We are given the magnetizing inductance \( L = 250 \, \text{mH} \) and core loss resistance \( R = 300 \, \Omega \). The power factor is the ratio of the real power to the apparent power. Since the secondary is open-circuited, we have only the primary magnetizing current to consider. The total impedance is given by:
\[
Z = R + j\omega L
\]
where \( \omega = 2\pi \times 50 \, \text{Hz} \), and the power factor \( \text{pf} = \frac{R}{|Z|} \). After calculating the impedance and the power factor, we get:
\[
\text{Power Factor} \approx 0.24 \, \text{to} \, 0.26
\]
Thus, the value of the power factor is \( 0.25 \).