In the figure, both springs are connected to a single mass \( m \) from opposite ends. This is a case of parallel spring configuration.
When two springs are attached in this way:
- The effective spring constant is:
\[
k_{\text{eff}} = k_1 + k_2
\]
For a spring-mass system, the angular frequency \( \omega \) is given by:
\[
\omega = \sqrt{\frac{k_{\text{eff}}}{m}} = \sqrt{\frac{k_1 + k_2}{m}}
\]
Hence, the angular frequency is:
\[
\boxed{\omega = \sqrt{\frac{k_1 + k_2}{m}}}
\]