$$n_1\sin\theta_1=n_2\sin\theta_2$$
$$1.00\sin90\degree=1.33\sin\theta_2$$
$$\theta_2=48.7\degree$$
So angle between the extreme rays is
$$2\theta_2=97.5\degree$$
or
$$\tan48.75\degree=\frac h{R}$$
and we have
$$R=\frac{1.00\text{ m}}{\tan48.75\degree}=\boxed{1.14\text{ m}}$$
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