CAIE FP2 2012 June — Question 3 10 marks

Exam BoardCAIE
ModuleFP2 (Further Pure Mathematics 2)
Year2012
SessionJune
Marks10
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, and careful analysis of the loss of contact condition. The multi-part structure demands setting up force equations with variable normal reaction, applying conservation of energy twice in different contexts, and understanding when contact is lost (R=0). While the techniques are standard for FM students, the problem requires sustained reasoning across multiple steps and careful geometric/trigonometric setup, placing it well above average difficulty.
Spec6.02i Conservation of energy: mechanical energy principle6.02j Conservation with elastics: springs and strings6.05c Horizontal circles: conical pendulum, banked tracks6.05d Variable speed circles: energy methods

A particle \(P\) of mass \(m\) is projected horizontally with speed \(\sqrt{\left(\frac{1}{2}ga\right)}\) from the lowest point of the inside of a fixed hollow smooth sphere of internal radius \(a\) and centre \(O\). The angle between \(OP\) and the downward vertical at \(O\) is denoted by \(\theta\). Show that, as long as \(P\) remains in contact with the inner surface of the sphere, the magnitude of the reaction between the sphere and the particle is \(\frac{5}{2}mg(1 + 2\cos\theta)\). [4] Find the speed of \(P\)
  1. when it loses contact with the sphere, [3]
  2. when, in the subsequent motion, it passes through the horizontal plane containing \(O\). (You may assume that this happens before \(P\) comes into contact with the sphere again.) [3]

Question 3:

(i)
(iii) ---
3
(i)
AnswerMarks
(iii)2
Use conservation of energy: ½mv = ½m(7ga/2)
– mga (1 – cos θ) B1
2
[v = 3ga/2 + 2ga cos θ]
2
Equate radial forces: R = mv /a + mg cos θ B1
Eliminate v to find R: R = (3mg/2) (1 + 2 cos θ) A.G. M1 A1
Find cos θ 1 when R = 0: cos θ 1 = – ½ [θ1 = 2π/3] B1
Find speed at this point: v1 2 = ½ ga, v1 = √(½ ga) M1 A1
EITHER: Use energy to find reqd speed v 2: ½mv2 2 = ½mv1 2 – mga cos θ1
or ½m(7ga/2) – mga M1
Simplify: ½v2 2 = ¼ga + ½ga, v2 = √(3ga/2) M1 A1
OR: Find horiz. comp. of v 2: v1 cos (π–θ) [= ½v1 = √(ga/8)] (M1)
Find vertical comp. of v2: √{v1 2 sin 2 (π–θ) + ga} [= √(11ga/8)] (M1)
AnswerMarks
Combine comps. to find v2: v2 = √(ga/8 + 11ga/8) = √(3ga/2) (A1)4
3
AnswerMarks Guidance
3[10]
Page 5Mark Scheme: Teachers’ version Syllabus
GCE A LEVEL – May/June 20129231 22
Question 3:
--- 3
(i)
(iii) ---
3
(i)
(iii) | 2
Use conservation of energy: ½mv = ½m(7ga/2)
– mga (1 – cos θ) B1
2
[v = 3ga/2 + 2ga cos θ]
2
Equate radial forces: R = mv /a + mg cos θ B1
Eliminate v to find R: R = (3mg/2) (1 + 2 cos θ) A.G. M1 A1
Find cos θ 1 when R = 0: cos θ 1 = – ½ [θ1 = 2π/3] B1
Find speed at this point: v1 2 = ½ ga, v1 = √(½ ga) M1 A1
EITHER: Use energy to find reqd speed v 2: ½mv2 2 = ½mv1 2 – mga cos θ1
or ½m(7ga/2) – mga M1
Simplify: ½v2 2 = ¼ga + ½ga, v2 = √(3ga/2) M1 A1
OR: Find horiz. comp. of v 2: v1 cos (π–θ) [= ½v1 = √(ga/8)] (M1)
Find vertical comp. of v2: √{v1 2 sin 2 (π–θ) + ga} [= √(11ga/8)] (M1)
Combine comps. to find v2: v2 = √(ga/8 + 11ga/8) = √(3ga/2) (A1) | 4
3
3 | [10]
Page 5 | Mark Scheme: Teachers’ version | Syllabus | Paper
GCE A LEVEL – May/June 2012 | 9231 | 22
A particle $P$ of mass $m$ is projected horizontally with speed $\sqrt{\left(\frac{1}{2}ga\right)}$ from the lowest point of the inside of a fixed hollow smooth sphere of internal radius $a$ and centre $O$. The angle between $OP$ and the downward vertical at $O$ is denoted by $\theta$. Show that, as long as $P$ remains in contact with the inner surface of the sphere, the magnitude of the reaction between the sphere and the particle is $\frac{5}{2}mg(1 + 2\cos\theta)$.
[4]

Find the speed of $P$
\begin{enumerate}[label=(\roman*)]
\item when it loses contact with the sphere, [3]
\item when, in the subsequent motion, it passes through the horizontal plane containing $O$. (You may assume that this happens before $P$ comes into contact with the sphere again.) [3]
\end{enumerate}

\hfill \mbox{\textit{CAIE FP2 2012 Q3 [10]}}