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continuous sensors - 23.39<br />

6.<br />

θ w<br />

a) V out = ( V 2 – V 1 ) ⎛----------⎞ + V<br />

⎝ ⎠ 1 = ( 5V – 0V)<br />

⎛-----------------<br />

42deg ⎞ + 0V = 0.7V<br />

⎝300deg⎠<br />

θ max<br />

θ w<br />

b) 2.765V = ( 5V – 0V)<br />

⎛-----------------<br />

⎞ + 0V<br />

⎝300deg⎠<br />

θ w<br />

2.765V = ( 5V – 0V)<br />

⎛-----------------<br />

⎞ + 0V<br />

⎝300deg⎠<br />

= 165.9deg<br />

θ w<br />

7.<br />

θ output<br />

=<br />

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

deg<br />

count<br />

θ input<br />

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

θ output<br />

50<br />

= ----- θ<br />

1 input = 50⎛0.1-------------<br />

deg ⎞ = 5-------------<br />

deg<br />

⎝ count⎠<br />

count<br />

R<br />

360 deg --------<br />

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

rot<br />

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

deg = 72 count -------------<br />

rot<br />

count<br />

8.<br />

strain gauge measures strain in a material using a stretching wire that increases resistance<br />

- accelerometers measure acceleration with a cantilevered mass on a piezoelectric<br />

element.<br />

9.<br />

R<br />

DMM V = K s ω<br />

ω· + ω⎛-----<br />

K2 ⎞ = V ⎛ K<br />

⎝JR⎠<br />

s ----- ⎞<br />

⎝JR⎠<br />

V s<br />

= ω( K) + ω· ⎛JR<br />

⎝<br />

----- ⎞<br />

K ⎠<br />

+<br />

-<br />

When the motor shaft is turned by<br />

another torque source a voltage is generated<br />

that is proportional to the angular<br />

velocity. This is the reverse emf. A dmm,<br />

or other high impedance instrument can<br />

be used to measure this, thus minizing<br />

the loses in resistor R.<br />

www.PA<strong>Control</strong>.com

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