A body executes simple harmonic motion under the action of a force $F_1$ with a frequency $n_1$ and under another force $F_2$ with frequency $n_2$. If both forces act simultaneously in the same direction, the frequency of oscillation of the body is
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When SHM forces combine in the same direction, the net frequency is the square root of the sum of squares of individual frequencies.
If two simple harmonic restoring forces act in the same direction on the same body, their accelerations (and hence force constants) add. Since frequency $n = \dfrac{1}{2\pi} \sqrt{\dfrac{k}{m}}$, the effective force constant becomes $k_{\text{eq}} = k_1 + k_2$.
Thus, $n_{\text{eq}} = \sqrt{n_1^2 + n_2^2}$