2016 Paper 2 Q9

Year: 2016
Paper: 2
Question Number: 9

Course: LFM Pure and Mechanics
Section: Momentum and Collisions

Difficulty: 1600.0 Banger: 1473.6

Problem

A small bullet of mass \(m\) is fired into a block of wood of mass \(M\) which is at rest. The speed of the bullet on entering the block is \(u\). Its trajectory within the block is a horizontal straight line and the resistance to the bullet's motion is \(R\), which is constant.
  1. The block is fixed. The bullet travels a distance \(a\) inside the block before coming to rest. Find an expression for \(a\) in terms of \(m\), \(u\) and \(R\).
  2. Instead, the block is free to move on a smooth horizontal table. The bullet travels a distance \(b\) inside the block before coming to rest relative to the block, at which time the block has moved a distance \(c\) on the table. Find expressions for \(b\) and \(c\) in terms of \(M\), \(m\) and \(a\).

Solution

  1. Since \(R\) is constant, \(F=ma \Rightarrow \text{acc} = \frac{R}{m}\) and \(v^2 = u^2 + 2as\) so \(0 = u^2 - 2 \frac{R}{m}a\), ie \(a = \frac{m u^2}{2R}\)
  2. By conservation of momentum, the bullet/block combination will eventually be travelling at \(v = \frac{m}{m+M}u\). The bullet will slow down to this speed in a time of \(\frac{m}{m+M}u = u - \frac{R}{m} T \Rightarrow T = \frac{Mm}{R(m+M)}u\) and will travel \(b+c = \frac{\left ( 1 - \left ( \frac{m}{m+M} \right)^2\right)u^2m}{2R}= \left ( 1 - \left ( \frac{m}{m+M} \right)^2\right)a\). The block will travell \(c = \frac12 \frac{R}{M} \frac{M^2m^2u^2}{R^2(m+M)^2} = \frac{Mm}{(m+M)^2}a\) Therefore the \(b = \left ( 1 - \left ( \frac{m}{m+M} \right)^2\right)a - \frac{Mm}{(m+M)^2}a = \frac{M}{M+m}a\)
Work done by friction is the relative gain in KE for the block. ie \(R \cdot c = \frac12 M \left ( \frac{m}{m+M}u\right)^2 \Rightarrow c = \frac{Mm}{(M+m)^2}a\).
Examiner's report
— 2016 STEP 2, Question 9

This question was the most popular of the mechanics questions, and many candidates were able to complete the first part of the question successfully. In many cases this was as far as they got, as a large number of candidates were unable to make significant progress on part (ii). Where candidates were able to identify a correct strategy for solving the problem they were often successful in reaching expressions, only losing marks through errors in the algebra.

As in previous years the Pure questions were the most popular of the paper with questions 1, 3 and 7 the most popular of these. The least popular questions of the paper were questions 10, 11, 12 and 13 with fewer than 400 attempts for each of them. There were many examples of solutions in this paper that were insufficiently well explained, given that the answer to be reached had been provided in the question.

Source: Cambridge STEP 2016 Examiner's Report · 2016-full.pdf
Rating Information

Difficulty Rating: 1600.0

Difficulty Comparisons: 0

Banger Rating: 1473.6

Banger Comparisons: 2

Show LaTeX source
Problem source
A small bullet of mass $m$ is fired into a block of wood of mass $M$ which is
at rest. 
The speed
of the bullet on entering the block is $u$.  Its trajectory 
within the block is a horizontal
straight line and  the resistance to the 
bullet's motion is $R$, which is constant.

\begin{questionparts}
\item The block is fixed. The bullet travels a distance
$a$ inside the block before coming to rest.
Find an expression for $a$ in terms of $m$, $u$ and $R$.

\item Instead, the block is free to move on a smooth horizontal 
table. The bullet travels a distance $b$ inside the block
before coming to rest relative to the block, at which time the 
block has moved a distance $c$ on the table. 
Find expressions for $b$ and $c$ in terms of $M$, $m$ and $a$.
 \end{questionparts}
Solution source
\begin{questionparts}
\item Since $R$ is constant, $F=ma \Rightarrow \text{acc} = \frac{R}{m}$ and $v^2 = u^2 + 2as$ so $0 = u^2 - 2 \frac{R}{m}a$, ie $a = \frac{m u^2}{2R}$

\item By conservation of momentum, the bullet/block combination will eventually be travelling at $v = \frac{m}{m+M}u$.

The bullet will slow down to this speed in a time of $\frac{m}{m+M}u = u - \frac{R}{m} T \Rightarrow T = \frac{Mm}{R(m+M)}u$ and will travel $b+c = \frac{\left ( 1 - \left ( \frac{m}{m+M} \right)^2\right)u^2m}{2R}= \left ( 1 - \left ( \frac{m}{m+M} \right)^2\right)a$.

The block will travell $c = \frac12 \frac{R}{M} \frac{M^2m^2u^2}{R^2(m+M)^2} = \frac{Mm}{(m+M)^2}a$

Therefore the $b = \left ( 1 - \left ( \frac{m}{m+M} \right)^2\right)a -  \frac{Mm}{(m+M)^2}a = \frac{M}{M+m}a$

\end{questionparts}

Work done by friction is the relative gain in KE for the block. ie $R \cdot c = \frac12 M \left (  \frac{m}{m+M}u\right)^2 \Rightarrow c = \frac{Mm}{(M+m)^2}a$.