The frequency of oscillation of a rigid dipole in an electric field is given by f=2π1IpE, where p is the dipole moment, E is the magnitude of the electric field, and I is the moment of inertia.
This implies f∝E.
The initial electric field is E1=E0x^, so its magnitude is E1=E0.
The initial frequency is f1∝E0.
When the second electric field E2=2E0(y^+z^) is introduced, the net electric field becomes Enet=E1+E2=E0x^+2E0y^+2E0z^.
The magnitude of the net electric field is Enet=E02+(2E0)2+(2E0)2=E02+4E02+4E02=3E0.
The new frequency is f2∝3E0.
The percentage change in the frequency is given by f1f2−f1×100%.
Substituting the values, we get (E03E0−1)×100%=(3−1)×100%.
Using 3≈1.732, the percentage change is (1.732−1)×100%=73.2%.
The approximate percentage change is 73%.
Answer: 73%