Question:

Two identical springs are connected in series and parallel as shown in the figure. If $ f_{s} $ and $ f_{p} $ are frequency of series and parallel arrangement what is $ \frac{f_{s}}{f_{p}} $ ?

Updated On: Aug 15, 2022
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The Correct Option is A

Solution and Explanation

In first case, springs are connected in parallel, so their equivalent spring constant $k_p =k_1+k_2 $ So, frequency of this spring block system is given by $f_p =\frac{1}{2\pi} \sqrt{\frac{k_p}{m}} $ or $ f_p =\frac{1}{2\pi} \sqrt{\frac{k_1+k_2}{m}} $ but $ k_1=k_2 $ $ \therefore f_p =\frac{1}{2\pi} \sqrt{\frac{2k}{m}} $ ... (i) Now, in second case, springs are connected in series, so their equivalent spring constant $ k=\frac{k_1k_2}{k_1+k_2} $ Hence, frequency of this arrangement is given by $ f_s =\frac{1}{2\pi} \sqrt{\frac{k_1k_2}{(k_1+k_2)}} $ or $f_s =\frac{1}{2\pi}\sqrt{\frac{k}{2m}}$ ... (ii) Dividing E (ii) by E (i), we get $ \frac{f_s}{f_p} =\frac{\frac{1}{2\pi} \sqrt{\frac{k}{2m}}}{\frac{1}{2\pi} \sqrt{\frac{2k}{m}}}$ $=\sqrt{\frac{1}{4}} =\frac{1}{2} $
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Concepts Used:

System of Particles and Rotational Motion

  1. The system of particles refers to the extended body which is considered a rigid body most of the time for simple or easy understanding. A rigid body is a body with a perfectly definite and unchangeable shape.
  2. The distance between the pair of particles in such a body does not replace or alter. Rotational motion can be described as the motion of a rigid body originates in such a manner that all of its particles move in a circle about an axis with a common angular velocity.
  3. The few common examples of rotational motion are the motion of the blade of a windmill and periodic motion.