Nation projector carbons (1935)

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.

National Projector Carbons carbons are clamped near the holder end and neither is rotated. It is therefore necessary to increase the conductance of the electrode by coating it with metal, which in this case is copper. The copper does not enter the arc stream, its main function being to furnish a low-resistance path for the current from the carbon holder to a point near the arc. It also protects the carbon from oxidation. Figures 60 to 65 illustrate the performance of the A.C. high-intensity arc under different operating conditions. These illustrations are all traced from actual arc images and show the true relationship between the different elements of the arc. If the current is too great, the copper will melt to a considerable distance from the arc, as shown in Figure 60. The arc then becomes unsteady and is apt to blow out. Also, the arc voltage and consumption of the carbons are increased to such an extent that they may be outside the range of control of the arc-feeding mechanism. If, on the other hand, the current is too low, the copper will not melt away as far from the arc, the light will be very much reduced, and the current and voltage will not be constant. This condition results in an unsteady arc, which "flops" from the top to the bottom of the carbon, as illustrated in Figure 61. If the recommended current and voltage limits are observed neither of these undesirable conditions will be encountered. Figure 60 8 mm A.c. High Intensity Carbons, Overloaded: 90 Amperes, 35 Volts 76