Measure displacement from each arrangement's gravitational equilibrium. The series and parallel spring stiffness follows by adding forces or extensions. In the parallel arrangement the two spring forces change by each, giving equivalent stiffness . In series the common force extends each spring by , so total extension is and the equivalent stiffness is . HenceThe corresponding angular frequencies are . gravity shifts the equilibrium extensions but does not alter the small-oscillation stiffness of these ideal linear, massless springs.
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