Motion picture sound engineering (1938)

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.

508 MOTION PICTURE SOUND ENGINEERING D — £iL • I\P T if where Rp = plate to filament resistance Ep = plate voltage Ip = plate current Figure 357 shows a typical plate voltage-plate current curve for a triode and it will be noticed that the value obtained by dividing the plate voltage by the plate current will vary, depending upon what point on the curve is considered. Since, under operating conditions, we utilize a considerable portion of the curve, it is obvious that the direct-current plate to filament resistance would not necessarily give a true indication of the situation under operating conditions. We, therefore, make use of what is known as the alternatingOutput //npe&vce current plate to filament resistance. By reference to Figure 358 it may be seen that it is determined as follows: P/ate Vo/taye Figure 3 57 — Plate current-plate voltage characteristic of threeelement vacuum tube. of curve to t/?e curre/tf ar/s P/ate l/o/taye Figure 358 — The plate-filament resistance may be determined from the plate voltage-plate current curve. RP = P2 pl IP2 — 1 Pi This is known as the alternating-current plate-filament resistance and is also sometimes called the plate-filament impedance. 9, MUTUAL CONDUCTANCE The conductance of an ordinary direct-current circuit is considered as the reciprocal of the resistance. If we designate the conductance by the lettd G, then In The three-element vacuum tube, however, we are principally interested in The variation in plate current produced by a change of grid voltage rather than by a change of plate voltage. The mutual conductance therefore must equal the plate current divided by the grid voltage rather than the plate current divided by the plate voltage, and if we designate the mutual conductance by the symbol Gm, then