Patent GB-1064151-A (GB)
Title: Improvements in or relating to electrical measuring instruments
Inventor: YOUNG REGINALD SEARLES
IPC: G01B7/06
Filed: 1962-10-11
Abstract: 1, 064,151. Determining physical dimensions, measuring impedance. BRITISH ALUMINIUM CO. Ltd. Oct.10, 1963 [Oct. 11, 1962], No.38575/62. Headings G1N and G1U. Relates to an instrument, for measuring the thickness of a coating or film of electrically non- conducting material on a metal base, or for measuring the resistivity of a metal sample having an investigating coil 14 inductively coupled to an oscillator circuit (Gouriet type) whereby variation of the "Q" of the said coil in proportion to the thickness or resistivity affects the amplitude of oscillation of an oscillator valve and an adjustment to maintain the amplitude constant at a pre-set value is used as a measure of the thickness or resistivity. MEASURING THICKNESS. The instrument is set up to be independent of the resistivity of a coated metal sample by placing the head coil 14 first on a metal base of low resistivity and then on one of high resistivity and adjusting C11, C12 and L2 to give the same selected amplitude indication on a meter 20. The frequency of a tuned circuit L9 C1 1 is made less than that of the oscillator proper (including pentode V1) as determined by a series tuned circuit L2, C3. Any increase in separation of the investigating head (coil 14) from the metal base lowers the tuned frequency of L9, C11 and reduces its losses. These effects are additive and increase the tuned impedance of L2 resulting in a greater amplitude of oscillation as seen by meter 20. The departure from the pre-selected amplitude represents the thickness of the coating. Instead of calibrating the meter to read thickness a capacitor 7 is so calibrated and the amount it has to be adjusted to maintain constant the selected value is a measure of the thickness of the coating. The meter may be replaced by or associated with recording means. MEASURING RESISTIVITY. In this case a transformer secondary winding L9 is interchanged with the variable inductance L2, the tuned circuit now composed of L2, C11 being tuned to a frequency lower than the series circuit now comprising secondary winding L9 and C3. The effect is that as the spacing between coil 14 and the metal, increases, the losses of the series circuit are reduced to approach that of L2, C11 tuned circuit so that more energy is transferred to the latter circuit. The change in energy transferred to the parallel tuned circuit L2, C11 is of opposite sense to the change in energy losses of the series tuned circuit L9, C3 so that these can be made to compensate one another and the instrument made insensitive to the spacing of the coil 14 from the metal sample and hence of coating thickness. At the same time increase in resistivity of the metal sample increases the series circuit losses and reduces the frequency of oscillation thereof so that energy transferred to the parallel tuned circuit also increases. Thus the change in the losses of the series circuit due to change of resistivity of the metal sample is in the same sense as the energy loss due to transfer to the parallel tuned circuit and the amplitude of oscillation is varied accordingly and is a measure of the resistivity of the metal sample. In this embodiment the capacitor 7 may be omitted, and a feedback variable resistor 8 calibrated so that adjustment thereof to maintain constant amplitude provides a measure of the resistivity. A portion of the feedback resistor 8 may be a thermistor to provide temperature compensation.