To solve the problem of determining the speed of the car on a frictionless banked curve, we use the concept of circular motion on a banked road. When a car travels on a banked curve, the necessary centripetal force is provided by the horizontal component of the normal force due to the banking.
For a banked curve with an angle $\theta$, radius $r$, and with gravity $g = 9.8 \, ms^{-2}$, the optimum speed $v$ of the car that doesn't rely on friction is given by:
$$ v = \sqrt{rg \cdot \tan(\theta)} $$
Given:
The tangent of the angle $\theta = 45^{\circ}$ is:
$$ \tan(45^{\circ}) = 1 $$
Substituting the given values into the formula:
$$ v = \sqrt{90 \times 9.8 \times 1} $$
Calculate the value:
$$ v = \sqrt{882} $$
Upon calculation, we get:
$$ v \approx 29.7\, ms^{-1} $$
Rounding this to the nearest whole number, we find:
$$ v \approx 30\, ms^{-1} $$
Thus, the correct speed of the car negotiating the banked curve is $30 \,ms^{-1}$.
Conclusion: The correct answer is $30 \,ms^{-1}$. This matches the given correct answer.