Correct Answer - Option 1 : 612.5 rpm
Concept:
The EMF equation of a DC Machine is
\({E_b} = \frac{{NPϕ Z}}{{60A}}\)
From the above equation,
\(N \propto \frac{{{E_b}}}{ϕ }\)
In a dc generator, induced emf is
Eg = V + IaRa
In a dc motor, back emf is
Eb = V – IaRa
Where,
N is the speed in rpm
ϕ is the flux per pole
P is the number of poles
Z is the number of conductors
V is the terminal voltage
Ia is the armature current
Ra is the armature resistance
Calculation:
Case 1:
Terminal voltage (Vt) = 250 V
Armature current (Ia1) = 100 A
Speed (N1) = 300 rpm
Armature resistance (Ra) = 0.10 Ω
Back emf, Eb1 = Vt – Ia1Ra
= 250 – 100 × 0.1 = 240 V
Case 2:
Terminal voltage (Vt) = 250 V
Armature current (Ia2) = 50 A
Let the speed, in this case, is N2
Armature resistance (Ra) = 0.10 Ω
Back emf, Eb2 = Vt – Ia2Ra
= 250 – 50 × 0.1 = 245 V
ϕ2 = 0.5 ϕ1
\(\frac{{{E_{b1}}}}{{{E_{b2}}}} = \frac{{{N_1}}}{{{N_2}}} \times \frac{{{\phi _1}}}{{{\phi _2}}}\)
\( \Rightarrow \frac{{240}}{{245}} = \frac{{300}}{{{N_2}}} \times \frac{{{\phi _1}}}{{0.5{\phi _1}}}\)
⇒ N2 = 612.5 rpm