EE 4770 Lecture Notes

Generated from file lsli04.dvi.

This page was generated using an imperfect translator. Text may be poorly positioned and mathematics will be barely readable. Illustrations will not show at all. If possible, view the PostScript or PDF versions of these notes.


04-1                                  The Wheatstone Bridge                                        *
 *          04-1





       Raison d'^etre:  convert tiny changes in resistance to voltage.


       Shown with an instrumentation amplifier.
       Like an ideal op-amp but with finite gain.


       Gain of instrumentation amplifier denoted by A.


       vo  = A(v+   vi).


       The Wheatstone bridge consists of four arms.




                      RB              RD
       vo  = A    ______________ ______________      vE .
                  RA  + RB       RC  + RD


04-1                   EE 4770 Lecture Transparency.  Formatted  13:06,  22 January 1999 from lsli0*
 *4.                  04-1

04-2 * * 04-2 Transducer can be placed in one, two, or four arms. Typical function: Ht(x) = R(1 + xk), xk o 1 where R is the nominal resistance of the transducer and k is a con- stant. For simplicity write function as: Ht(x) = R + Rs, where R is independent of the process-variable value and Rs is dependent on the process-variable value. Typically, R AE Rs. Usually, need to convert Rs to a voltage. 04-2 EE 4770 Lecture Transparency. Formatted 13:06, 22 January 1999 from lsli0* *4. 04-2
04-3 * * 04-3 Complementary Pairs Frequently, transducer pairs can have complementary responses. If so, there are two (usually identical) transducers: : : : : :positioned so they react oppositely to the process variable: : : : : :so that when their responses are subtracted: : : : : :their response to the process variable add: : : : : :and unwanted quantities cancel out. For example, consider: Ht1 (x) = R(1 + xk) and Ht2 (x) = R(1 xk). Sum: Ht1 (x) + Ht2 (x) = R. (Not helpful.) Difference: Ht1 (x) Ht2 (x) = 2xk. (Much better.) 04-3 EE 4770 Lecture Transparency. Formatted 13:06, 22 January 1999 from lsli0* *4. 04-3
04-4 * * 04-4 One-Transducer Configuration Arm B: Ht(x) = R + Rs = R(1 + xk). Other Arms: Resistor of value R. Rs Rs xk vo = A _________________ vE ss A _____vE = A ____vE . 2(2R + Rs) 4R 4 04-4 EE 4770 Lecture Transparency. Formatted 13:06, 22 January 1999 from lsli0* *4. 04-4
04-5 * * 04-5 Two-Transducer Configuration Arm A: Ht2 (x) = R Rs = R(1 xk). Arm B: Ht1 (x) = R + Rs = R(1 + xk). Other Arms: Resistor of value R. Rs xk vo = A _____vE = A ____vE . 2R 2 As one might expect, twice as sensitive. 04-5 EE 4770 Lecture Transparency. Formatted 13:06, 22 January 1999 from lsli0* *4. 04-5
04-6 * * 04-6 Four-Transducer Configuration Arms A and D: Ht2 (x) = R Rs = R(1 xk). Arms B and C: Ht1 (x) = R + Rs = R(1 + xk). Rs vo = A ____vE = AxkvE . R 04-6 EE 4770 Lecture Transparency. Formatted 13:06, 22 January 1999 from lsli0* *4. 04-6
04-7 Wheatstone Bridge Transfer Functions * * 04-7 Goal Let Rt = R Rs = R(1 xk) be the transducer response(s). Assume bridge designed properly. Need to find two functions: Hc(Rt) = : : : and Hc(Rs) = : : : Both functions are equivalent. Choose whichever is more convenient. Four-Transducer Configuration Hc(Rs) = vo = A Rs__RvE . Let Rt = R + Rs. Then Rs = Rt R. Hc(Rt) = A Rt__R_____RvE = A Rt__R 1 vE . Two-Transducer Configuration Hc(Rs) = vo = A__2Rs__RvE . Hc(Rt) = A__2Rt__R_____RvE = A__2 Rt__R 1 vE . One-Transducer Configuration Hc(Rs) = vo = A__4Rs__RvE . Hc(Rt) = A__4Rt__R_____RvE = A__4 Rt__R 1 vE . 04-7 EE 4770 Lecture Transparency. Formatted 13:06, 22 January 1999 from lsli0* *4. 04-7
04-8 Wheatstone Bridge Sample Problem * * 04-8 Design a system with output vo = H (x), where process variable x is strain and, x 2 [0; 105 ], and H (x) = 106 x V. Strain will be covered in more detail later. For now, all we need to know is that strain is dimensionless. Strain is measured by a strain gauge. Strain gauges frequently used in complementary pairs. Use strain gauges with response: Ht(- ) = R(1 + - Gf ), where - denotes strain and constant Gf = 2. (Gf called gauge factor, a dimensionless quantity.) Position the two strain gauges to obtain response: Ht(x) = R(1 + xGf ) and Ht0(x) = R(1 xGf ). 04-8 EE 4770 Lecture Transparency. Formatted 13:06, 22 January 1999 from lsli0* *4. 04-8
04-9 * * 04-9 Derivation of Conditioning Circuit Needed A Wheatstone bridge is the obvious choice because transducer response is in form R Rs. Nevertheless, conditioning-circuit derivation will be presented. H(x) = Hc(Ht(x)) (Analysis performed as though there were one transducer.) y_ 1 y = Ht(x) = Rt = R(1 + xGf ). Then x = _R______G. f y_ 1 _y_ 1 Then Hc(y) = H R_______G = 106 R_______ V. f Gf Response for two-transducer configuration: Hc(Rt) = A__2 Rt__R 1 vE . 6 Choose A and vE so that A__2vE = 10___GV is satisfied. f For example, vE = 10 V and A = 105 . 04-9 EE 4770 Lecture Transparency. Formatted 13:06, 22 January 1999 from lsli0* *4. 04-9

ECE Home Page 4770 Home Page Up
David M. Koppelman - koppel@ee.lsu.edu
Modified 22 Jan 1999 13:08 (19:08 UTC)