate, calomel, alu-minium and manganese. When burnt, asignificant proportion of the light emittedby these constituents has a wavelengthbelow 240 nm (ref. 11). The radiative ener-gy of these emissions is sufficient to dissoci-ate atmospheric molecular oxygen intoatomic oxygen, enabling the reactionO2&O→O3 to take place. This proposedmechanism could explain the formation ofbursts of O3 without the participation ofNOx, and is therefore similar to the processof ultraviolet-radiation-induced formationof O3 in the stratosphere7,8.Arun K. Attri, Ujjwal Kumar, V. K. JainSchool of Environmental Sciences, JawaharlalNehru University, New Delhi 110 067, Indiae-mail: [email protected]

1. Ramanathan, V., Singh, H. B., Ciceron, R. J. & Kiehl, J. T.

J. Geophys. Res. 90, 5547–5566 (1985).

2. Lacis, A. A., Weubbles, D. J. & Logan, J. A. J. Geophys. Res. 95,

9971–9981 (1990).

3. Wang, W. C. & Sze, N. D. Nature 286, 589–590 (1980).

4. Crutzen, P. J. & Zimmermann, P. H. Tellus 43A–B,

136–151(1991).

5. Walcek, C. J. & Yuan, H.-H. J. Appl. Meteorol. 34,

1056–1069 (1995).

6. Johnson, D. W. et al. Nature 353, 617–621 (1991).

7. Chapman, S. R. Meteorol. Soc. Mem. 3, 103–125 (1930).

8. Brausser, G. P. et al. J. Geophys. Res. 95, 5639–5655 (1990).

9. Singh, A. et al. Atmos. Environ. 31, 3421–3427 (1997).

10.Holmes, H. H. in The Encyclopedia Americana Int. edn, Vol. 11,

263–265 (American Corp., New York, 1983).

11.Reader, J. & Corliss, C. H. in CRC Handbook of Chemistry and

Physics 63rd edn (eds Weast, R. C. & Astle, M. J.) E205–E368

(CRC, Florida, 1982–83).

Figure 1 Ambient concen-

tration (parts per billion by

volume) of O3 (red circles),

NO (green) and NO2 (blue) in

the environment as a func-

tion of time after lighting

colour-emitting ‘pencil’

sparklers. a–d, Values

correspond to the simulta-

neous burning of one, three,

four and six sparklers,

respectively; vertical black

lines indicate the duration of

burning for the sparklers

(starting at 0 s). O3 begins to

accumulate in each case at

around 100 s; this time lag

corresponds to the volume

of air in the assembly of the

Teflon tube and manifold

attached to the O3 and NOx

analysers. During the exper-

iments, the open end of the

Teflon tube leading to the analysers was kept 900 cm away from the sparklers. The average weight of inflammable material (initial weight

minus weight after burning) was 9.1550.85 g per sparkler. The burn time varied from 26 s for one sparkler to a maximum of 42 s for

six; this variation was due to differences in the weight of the burning mixture. O3 formation was independent of microclimatic factors such

as temperature and humidity of the ambient air. The concentrations of NO and NO2 did not change during the O3 burst. Further details are

available from the authors.

25

15

5

–5

595

395

195

–5

1,995

1,495

995

495

–5

1,195

995

795

595

395

195

–50 100 200 300 400 500 0 100 200 300 400 500

Time (s)

Con

cent

ratio

n (p

.p.b

.v.)

a b

c d

O3 O3

O3 O3

NO2

NO

Con

cent

ratio

n (p

.p.b

.v.)

Time (s)

© 2001 Macmillan Magazines Ltd