The magnetic field \( B \) inside a toroid depends on the permeability of the material filling the toroid. The relation between the permeability of the material and the permeability of free space is given by:
\[
\mu = \mu_0 (1 + \chi)
\]
where:
- \( \mu_0 \) is the permeability of free space,
- \( \chi \) is the susceptibility of the material,
- \( \mu \) is the permeability of the material inside the toroid.
The magnetic field inside the toroid is given by:
\[
B = \frac{\mu I}{2 \pi r}
\]
where:
- \( I \) is the current,
- \( r \) is the radius of the toroid,
- \( \mu \) is the permeability of the material inside the toroid.
Now, the percentage increase in the magnetic field when the toroid is filled with the material is given by:
\[
{Percentage increase in } B = \frac{\Delta B}{B_{{initial}}} \times 100
\]
The initial magnetic field \( B_{{initial}} \) is given by \( B_{{initial}} = \frac{\mu_0 I}{2 \pi r} \), and the final magnetic field \( B_{{final}} \) is given by \( B_{{final}} = \frac{\mu_0 (1 + \chi) I}{2 \pi r} \).
Thus, the percentage increase in the magnetic field is:
\[
\frac{\Delta B}{B_{{initial}}} = \frac{B_{{final}} - B_{{initial}}}{B_{{initial}}} = \frac{\frac{\mu_0 (1 + \chi) I}{2 \pi r} - \frac{\mu_0 I}{2 \pi r}}{\frac{\mu_0 I}{2 \pi r}} = \chi
\]
Substituting \( \chi = 2 \times 10^{-2} \):
\[
{Percentage increase in } B = 2 \times 10^{-2} \times 100 = 2\%
\]
Thus, the percentage increase in the magnetic field is \( \boxed{2\%} \).