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Y-Y. Noh, N. Zhao, M. Caironi and H. Sirringhaus, Nature Nanotechnology, 2007, 2, 12, 784. 9. R. Small and M. in het Panhuis, Small, 2007, 3, 9, 1500. 10. P. G. J. I. Milne, A. A. Gardner, E. G. Steinke, Organic Electronics, 2001, 2, 2, 65. 11. T. Kawase, S. J. Newsome and T. Shimoda, Japanese Journal of Applied Physics, 2005, 44, 1, 6A, 3649. 12. T. Someya, Y. Kato, T. Sekitani, S. Iba, Y. Nguchi, Y. Murase, H. Kawaguchi and T. Sakurai, Proceedings of the National Academy of Sciences, 2005, 102, 35, 12321.

4 ml/h, tpulse = 100 μs. Drop formation and break up were predicted at about 50 μm distance from the nozzle. The falling droplet grew and evolved to a cap. The experimental case study showed many similarities, including the droplet break up time of about 123 μs, which agrees very well with the predictions. However, the predicted travelled distance is smaller than in the experiment. This is attributed to the fact that the experiment is not under constant flow rate during the pulse. As a result, the computer model needs modifications to account for a pressure waveform at inlet.

5. Z. Liu, Y. Su and K. Varahramyan, Thin Solid Films, 2005, 478, 275. 6. S. Sapp, S. B. Losowi, P. L. N. Caruzo, Applied Physics Letters, 2006, 88, 15. 7. Ginley, Journal of Undergraduate Research, 2005, 5, 24. 8. J. Ouyanga, Q. -W Chua, Y. Yanga, G. Lib and J. Shinarb, Polymer, 2004, 45, 8443. 9. A-S Yang, C-H Cheng and C-T Lin in Proceedings of the Institute of Mechanical Engineering Part C: Journal of Mechanical Engineering Science, 2006, 220, 4, 435. 10. M. Jonsson, J. Brigerson and X. Chrispin, Synthetic Metals, 2003, 139, 1.

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