Method for adjusting a resistance-gage force transducer and an adjusted force transducer thus obtained

• US 4,688,434 A
• Filed: 04/04/1986
• Issued: 08/25/1987
• Est. Priority Date: 04/09/1985
• Status: Expired due to Fees

• Current Assignee: Sfernice Societe Francaise de L'Electro-Resistance
• Original Assignee: Sfernice Societe Francaise de L'Electro-Resistance
• Inventors: Cherbuy, Jean
• Primary Examiner(s): NOT, DEFINED
• Application Number:
  US06/848,289
• Time in Patent Office: 508 Days
• Field of Search: 73/765, 73/862.65, 73/862.66, 73/1 B, 338/2, 338/5, 338/195
• US Class Current: 73/862.622
• CPC Class Codes: G01G 3/1404 combined with means to connect the strain gauges on electrical bridges
• CPC Class Codes: G01G 3/1414 Arrangements for correcting or for compensating for unwanted effects

Abstract

A force transducer comprises a resilient bar (1) which carries a measuring bridge formed by resistance gages (R₁, . . . R₄). One end of the bar is attached to a stationary support (2) and the other end is subjected to a force (P) to be measured. A method for ensuring that the signal delivered by the measuring bridge is proportional to the applied force and insensitive to parasitic couples consists in determining the initial characteristics of the transducer, in computing the relative errors arising from a displacement of the force (P) applied as a function of the angle made between the resistance gages (R₁, . . . R₄) and the longitudinal direction (O_x) of the bar (1) and in cancelling these errors by making changes in one or a number of gages in order to modify the angle aforesaid.

Claims

1. A method for adjusting a resistance-gage force transducer (resistance gages R₁, R₂, R₃, R₄) comprising a resilient bar (1) attached at one end to a stationary support (2) and subjected at the other end to the force (P) to be measured, said bar (1) being adapted to carry resistance gages (R₁, . . . R₄) electrically connected to each other so as to form a measuring bridge for delivering an electrical signal which is a function of the force applied to said other end of the bar, said transducer being adjustable by means of said method in such a manner as to ensure that said electrical signal is proportional to the applied force and insensitive to the torsional and flexural couples generated by the displacements of the point of application of the force (P) to be measured, said method being distinguished by the following steps:

A. Determination of the initial characteristics of the transducer,

B. Computation of the relative errors of the transducer arising from a displacement of the applied force (P) as a function of the angle θ

formed between the resistance gages (R₁, . . . R₄) and the longitudinal direction (O_x) of the bar,

C. Cancellation of these errors by making modifications in one or a number of resistance gages in order to produce a modification of the angle θ

aforesaid.

2. A method according to claim 1, wherein the errors of the transducer are computed by means of the following relations:

space="preserve" listing-type="equation">e.sub.x =e.sub.x.sbsb.o +1/C.sub.x Σ

cos 2θ

space="preserve" listing-type="equation">e.sub.z =e.sub.z.sbsb.o +1/C.sub.z Σ

sin 2θ

where

e_x and e_z are the errors due to a displacement of the force (P) applied respectively along the axis (O_x) of the bar (1) and along an axis (O_z) perpendicular to said bar axis and to the applied force (P),

e_x.sbsb.o and e_z.sbsb.o are the initial errors determined during the step which involves initial characterization of the transducer,

C_x and C_z are known constants which are established by design and by the conditions of initial characterization of the transducer,

and wherein the corrections to be made in the angle θ

of each resistor are determined from the relations given above in order to cancel the errors e_x and e_z.

3. A method according to claim 2 in which the resistance gages form a zero angle θ

with the axis O_x of the bar, wherein the error e_x aforesaid is cancelled by applying to a resistance gage having a suitable parity a correction;

space="preserve" listing-type="equation">dθ

.sub.x ≅

(C.sub.x |e.sub.x0 |/4)1/2

and by applying a correction -dθ

_x to the other gage having the same parity and the error e_z is cancelled by applying to a gage having a suitable parity a correction;

space="preserve" listing-type="equation">dθ

.sub.z ≅

C.sub.z |e.sub.z0 |/4

and by applying a correction -dθ

_z to a gage having a different parity.

4. A method according to claim 2 in which the resistance gages comprise groups such that in each group having a same parity there is a gage forming an angle θ

=0 and a gage forming an angle θ

=π

/4, wherein the error e_x is cancelled by applying to one of the gages θ

=π

/4 a correction;

space="preserve" listing-type="equation">dθ

.sub.x =C.sub.x e.sub.x O/2

and the error e_z is cancelled by applying to a gage θ

=0 a correction;

space="preserve" listing-type="equation">dθ

.sub.z =C.sub.z e.sub.z1 /2.

5. A method according to claim 3 in which the resistance gages (R₁ . . . R₄) are constituted by resistive layers having the shape of rectangles and applied on the bar (1), wherein the angle θ

of the resistance gages is corrected by cutting two parallel grooves (l₁, l₂) in said layers so as to form a parallelogram with the two opposite sides of the rectangle formed by each gage, said grooves being inclined with respect to the initial direction of said gages at the angle dθ

_x or dθ

_z determined by the relations given above.

6. A method according to claim 3 in which the resistance gages (R₁, . . . R₄) are constituted by resistive layers having the shape of rectangles and applied on the bar (1), wherein the angle θ

of said resistance gages is corrected by forming notches (e₁, e₂, . . . ) transversely in the longitudinal edges of said gages in order to ensure that the resultant electrical direction (L₁) of said gages forms the angle dθ

_x or dθ

_z with the initial direction, said angle being determined by the relations given above.

7. A method according to claim 6, wherein said grooves (l₁, l₂) or notches (e₁, e₂, . . . ) are cut by means of a laser beam.

8. A method according to claim 3 in which the resistance gages are formed by a principal resistor (R₀) which makes a predetermined angle with the longitudinal axis (O_x) of the bar (1), each principal resistor (R₀) being connected in series with an additional resistor (R_a, R_b) having a low ohmic value in comparison with the ohmic value of the principal resistor (R₀) and inclined at a predetermined angle θ

with respect to said principal resistor, wherein the errors (e_x) and (e_z) are cancelled by modifying the ohmic value of one or a number of said additional resistors (R_a, R_b), the effect of said modification being to modify the virtual angle made between the resistance gage and the axis (O_x) of the bar (1).

9. A resistance-gage force transducer (resistance gages R₁, . . . R₄) comprising a resilient bar (1) such that one end of said bar is intended to be attached to a stationary support (2) and the other end is subjected to the force (P) to be measured, said bar (1) being adapted to carry resistance gages (R₁, . . . R₄) electrically connected to each other so as to form a measuring bridge for delivering an electrical signal which is a function of the force (P) applied to said other end of the bar, said transducer being so adjusted as to ensure that the signal is proportional to the applied force (P) and insensitive to the torsional and flexural couples generated by the displacements of the point of application of the force to be measured, wherein the angle θ

formed between one or a plurality of resistance gages (R₁, . . . R₄) and the longitudinal direction (O_x) of the bar (1) satisfies the following relations;

space="preserve" listing-type="equation">e.sub.x =e.sub.x.sbsb.o +1/C.sub.x Σ

cos 2θ

=0

space="preserve" listing-type="equation">e.sub.z =e.sub.z.sbsb.o +1/C.sub.z Σ

sin 2θ

=0

where

e_x and e_z are the errors due to a displacement of the force (P) applied respectively along the axis (O_x) of the bar (1) and along an axis (O_z) perpendicular to said axis of the bar and to the applied force,

e_x.sbsb.o and e_z.sbsb.o are the initial errors determined during a step which involves initial characterization of the transducer,

C_x and C_z are known constants established by design and by the conditions of said initial characterization.

10. A force transducer according to claim 9 in which the resistance gages (R₁, . . . R₄) are constituted by resistive layers having the shape of rectangles and applied on the bar (1), wherein the resistance gages (R₁, . . . R₄) each have two parallel grooves (l₁, l₂) cut so as to form a parallelogram with the two opposite sides of the rectangle formed by each gage, said grooves being inclined with respect to the initial direction of said gages at an angle dθ

_x or dθ

_z which is determined by the following relations;

space="preserve" listing-type="equation">dθ

.sub.x ≅

(C.sub.x |e.sub.x0 |/4)1/2

space="preserve" listing-type="equation">dθ

.sub.z ≅

C.sub.z |e.sub.z0 |/4.

11. A force transducer according to claim 9, wherein each resistance gage comprises a principal resistor (R₀) which makes a predetermined angle with the longitudinal axis (O_x) of the bar (1), each principal resistor (R₀) being connected in series with additional resistors (R_a, R_b, . . . ) having a low ohmic value in comparison with the ohmic value of the principal resistor (R₀) and inclined at a predetermined angle θ

with respect to said principal resistor, and wherein the ohmic value of one or a number of said additional resistors has been modified, the effect of said modification being to modify the virtual angle made between the resistance gage and the axis (O_x) of the bar (1).