CAIE FP2 2017 November — Question 11 EITHER

Exam BoardCAIE
ModuleFP2 (Further Pure Mathematics 2)
Year2017
SessionNovember
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicCircular Motion 2
TypeParticle on inner surface of sphere/bowl
DifficultyChallenging +1.8 This is a challenging Further Maths mechanics problem requiring energy conservation, circular motion dynamics (centripetal force), and the condition for losing contact (R=0). It involves multiple parts with geometric complexity (angles α and β on opposite sides), algebraic manipulation with given cos α = 1/16, and finding relationships between initial speed and loss of contact conditions. The multi-step nature, need to coordinate energy and force equations, and the geometric setup place it well above average difficulty but within reach of strong FM students.
Spec3.02h Motion under gravity: vector form6.02d Mechanical energy: KE and PE concepts6.02e Calculate KE and PE: using formulae6.02i Conservation of energy: mechanical energy principle6.05d Variable speed circles: energy methods

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A particle \(P\) of mass \(m\) is free to move on the smooth inner surface of a fixed hollow sphere of radius \(a\). The centre of the sphere is \(O\). The points \(A\) and \(A ^ { \prime }\) are on the inner surface of the sphere, on opposite sides of the vertical through \(O\); the radius \(O A\) makes an angle \(\alpha\) with the downward vertical and the radius \(O A ^ { \prime }\) makes an angle \(\beta\) with the upward vertical. The point \(B\) is on the inner surface of the sphere, vertically below \(O\). The point \(B ^ { \prime }\) is on the inner surface of the sphere and such that \(O B ^ { \prime }\) makes an angle \(2 \beta\) with the upward vertical through \(O\) (see diagram). It is given that \(\cos \alpha = \frac { 1 } { 16 }\).
  1. \(P\) is projected from \(A\) with speed \(u\) along the surface of the sphere downwards towards \(B\). Subsequently it loses contact with the sphere at \(A ^ { \prime }\). Show that \(u ^ { 2 } = \frac { 1 } { 8 } a g ( 1 + 24 \cos \beta )\).
  2. \(P\) is now projected from \(B\) with speed \(u\) along the surface of the sphere towards \(B ^ { \prime }\). Subsequently it loses contact with the sphere at \(B ^ { \prime }\). Find \(\cos \beta\).
  3. In part (i), the reaction of the sphere on \(P\) when it is initially projected at \(A\) is \(R\). Find \(R\) in terms of \(m\) and \(g\).

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A particle $P$ of mass $m$ is free to move on the smooth inner surface of a fixed hollow sphere of radius $a$. The centre of the sphere is $O$. The points $A$ and $A ^ { \prime }$ are on the inner surface of the sphere, on opposite sides of the vertical through $O$; the radius $O A$ makes an angle $\alpha$ with the downward vertical and the radius $O A ^ { \prime }$ makes an angle $\beta$ with the upward vertical. The point $B$ is on the inner surface of the sphere, vertically below $O$. The point $B ^ { \prime }$ is on the inner surface of the sphere and such that $O B ^ { \prime }$ makes an angle $2 \beta$ with the upward vertical through $O$ (see diagram). It is given that $\cos \alpha = \frac { 1 } { 16 }$.\\
(i) $P$ is projected from $A$ with speed $u$ along the surface of the sphere downwards towards $B$. Subsequently it loses contact with the sphere at $A ^ { \prime }$. Show that $u ^ { 2 } = \frac { 1 } { 8 } a g ( 1 + 24 \cos \beta )$.\\

(ii) $P$ is now projected from $B$ with speed $u$ along the surface of the sphere towards $B ^ { \prime }$. Subsequently it loses contact with the sphere at $B ^ { \prime }$. Find $\cos \beta$.\\

(iii) In part (i), the reaction of the sphere on $P$ when it is initially projected at $A$ is $R$. Find $R$ in terms of $m$ and $g$.\\

\hfill \mbox{\textit{CAIE FP2 2017 Q11 EITHER}}