# US 4,372,173 A · Resonator force transducer > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 4,372,173 A - Document ID: US4372173A - Status: Granted - Kind: A - Application number: 06/198,705 - Filed: 1980-10-20 - Granted: 1983-02-08 - Earliest claimed: 1980-10-20 - Assignees: Quartex, Inc. - Inventors: Errol P. EerNisse; Jerome M. Paros - Web page: https://patentgrep.com/patent/US4372173A ## CPC - G01P 15/097: by vibratory elements - G01L 1/162: {using piezoelectric resonators} - Y10S 73/01: Vibration - Y10S 73/04: Piezoelectric - G01P: MEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT (measuring or recording blood flow A61B5/02, A61B8/06; monitoring speed or deceleration of electrically-propelled vehicles B60L3/00; vehicle lighting systems adapted to indicate speed B60Q1/54; determining position or course in navigation, measuring ground distance in geodesy or surveying G01C; combined measuring devices for measuring two or more variables of movement G01C23/00; measuring velocity of sound G01H; measuring velocity of light G01J7/00; measuring direction or velocity of solid objects by reception or emission of radiowaves or other waves and based on propagation effects, e.g. Doppler effect, propagation time, direction of propagation, G01S; measuring speed of nuclear radiation G01T; measuring acceleration of gravity G01V; {measuring or recording the speed of trains B61L23/00; speed indicators incorporated in motor vehicles B60K35/00; measuring frequency or phase G01R; traffic control G08G}) - G01L: MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE (weighing G01G) - Y10S: TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS ## Abstract A vibratory, force transducer includes a pair of elongate, generally parallel bars coupled together at their ends in a type of double-ended tuning fork arrangement. The bars each have a thickness of t, a width of w and a length between fixed ends of L. The distance separating the points where the bars are coupled together is m. Apparatus is provided to cause the bars to vibrate in a transverse direction and in substantially 180.degree. phase opposition. Apparatus is also provided for determining the frequency of vibration of the bars so that when the bars are subjected to either compressive or tensile forces along the longitudinal axis of the bars, the magnitude of such forces can be readily determined by simply determining the magnitude of the frequency change. The values of w and t are selected so that 0.4<t/w<4, and this reduces the likelihood of buckling the transducer when it is subjected to compressive forces while also maintaining a configuration which is relatively easy to fabricate using a photolithographic process. The values of t, w, L and m are selected so that various spurious modes of oscillation of the transducer, which causes a reduction in the mechanical Q and thus an erroneous reading of applied forces, are avoided. The disclosed selection processes for t, w, and L may be applied also to single beam flexure mode transducers to avoid spurious modes of oscillation while maintaining a configuration which is relatively easy to fabricate using photolithographic processes. ## Claims ### Claim 1 A vibratory force transducer comprising a pair of elongate, generally parallel bars coupled together at their ends and adapted to vibrate 180.degree. out of phase in a transverse direction, said bars each having a thickness t and a width w, the distance between the locations at which the bar ends are coupled together being m and the lengths of the bars being generally L, wherein 0.4<t/w<4, and L/m.gtoreq.1, means for causing said bars to resonate at a frequency f in substantially 180.degree. phase opposition in a transverse direction, said frequency varying with variation in force applied longitudinally to said bars. ### Claim 2 (depends on 1) A transducer as in claim 1 wherein t, w, L, and m are selected so that for any value of S in the range S.sub.min to S.sub.max, where S is the force sensitivity of the transducer, with positive values of S representing tensile forces and negative values representing compressive forces, and S.sub.min and S.sub.max are the minimum and maximum values of S respectively used to define the desired operating range, the following inequality holds: ##EQU11## where F.sub.p1 is the fundamental resonant frequency of the bars in a spurious mode where the bars oscillate in phase in a direction normal to the plane of the bars. ### Claim 3 (depends on 2) A transducer as in claim 2 wherein t, w, L, and m are selected so that: ##EQU12## ### Claim 4 (depends on 2) A transducer as in claim 2 wherein t, w, L, and m are selected so that: ##EQU13## where f.sub.p2 is the second overtone of f.sub.p1. ### Claim 5 (depends on 2) A transducer as in claim 2 wherein t, w, L, and m are selected so that: ##EQU14## where f.sub.p2 is the second overtone of f.sub.p1. ### Claim 6 (depends on 2) A transducer as in claim 2 wherein t, w, L, and m are selected so that: ##EQU15## where f.sub.p3 is the third overtone of f.sub.p1. ### Claim 7 (depends on 2) A transducer as in claim 2 wherein t, w, L and m are selected so that: ##EQU16## where f.sub.p3 is a third overtone of f.sub.p1. ### Claim 8 (depends on 1) A transducer as in claim 1 wherein t, w, L and m are selected so that for any value of S in the range S.sub.min to S.sub.max, where S is the force sensitivity of the transducer, with positive values of S representing tensile forces and negative values representing compressive forces, and S.sub.min and S.sub.max are the minimum and maximum values of S respectively used to define the desired operating range, the following inequality holds: ##EQU17## where f.sub.d is the fundamental resonant frequency of the bars in a spurious mode where the bars oscillate out of phase in a direction normal to the plane of the bars. ### Claim 9 (depends on 8) A transducer as in claim 8 wherein t, w, L and m are selected so that: ##EQU18## ### Claim 10 (depends on 1) A transducer as in claim 1 further including a pair of enlarged end portions to which respective ends of the bars are coupled, said enlarged end portions providing mounting surfaces for mounting the bars to a support structure while also defining L. ### Claim 11 (depends on 1) A transducer as in claim 1 wherein t, w, L, and m are selected so that for any value of S in the range S.sub.min to S.sub.max, where S is the force sensitivity of the transducer, with positive values of S representing tensile forces and negative values representing compressive forces, and S.sub.min and S.sub.max are the minimum and maximum values of S respectively used to define the desired operating range, the following inequality holds: ##EQU19## where f.sub.p1 is the fundamental resonant frequency of the bars in a spurious mode where the bars oscillate in phase in a direction normal to the plane of the bars. ### Claim 12 (depends on 1) A transducer as in claim 1 wherein t, w, L, and m are selected so that for any value of S in the range S.sub.min to S.sub.max, where S is the force sensitivity of the transducer, with positive values of S representing tensile forces and negative values representing compressive forces, and S.sub.min and S.sub.max are the minimum and maximum values of S respectively used to define the desired operating range, the following inequality holds: ##EQU20## where f.sub.p2 is the second overtone of the fundamental resonant frequency of the bars in a spurious mode where the bars oscillate in phase in a direction normal to the plane of the bars. ### Claim 13 (depends on 1) A transducer as in claim 1 wherein t, w, L, and m are selected so that for any value of S in the range S.sub.min to S.sub.max, where S is the force sensitivity of the transducer, with positive values of S representing tensile forces and negative values representing compressive forces, and S.sub.min and S.sub.max are the minimum and maximum values of S respectively used to define the desired operating range, the following inequality holds: ##EQU21## where f.sub.p2 is the second overtone of the fundamental resonant frequency of the bars in a spurious mode where the bars oscillate in phase in a direction normal to the plane of the bars. ### Claim 14 (depends on 1) A transducer as in claim 1 wherein t, w, L, and m are selected so that for any value of S in the range S.sub.min to S.sub.max, where S is the force sensitivity of the transducer, with positive values of S representing tensile forces and negative values representing compressive forces, and S.sub.min and S.sub.max are the minimum and maximum values of S respectively used to define the desired operating range, the following inequality holds: ##EQU22## where f.sub.p3 is the third overtone of the fundamental resonant frequency of the bars in a spurious mode where the bars oscillate in phase in a direction normal to the plane of the bars. ### Claim 15 (depends on 1) A transducer as in claim 1 wherein t, w, L, and m are selected so that for any value of S in the range S.sub.min to S.sub.max, where S is the force sensitivity of the transducer, with positive values of S representing tensile forces and negative values representing compressive forces, and S.sub.min and S.sub.max are the minimum and maximum values of S respectively used to define the desired operating range, the following inequality holds: ##EQU23## where f.sub.p3 is the third overtone of the fundamental resonant frequency of the bars in a spurious mode where the bars oscillate in phase in a direction normal to the plane of the bars. ### Claim 16 (depends on 1) A transducer as in claim 1 wherein t, w, L, and m are selected so that for any value of S in the range S.sub.min to S.sub.max, where S is the force sensitivity of the transducer, with positive values of S representing tensile forces and negative values representing compressive forces, and S.sub.min and S.sub.max are the minimum and maximum values of S respectively used to define the desired operating range, the following inequality holds: ##EQU24## where f.sub.d is the fundamental resonant frequency of the bars in a spurious mode where the bars oscillate out of phase in a direction normal to the plane of the bars. ### Claim 17 A vibratory, double-bar force transducer comprising a generally rectangular sheet of material having a thickness t, a width 2 w+g, and a length L, said sheet of material including an elongate slot having a length m and centrally located therein to divide the sheet into two bar segments, each having a width w, said slot having a width g, wherein 0.4<t/w<4, and L/m.gtoreq.1, and means for causing said bar segments to vibrate at a frequency f in substantially 180.degree. phase opposition in a transverse direction, and means for determining the frequency of vibration of said bar segments. ### Claim 18 (depends on 17) A transducer as in claim 17 wherein said sheet of material is enlarged at its ends to have a width greater than 2 w+g, the distance separating the enlarged portions being L. ### Claim 19 (depends on 17, 18) A transducer as in claim 17 or 18 wherein t, w, L, and m are selected so that for any value of S in the range S.sub.min to S.sub.max, where S is the sensitivity of the transducer, with positive values of S representing tensile forces and negative values representing compressive forces, and S.sub.min and S.sub.max are the minimum and maximum values respectively of S used to define the desired operating range, at least one of the following inequalities holds: ##EQU25## where f.sub.p1 is the fundamental resonant frequency of the bars in a spurious mode where the bars oscillate in phase in a direction normal to the plane of the bars, f.sub.p2 is the second overtone of f.sub.p1, f.sub.p3 is the third overtone of f.sub.p1, and F.sub.d is the fundamental resonant frequency of the bars in a spurious mode where the bars oscillate out of phase in a direction normal to the plane of bars. ### Claim 20 A vibratory force transducer comprising an elongate beam having a thickness t and width w, wherein 0.4<t/w<4, means for causing said beam to resonate at a frequency f in a transverse direction, and wherein t and w are selected so that for any value of S in the range S.sub.min to S.sub.max, where S is the force sensitivity of the transducer, with positive values of S representing tensile forces and negative values representing compressive forces, and S.sub.min and S.sub.max are the minimum and maximum values of S respectively used to define the desired operating range, at one of the following inequalities holds: ##EQU26## where f.sub.p1 is the fundamental resonant frequency of the beam in a spurious mode where the beam oscillates in a direction normal to the transverse plane, f.sub.p2 is the second overtone of f.sub.p1, and f.sub.p3 is the third overtone of f.sub.p1. ### Claim 21 A vibratory force transducer comprising at least one elongate beam having a thickness t and a width w, means for causing said beam to resonate at a frequency f in a transverse direction, wherein t and w are selected so that for any value of S in the range S.sub.min to S.sub.max, where S is the force sensitivity of the transducer, with positive values of S representing tensile forces and negative values representing compressive forces, and S.sub.min and S.sub.max are the minimum and maximum values of S respectively used to define the desired operating range, at least one of the following inequalities holds: ##EQU27## where f.sub.p1 is the fundamental resonant frequency of the beam in a spurious mode where the beam oscillates in a direction normal to the transverse plane, f.sub.p2 is the second overtone of f.sub.p1, and f.sub.p3 is the third overtone of f.sub.p1. ### Claim 22 A vibratory force transducer comprising a pair of elongate, generally parallel bars coupled together at their ends and adapted to vibrate 180.degree. out of phase in a transverse direction, said bars having a thickness t and a width w, the distance between locations at which the bar ends are coupled together being m and the lengths of the bars being generally L, means for causing said bars to resonate at a frequency f in substantially 180.degree. phase opposition in a transverse direction, wherein t, w, L, and m are selected so that for any value of S in the range S.sub.min and S.sub.max, where S is the force sensitivity of the transducer, with positive values of S representing tensile forces and negative values representing compressive forces, and S.sub.min and S.sub.max are the minimum and maximum values of S respectively used to define the desired operating range, at least one of the following inequalities holds: ##EQU28## where f.sub.p1 is the fundamental resonant frequency of the bars in a spurious mode where the bars oscillate in phase in a direction normal to the plane of the bars, f.sub.p2 is the second overtone of f.sub.p1, f.sub.p3 is the third overtone of f.sub.p1, and f.sub.d is the fundamental resonant frequency of the bars in a spurious mode where the bars oscillate out of phase in a direction normal to the plane of the bars.