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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
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
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
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
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
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
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

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  • 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