Journal of the Society of Motion Picture and Television Engineers (1950-1954)

Record Details:

Something wrong or inaccurate about this page? Let us Know!

Thanks for helping us continually improve the quality of the Lantern search engine for all of our users! We have millions of scanned pages, so user reports are incredibly helpful for us to identify places where we can improve and update the metadata.

Please describe the issue below, and click "Submit" to send your comments to our team! If you'd prefer, you can also send us an email to mhdl@commarts.wisc.edu with your comments.




We use Optical Character Recognition (OCR) during our scanning and processing workflow to make the content of each page searchable. You can view the automatically generated text below as well as copy and paste individual pieces of text to quote in your own work.

Text recognition is never 100% accurate. Many parts of the scanned page may not be reflected in the OCR text output, including: images, page layout, certain fonts or handwriting.

Variation of voltage Vc across spor* .condenser ond -Q-rLrL grid volttt3«Vqi of control .tube Fig. 28. Circuit diagram of spark generator for cinematography at 50,000 frames/sec. C across the spark-gap S. The charging current is controlled by transmitter tube TI in such a manner that it is interrupted during the time interval /i/a preceding the spark breakdown, during which the voltage across S remains constant and equal to Vi. Thus the spark-gap breakdown voltage Vz should be between Vi and the voltage V across K, initially 10 kv. Tube TI is itself controlled by receiver tube T2, whose grid voltage is derived from the spark condenser voltage by means of a potentiometer and a bias battery. Just after the spark breakdown, TI is conducting while T2 is cut off. The spark condenser voltage and, hence, the grid voltage of T2, then increase exponentially. When T2 starts drawing plate current, the grid voltage of TI begins to decrease, until time ti when TI is completely cut off and the charging current is interrupted. From then on, the voltage across C remains constant until a rectangular pulse is applied to the grid of TI at time /2. Charging of C is then resumed until time t3, when breakdown occurs. The voltage across C is again at zero at time t\, when the circuit is ready to repeat the same cycle of operation. The periodic pulses applied to the grid of TI are produced by a variablefrequency pulse generator exterior to the spark generator proper. Figure 29 shows the spark generator with the cover removed. The above circuit makes it possible to reach a rate of 50,000 sparks/sec in air without any air-blast. The images are recorded by means of the rotating-mirror camera shown in Fig. 30, with the optical setup of Fig. 31. The fixed rim of this camera holds about 2.5 m of standard 35mm film. At the maximum mirror speed of 20,000 rpm, about 200 circular images 10 mm in diameter may be recorded at the rate of 50,000 frames/sec. Figure 32 shows a portion of a typical record of the impact failure of a standard European notched Fayolle and Naslin: High-Speed Photography