The impedance \( Z \) of a series R-C combination is given by:
\[
Z = \sqrt{X_L^2 + R^2}
\]
where \( X_L = \omega L \) is the inductive reactance and \( R \) is the resistance. In this case, we are given:
\[
Z = \frac{R}{\sqrt{2}}
\]
Since \( X_L = 0 \), the equation simplifies to:
\[
Z = R
\]
Now, the time constant \( \tau \) for an R-C circuit is given by:
\[
\tau = R \cdot C
\]
Using the relation for the impedance of the circuit, we have:
\[
Z = \frac{1}{\omega C} = \frac{R}{\sqrt{2}}
\]
So, we can solve for \( C \) as follows:
\[
C = \frac{1}{\omega R \sqrt{2}}
\]
Substituting \( \omega = 1000 \) rad/s and simplifying:
\[
C = \frac{1}{1000 R \sqrt{2}} = \frac{1}{1000 R} \quad \text{(in milliseconds)}
\]
Thus, the time constant \( \tau \) is:
\[
\tau = R \cdot \frac{1}{1000 R} = 1 \, \text{ms}
\]
Thus, the correct answer is \( \tau = 1 \, \text{ms} \).