Answer: A
Solution (State Equations)
In state-space analysis of circuits, we typically choose the voltage across the capacitor (Vc) and the current through the inductor (iL) as our state variables.
Step 1: Apply KCL at the top node
The input current I splits into the capacitor current (ic) and the inductor branch current (iL):
I = ic + iL
Since ic = C(dVc/dt):
I = C(dVc/dt) + iL
I = ic + iL
Since ic = C(dVc/dt):
I = C(dVc/dt) + iL
Rearranging for the derivative of the first state variable:
dVc/dt = (0)Vc - (1/C)iL + (1/C)I --- (Eq. 1)
Step 2: Apply KVL to the right-hand branch
The voltage across the capacitor (Vc) is equal to the voltage across the series combination of L and R:
Vc = VL + VR
Since VL = L(diL/dt) and VR = iLR:
Vc = L(diL/dt) + iLR
Vc = VL + VR
Since VL = L(diL/dt) and VR = iLR:
Vc = L(diL/dt) + iLR
Rearranging for the derivative of the second state variable:
diL/dt = (1/L)Vc - (R/L)iL + (0)I --- (Eq. 2)
Step 3: Convert to Matrix Form (State-Space)
The standard form is แบ = Ax + Bu. Combining Eq. 1 and Eq. 2:
d/dt
=
+
[I]
Vc
iL
0
-1/C
1/L
-R/L
Vc
iL
1/C
0
Conclusion
Comparing our derived matrices to the given choices, the values in the A matrix [0, -1/C; 1/L, -R/L] and the B matrix [1/C; 0] match perfectly with Option 1.