Step 1: Magnetic field produced by the stator currents.
The stator conductors (A, A$'$, B, B$'$) are carrying equal DC currents, arranged symmetrically. From figure (i), currents in opposite sides create a magnetic field that is approximately sinusoidal and distributed across the air gap. This field is stationary in space but constant in magnitude because the currents are DC.
Step 2: Induced e.m.f. in the rotor conductors.
The rotor is rotating clockwise at angular speed $\omega$. A conductor cutting the stationary flux at speed $\omega r$ will experience an induced e.m.f. according to:
\[
e = B \cdot l \cdot v = B l \omega r
\]
where $B$ is the flux density produced by the stator field. Thus, the induced e.m.f. in each rotor coil is AC in time because of rotation relative to the stator magnetic field.
Step 3: Relative positions of coils $a$–$a'$ and $b$–$b'$.
From the diagram, $a$–$a'$ and $b$–$b'$ are placed at $\;90^{\circ}$ apart (electrical). The stator MMF distribution is such that both $a$ and $b$ conductors see the same polarity of flux simultaneously due to symmetric current placement. Hence, their induced e.m.f.s will be in phase, not displaced.
Step 4: Evaluation of options.
- (A) \; Correct – Both $E_{a\text{–}a'}$ and $E_{b\text{–}b'}$ are finite and in phase.
- (B) \; Incorrect – No phase lead exists between the two.
- (C) \; Incorrect – No phase lead of $E_{a\text{–}a'}$ over $E_{b\text{–}b'}$.
- (D) \; Incorrect – Induced e.m.f.s are not zero because the rotor is rotating in a magnetic field.
% Final Answer
\[
\boxed{\text{Option (A): $E_{a\text{–}a'}$ and $E_{b\text{–}b'}$ are finite and in phase.}}
\]
The correct combination that relates the constructional feature, machine type and mitigation is \(\underline{\hspace{2cm}}\). 
Given an open-loop transfer function \(GH = \frac{100}{s}(s+100)\) for a unity feedback system with a unit step input \(r(t)=u(t)\), determine the rise time \(t_r\).
Consider a linear time-invariant system represented by the state-space equation: \[ \dot{x} = \begin{bmatrix} a & b -a & 0 \end{bmatrix} x + \begin{bmatrix} 1 0 \end{bmatrix} u \] The closed-loop poles of the system are located at \(-2 \pm j3\). The value of the parameter \(b\) is: