Step 1: Understanding the magnetic field inside the toroid.
The magnetic field \( B \) inside a toroid with current \( I \) is given by the formula:
\[
B = \frac{\mu_0 N I}{2 \pi r},
\]
where:
- \( \mu_0 \) is the permeability of free space,
- \( N \) is the number of turns of the coil,
- \( I \) is the current passing through the coil,
- \( r \) is the radius of the toroid.
When the toroid is filled with a material of magnetic susceptibility \( \chi \), the permeability \( \mu \) of the material becomes:
\[
\mu = \mu_0 (1 + \chi).
\]
Step 2: Magnetic field with material inside the toroid.
The magnetic field in the toroid with the material inserted becomes:
\[
B = \frac{\mu N I}{2 \pi r} = \frac{\mu_0 (1 + \chi) N I}{2 \pi r}.
\]
Step 3: Comparing the magnetic fields.
The magnetic field without the material is:
\[
B_0 = \frac{\mu_0 N I}{2 \pi r}.
\]
The ratio of the magnetic field with the material to the magnetic field without the material is:
\[
\frac{B}{B_0} = \frac{\mu_0 (1 + \chi) N I}{2 \pi r} \div \frac{\mu_0 N I}{2 \pi r} = 1 + \chi.
\]
Step 4: Percentage increase in the magnetic field.
The percentage increase in the magnetic field is given by:
\[
\text{Percentage increase} = (1 + \chi - 1) \times 100 = \chi \times 100.
\]
Final Answer:
Thus, the percentage increase in the magnetic field is:
\[
\boxed{(1 + \chi) \times 100}.
\]