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Automating Manufacturing Systems - Process Control and ...

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continuous sensors - 23.16<br />

After the wire in Figure 23.16 has been deformed it will take on the new dimensions<br />

<strong>and</strong> resistance shown in Figure 23.17. If a force is applied as shown, the wire will<br />

become longer, as predicted by Young’s modulus. But, the cross sectional area will<br />

decrease, as predicted by Poison’s ratio. The new length <strong>and</strong> cross sectional area can then<br />

be used to find a new resistance.<br />

w’<br />

L’<br />

t’<br />

σ<br />

F<br />

--<br />

F<br />

= = ----- = Eε<br />

A wt<br />

∴ε<br />

=<br />

---------<br />

F<br />

Ewt<br />

F<br />

R' ρ------- L' ρ ---------------------------------------------<br />

L( ⎛ 1 ⎞ + ε)<br />

= =<br />

w't' w( 1 – νε ⎝<br />

⎠ )t( 1 – νε)<br />

∴∆R<br />

= R' – R = R<br />

( 1 + ε)<br />

( --------------------------------------- –<br />

1 – νε) ( 1 – νε)<br />

1<br />

where,<br />

ν = poissons ratio for the material<br />

F = applied force<br />

E = Youngs modulus for the material<br />

σε , = stress <strong>and</strong> strain of material<br />

Aside: Gauge factor, as defined below, is a commonly used measure of stain gauge<br />

sensitivity.<br />

GF<br />

=<br />

------ ⎛ ⎞ ∆R<br />

R ⎝ ⎠<br />

------------<br />

ε<br />

Figure 23.17<br />

The Electrical <strong>and</strong> Mechanical Properties of the Deformed Wire

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