Standard +0.8 This is a standard energy conservation problem with elastic strings, but requires careful bookkeeping of two states and solving simultaneous equations. The setup is straightforward (horizontal surface, no gravity complications), but students must correctly apply elastic PE formula (½λx²/a) at two positions and set up energy equations. The algebra to eliminate initial KE and solve for λ is non-trivial but methodical. Typical of Further Mechanics questions requiring multiple techniques but no novel insight.
One end of a light elastic string, of natural length \(a\) and modulus of elasticity \(\lambda mg\), is attached to a fixed point \(O\). The string lies on a smooth horizontal surface. A particle \(P\) of mass \(m\) is attached to the other end of the string. The particle \(P\) is projected in the direction \(OP\). When the length of the string is \(\frac{4}{3}a\), the speed of \(P\) is \(\sqrt{2ag}\). When the length of the string is \(\frac{5}{3}a\), the speed of \(P\) is \(\frac{1}{2}\sqrt{2ag}\).
Find the value of \(\lambda\). [4]
One end of a light elastic string, of natural length $a$ and modulus of elasticity $\lambda mg$, is attached to a fixed point $O$. The string lies on a smooth horizontal surface. A particle $P$ of mass $m$ is attached to the other end of the string. The particle $P$ is projected in the direction $OP$. When the length of the string is $\frac{4}{3}a$, the speed of $P$ is $\sqrt{2ag}$. When the length of the string is $\frac{5}{3}a$, the speed of $P$ is $\frac{1}{2}\sqrt{2ag}$.
Find the value of $\lambda$. [4]
\hfill \mbox{\textit{CAIE Further Paper 3 2023 Q2 [4]}}