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![The thermionic vacuum tube and its applications . uation (22)becomes: en= fp^^Q and the voltage amphfication is therefore (2C.) It must be noted that eg is the a-c. potential difference actuallyestablished The thermionic vacuum tube and its applications . uation (22)becomes: en= fp^^Q and the voltage amphfication is therefore (2C.) It must be noted that eg is the a-c. potential difference actuallyestablished](https://c8.alamy.com/comp/2CE5Y86/the-thermionic-vacuum-tube-and-its-applications-uation-22becomes-en=-fpq-and-the-voltage-amphfication-is-therefore-2c-it-must-be-noted-that-eg-is-the-a-c-potential-difference-actuallyestablished-between-filament-and-grid-it-will-be-seen-that-jx-increases-as-zo-is-increased-and-a-ymptot-ically-approaches-the-maxi-mum-value-at-when-zo-becomesinfinitely-large-compared-withtp-the-constant-which-de-pends-on-the-structure-ofthe-tube-and-determines-thestray-field-is-therefore-simplythe-maximum-voltage-amph-fication-obtainable-from-thetube-when-a-tube-is-to-beused-as-a-voltage-ampli-2CE5Y86.jpg)