Comment comprendre le verrou SR

Je ne peux pas comprendre comment fonctionne le verrou SR. Apparemment, vous branchez une ligne d'entrée de R, et une autre de S, et vous êtes censé obtenir des résultats dans et Q ' .$Q$$Q'$

Cependant, les deux R et S nécessitent une entrée de la sortie de l'autre, et la sortie de l'autre nécessite une entrée de la sortie de l'autre. Qu'est-ce qui vient en premier le poulet ou l'œuf ??

Lorsque vous branchez ce circuit pour la première fois, comment démarre-t-il?

Une bascule est implémentée comme un multivibrateur bi-stable; par conséquent, Q et Q 'sont garantis comme étant inverses l'un de l'autre, sauf lorsque S = 1, R = 1, ce qui n'est pas autorisé. La table d'excitation de la bascule SR est utile pour comprendre ce qui se produit lorsque des signaux sont appliqués aux entrées.

S R  Q(t) Q(t+1)   
----------------
0 x   0     0       
1 0   0     1   
0 1   1     0   
x 0   1     1   

Les sorties Q et Q 'changeront rapidement d'état et s'arrêteront à un état stable après que des signaux ont été appliqués à S et R.

Example 1: Q(t) = 0, Q'(t) = 1, S = 0, R = 0. 

State 1: Q(t+1 state 1)  = NOT(R OR Q'(t)) = NOT(0 OR 1) = 0
         Q'(t+1 state 1) = NOT(S OR Q(t)) =  NOT(0 OR 0) = 1

State 2: Q(t+1 state 1)  = NOT(R OR Q'(t+1 state 1)) = NOT(0 OR 1) = 0
         Q'(t+1 state 2) = NOT(S OR Q(t+1 state 1))  =  NOT(0 OR 0) = 1     

Since the outputs did not change, we have reached a steady state; therefore, Q(t+1) = 0, Q'(t+1) = 1.


Example 2: Q(t) = 0, Q'(t) = 1, S = 0, R = 1

State 1: Q(t+1 state 1)  = NOT(R OR Q'(t)) = NOT(1 OR 1) = 0
         Q'(t+1 state 1) = NOT(S OR Q(t))  = NOT(0 OR 0) = 1


State 2: Q(t+1 state 2)  = NOT(R OR Q'(t+1 state 1)) = NOT(1 OR 1) = 0
         Q'(t+1 state 2) = NOT(S OR Q(t+1 state 1))  =  NOT(0 OR 0) = 1     


We have reached a steady state; therefore, Q(t+1) = 0, Q'(t+1) = 1.


Example 3: Q(t) = 0, Q'(t) = 1, S = 1, R = 0

State 1: Q(t+1 state 1)  = NOT(R OR Q'(t)) = NOT(0 OR 1) = 0
         Q'(t+1 state 1) = NOT(S OR Q(t)) =  NOT(1 OR 0) = 0

State 2: Q(t+1 state 2)  = NOT(R OR Q'(t+1 state 1)) = NOT(0 OR 0) = 1
         Q'(t+1 state 2) = NOT(S OR Q(t+1 state 1))  = NOT(1 OR 0) = 0     

State 3: Q(t+1 state 3)  = NOT(R OR Q'(t+1 state 2)) = NOT(0 OR 0) = 1
         Q'(t+1 state 3) = NOT(S OR Q(t+1 state 2))  = NOT(1 OR 1) = 0     

We have reached a steady state; therefore, Q(t+1) = 1, Q'(t+1) = 0.


Example 4: Q(t) = 1, Q'(t) = 0, S = 1, R = 0

State 1: Q(t+1 state 1)  = NOT(R OR Q'(t)) = NOT(0 OR 0) = 1
         Q'(t+1 state 1) = NOT(S OR Q(t)) =  NOT(1 OR 1) = 0

State 2: Q(t+1 state 2)  = NOT(R OR Q'(t+1 state 1)) = NOT(0 OR 0) = 1
         Q'(t+1 state 2) = NOT(S OR Q(t+1 state 1))  = NOT(1 OR 1) = 0     

We have reached a steady state; therefore, Q(t+1) = 1, Q'(t+1) = 0.


Example 5: Q(t) = 1, Q'(t) = 0, S = 0, R = 0

State 1: Q(t+1 state 1)  = NOT(R OR Q'(t)) = NOT(0 OR 0) = 1
         Q'(t+1 state 1) = NOT(S OR Q(t)) =  NOT(0 OR 1) = 0

State 2: Q(t+1 state 2)  = NOT(R OR Q'(t+1 state 1)) = NOT(0 OR 0) = 1
         Q'(t+1 state 2) = NOT(S OR Q(t+1 state 1))  = NOT(0 OR 1) = 0     

We have reached a steady; state therefore, Q(t+1) = 1, Q'(t+1) = 0.



With Q=0, Q'=0, S=0, and R=0, an SR flip-flop will oscillate until one of the inputs is set to 1.

Example 6: Q(t) = 0, Q'(t) = 0, S = 0, R = 0

State 1: Q(t+1 state 1)  = NOT(R OR Q'(t)) = NOT(0 OR 0) = 1
         Q'(t+1 state 1) = NOT(S OR Q(t)) =  NOT(0 OR 0) = 1

State 2: Q(t+1 state 2)  = NOT(R OR Q'(t+1 state 1)) = NOT(0 OR 1) = 0
         Q'(t+1 state 2) = NOT(S OR Q(t+1 state 1))  = NOT(0 OR 1) = 0     

State 3: Q(t+1 state 3)  = NOT(R OR Q'(t+1 state 2)) = NOT(0 OR 0) = 1
         Q'(t+1 state 3) = NOT(S OR Q(t+1 state 2)) =  NOT(0 OR 0) = 1

State 4: Q(t+1 state 4)  = NOT(R OR Q'(t+1 state 3)) = NOT(0 OR 1) = 0
         Q'(t+1 state 4) = NOT(S OR Q(t+1 state 3))  = NOT(0 OR 1) = 0     


As one can see, a steady state is not possible until one of the inputs is set to 1 (which is usually handled by power-on reset circuitry).