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A Symbolic Analysis of Relay and Switching Circuits

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•<br />

7<br />

except for an illu str~tive example. Tbe method <strong>of</strong><br />

Pro<strong>of</strong> is that <strong>of</strong>' "perfect induction," i.e., the verification<br />

<strong>of</strong> the theorem for all possi ble cases.<br />

Since<br />

~r Pos~llpte 4 each variable is limited to the values<br />

o Bn d 1, this is B simple rna tter. Some <strong>of</strong> the the orems<br />

may be Droved more elegantly by recourse to p~evious<br />

theorems, Cut the method <strong>of</strong> perfect induction is so univer·sal<br />

thatit is pro ba bly to be preferred.<br />

1. 8. X + Y • y + x<br />

b. xy =yx<br />

2. a. x + (y + &) = (x + y) + g<br />

b. X(YIi) ..<br />

(xy)&<br />

-<br />

3. a • x(y + ii) ..<br />

xy + X5<br />

b. x + yfll<br />

-<br />

(x + y) (x + a-)<br />

-<br />

4. a • l-x ..<br />

x<br />

-<br />

b. 0 + x x<br />

5. a • 1 + x • 1<br />

b. O·x = 0<br />

For example, to Drove theo rem 4A,<br />

X is either ° or 1.<br />

..<br />

note the t<br />

If it is 0, the theorem f'ollows<br />

from 1)ostll1ate 2b; if 1, it folLOWS from rOs'tulate 3b.<br />

•<br />

'Je<br />

shall now define a new ope!'ation to be<br />

oalled negstion. rhe negative <strong>of</strong> a ~inderance X Will<br />

be Written X t <strong>and</strong> is defined as a variable Which is<br />

equal to 1 When X equals 0 <strong>and</strong> equal to 0 When X<br />

I

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