Force sensor for electrical measuring of forces, torques, acceleration pressures and mechanical stresses

• US 4,703,663 A
• Filed: 03/24/1986
• Issued: 11/03/1987
• Est. Priority Date: 08/09/1984
• Status: Expired due to Fees

• Current Assignee: OPPERMANN, CAROLA CHRISTINE (1/4 INTEREST), OPPERMANN, CHRISTA MARIA (1/2 INTEREST), OPPERMANN, VIOLA (1/4 INTEREST)
• Original Assignee: Klaus Oppermann
• Inventors: Oppermann, Klaus
• Primary Examiner(s): Ruehl, Charles A.
• Application Number:
  US06/859,984
• Time in Patent Office: 589 Days
• Field of Search: 73/766, 73/767, 73/768, 73/774, 73/777, 73/781, 73/862.63, 73/862.68, 338/5, 338/47, 338/99, 338/114
• US Class Current: 73/862.68
• CPC Class Codes: G01L 1/18 using properties of piezo-resistive materials, i.e. materials of which the ohmic resistance varies according to changes in magnitude or direction of force applied to the material
• CPC Class Codes: G01L 1/2293 of the semi-conductor type semi-conductor devices controllable by variations of applied mechanical force H01L29/84
• CPC Class Codes: G01L 9/0002 using variations in ohmic resistance G01L9/0051 takes precedence

Abstract

Force sensor for electric measuring of forces, mechanical stress or the like, which are converted in the interior of the force sensor into a mechanical normal stress field and then into an electric resistance change. Transverse to the normal stress σ_j a piezo-resistive measuring element (17) consisting of at least one layer of resistance material is applied whose material constant c is selected such that a mechanical strain of the measuring element resulting from the strain of a carrier body (1) does not influence the measurement. The resistance layers may be overlying crossing patterns M₁, M₂ forming area elements (13) of equal area size which completely exhibits the mutually perpendicular strains ε_x, ε_y of the carrier body (1). For compensating disturbing influences exterior of the normal stress field a compensation element (18) is provided corresponding to the measuring element (17).

Claims

1. A force sensor for electric measuring of forces, torques, acceleration, pressures and/or mechanical stresses applied to said force sensor in the form of a distributed mechanical stress field comprising:

(a) an electrically insulating carrier body;

(b) a piezo-resistive transducer comprising a first pattern of filaments firmly attached to said carrier body and at least one further pattern of filaments upon said first pattern, said patterns being separated by insulating layers, said filaments consisting of resistive material, said filaments of said first pattern having a direction transverse to that of said filaments of said further pattern;

(c) a force transmission means for applying said distributed mechanical stress field in normal direction onto said piezo-resistive transducer;

(d) plane elements formed by the projection of two adjacent of the said patterns in the direction of the lines of force of said stress field, said elements being of equal area and completely subjected to any strain of the carrier body caused by said distributed mechanical stress field, said strain having first and second strain components in the direction of said filaments of said first and said further patterns respectively; and

(e) a bridge circuit arrangement having branches consisting of said first and said further patterns, an electric current flowing through said first pattern in said direction of said first strain component and through said further pattern in said direction of said second strain component.

2. The force sensor of claim 1 wherein the resistive material is selected with a material constant c such that a change in resistance of said piezo-resistive transducer due to the application of said mechanical normal stress field remains essentially unaffected by mechanical strains of said transducer caused by said strain components of said carrier body.

3. The force sensor of claim 2 wherein said material constant c is determined by c=-μ

/(1-2μ

) where μ

is the Poisson'"'"'s ratio of the resistive material, the result being used for determining the pressure coefficient α

_p of the electric resistance of said resistive material.

4. The force sensor of claim 3 wherein α

p=(1+μ

)/E where E is the Young'"'"'s modulus of the resistive material.

5. The force sensor of claim 1 wherein a piezo-resistive compensation element corresponding to said piezo-resistive transducer is electrically connected in a first branch of a bridge circuit, a second branch thereof comprising said piezo-resistive transducer, said compensation element being arranged on a surface of said carrier body free from the influence of said normal stress field.

6. The force sensor of claim 1 wherein said piezo-resistive transducer is a thin film arranged firmly attached to said carrier body by means of cathode sputtering.

7. The force sensor of claim 1 wherein said plane elements of two adjacent patterns of filaments are of quadrangular form and have--in respect of said current direction--a ratio of length to width such that the product of ohmic area resistance of said filaments according to this ratio is the same in said two patterns.

8. The force sensor of claim 1 wherein at crossing points of said filaments of two adjacent of said patterns tangents of centre lines of said filaments form a right angle.

9. The force sensor of claim 1 wherein said filaments of two adjacent of said patterns are electrically series connected in one branch of said bridge circuit arrangement.

10. The force sensor of claim 5 wherein said piezo-resistive compensation element comprises a third pattern and at least one further pattern of filaments lying upon each other and said filaments of said patterns of said piezo-resistive transducer and said compensation element are arranged individually in different branches of a full bridge connection of said bridge circuit arrangement.

11. The force sensor of claim 1 wherein said filaments have ends provided with connecting means arranged on said carrier body such that they are free from said normal stress field.

12. The force sensor of claim 1 wherein one of said insulating layers provided between said patterns is formed by said carrier body.

13. The force sensor of claim 1 wherein between said force transtransmission body and the upper surface of patterns an intermediate layer of organic material is provided firmly attaching said upper surface of said pattern to said force transmission body.

14. The force sensor of claim 1 wherein said carrier body is a constructional element of a technical means.

15. The force sensor of claim 1 wherein said force transmission means is a solid body.

16. The force sensor of claim 1 wherein said force transmission means is a deformable medium.

17. A force sensor for electric measuring of forces, torques, accelerations, pressures and/or mechanical stresses acting in the form of a distributed mechanical stress field comprising:

(a) an electrically insulating carrier body,

(b) a piezo-resistive transducer comprising at least one two-dimensional pattern of filaments consisting of resistive material and firmly attached to said carrier body,

(c) a force transmission means for applying said distributed mechanical stress field normal to said piezo-resistive transducer;

wherein a material constant c of said resistive material is selected such that any change in resistance of the piezo-resistive transducer due to said stress field to be measured remains essentially uninfluenced by mechanical strain acting on said transducer and caused by mechanical strain caused in said carrier body upon application of said distributed mechanical stress field.

18. The force sensor of claim 17 wherein said material constant c is determined on the basis of the Poisson'"'"'s ratio μ

of said resistive material.

19. The force sensor of claim 18, wherein c=-μ

/(1-2μ

).

20. The force sensor of claim 18, wherein a pressure coefficient α

_p of the electric resistance of said resistive material is selected as α

_p =(1+μ

)/E where E is the Young'"'"'s modulus of the resistive material.

21. A force sensor for electrical measuring of forces, torques, acceleration, pressures and/or mechanical stresses applied to said force sensor in the form of a distributed mechanical stress field, comprising:

(a) an electrically insulating carrier body;

(b) a piezo-resistive transducer means comprising at least one pattern of filaments consisting of resistive material and firmly attached to said carrier body,

(c) a force transmission means for applying said distributed mechanical stress field in normal direction to said piezo-resistive transducer,

(d) a piezo-resistive compensation element having a design corresponding to said piezo-resistive transducer and being attached to a surface of said insulating carrier body, said compensation element being free from said distributed mechanical stress field, said piezo-resistive compensation element being electrically connected in branches of a bridge circuit arrangement;

wherein a material constant c of said resistive material is selected such that any change in resistance of the piezo-resistive transducer due to said stress field to be measured remains essentially uninfluenced by mechanical strain acting on said transducer and caused by mechanical strain caused in said carried body upon application of said distributed mechanical stress field.

22. The force sensor of claim 21 wherein an area of said force transmission means adjacent to said transducer means is provided with at least one flat recess opposing said associated compensation element.