1) This document is a 2012 HSC exam solution for a question about an object sinking in liquid.
2) The equation of motion for the object is derived using partial fractions, showing the velocity v over time t.
3) The displacement x over time is then derived by substituting the expression for v into the equation relating v and x.
4) The specific question is answered by substituting t = 4 seconds into the expressions for v and x to find how far the object has sunk after 4 seconds.
1 of 7
Download to read offline
More Related Content
2012 Extension 2 Resisted Motion
1. Extension II Mathematics: Mechanics
2012 HSC Resisted Motion
Brett M. Bujeya
John Paul College
June 23, 2013
This work is licensed under the Creative Commons 3.0 License.
Brett M. Bujeya 2012 HSC - Resisted Motion June 23, 2013 1 / 7
2. 2012 HSC, Question 13Question 13 (15 marks) Use a SEPARATE writing booklet.
(a) An object on the surface of a liquid is released at time t = 0 and immediately
sinks. Let x be its displacement in metres in a downward direction from the
surface at time t seconds.
The equation of motion is given by
2
dv v
= 10 ,
dt 40
where v is the velocity of the object.
(i)
(ii)
(iii)
t
20 e 1( )Show that v = .t
e + 1
dv dv 400
Use = v to show that x = 20logedt dx
400 v
How far does the object sink in the first 4 seconds?
.
4
2
2
2
Brett M. Bujeya 2012 HSC - Resisted Motion June 23, 2013 2 / 7
3. 2012 HSC, Question 13(i) Solution
dv
dt
= 10
v2
40
dv
dt
=
400 v2
40
40
v
0
dv
400 v2
=
t
0
dt
Using partial fractions,
40
dv
400 v2
= 40
dv
(20 + v)(20 v)
=
1
20 + v
+
1
20 v
dv
t
0
dt =
v
0
1
20 + v
+
1
20 v
dv
t = ln
20 + v
20 v
v
0
t = ln
20 + v
20 v
et
=
20 + v
20 v
20(et
1) = v(1 + et
)
v =
20(et
1)
1 + et
Brett M. Bujeya 2012 HSC - Resisted Motion June 23, 2013 3 / 7
4. 2012 HSC, Question 13(ii) Solution
v
dv
dx
= 10
v2
40
v
dv
dx
=
400 v2
40
x
0
dx = 40
v
0
v
400 v2
dv
x = 20 ln(400 v2
)
v
0
x = 20 ln
400 v2
400
x = 20 ln
400
400 v2
Brett M. Bujeya 2012 HSC - Resisted Motion June 23, 2013 4 / 7
5. 2012 HSC, Question 13(iii) Solution
When t = 0, v = 0 and x = 0
When t = 4, v =
20(e4
1)
e4 + 1
and
x = 20 ln
錚
錚 400
400 400(e41)2
(e4+1)2
錚
錚 = 20 ln
e4
+ 1
2
4e4
Hence, the particle moves 20 ln
e4
+ 1
2
4e4
metres in the 鍖rst 4 seconds.
Brett M. Bujeya 2012 HSC - Resisted Motion June 23, 2013 5 / 7
6. Notes From the Marking Centre I
i. In better responses, after 鍖nding the expression
dt
dv
=
40
400 v2
,
candidates used partial fractions and correct integration to obtain
t = ln
20 + v
20 v
. In better responses, candidates demonstrated their
competency by changing the subject to obtain the required expression for
v. In weaker responses, some candidates attempted to use the result for
dx
a2 x2
without resorting to partial fractions. In many of these
responses, candidates did not obtain the correct result of this integration.
ii. Having obtained
dx
dv
=
40v
400 v2
, the majority of candidates handled this
part well and obtained the required result.
Brett M. Bujeya 2012 HSC - Resisted Motion June 23, 2013 6 / 7
7. Notes From the Marking Centre II
iii. This part was again well done. The most successful approach was to
substitute t = 4 into v =
20(et
1)
et + 1
and then substitute this expression
into x = 20 ln
400
400 v2
.
Another approach was to integrate using
dx
dt
=
20(et
1)
et + 1
. Only a small
number of candidates used this approach, and of them very few
successfully obtained the required result.
Brett M. Bujeya 2012 HSC - Resisted Motion June 23, 2013 7 / 7