Date | May 2015 | Marks available | 2 | Reference code | 15M.2.hl.TZ1.13 |
Level | HL only | Paper | 2 | Time zone | TZ1 |
Command term | Find | Question number | 13 | Adapted from | N/A |
Question
Richard, a marine soldier, steps out of a stationary helicopter, 1000 m above the ground, at time t=0t=0. Let his height, in metres, above the ground be given by s(t)s(t). For the first 10 seconds his velocity, v(t)ms−1v(t)ms−1, is given by v(t)=−10tv(t)=−10t.
(i) Find his acceleration a(t)a(t) for t<10t<10.
(ii) Calculate v(10)v(10).
(iii) Show that s(10)=500s(10)=500.
At t=10t=10 his parachute opens and his acceleration a(t)a(t) is subsequently given by a(t)=−10−5v, t≥10a(t)=−10−5v, t≥10.
Given that dtdv=1dvdtdtdv=1dvdt, write down dtdvdtdv in terms of vv.
You are told that Richard’s acceleration, a(t)=−10−5va(t)=−10−5v, is always positive, for t≥10t≥10.
Hence show that t=10+15ln(98−2−v)t=10+15ln(98−2−v).
You are told that Richard’s acceleration, a(t)=−10−5va(t)=−10−5v, is always positive, for t≥10t≥10.
Hence find an expression for the velocity, vv, for t≥10t≥10.
You are told that Richard’s acceleration, a(t)=−10−5va(t)=−10−5v, is always positive, for t≥10t≥10.
Find an expression for his height, ss, above the ground for t≥10t≥10.
You are told that Richard’s acceleration, a(t)=−10−5va(t)=−10−5v, is always positive, for t≥10t≥10.
Find the value of tt when Richard lands on the ground.
Markscheme
(i) a(t)=dvdt=−10 (ms−2)a(t)=dvdt=−10 (ms−2) A1
(ii) t=10⇒v=−100 (ms−1)t=10⇒v=−100 (ms−1) A1
(iii) s=∫−10tdt=−5t2(+c)s=∫−10tdt=−5t2(+c) M1A1
s=1000 for t=0⇒c=1000s=1000 for t=0⇒c=1000 (M1)
s=−5t2+1000s=−5t2+1000 A1
at t=10, s=500 (m)t=10, s=500 (m) AG
Note: Accept use of definite integrals.
[6 marks]
dtdv=1(−10−5v)dtdv=1(−10−5v) A1
[1 mark]
METHOD 1
t=∫1−10−5vdv=−15ln(−10−5v)(+c)t=∫1−10−5vdv=−15ln(−10−5v)(+c) M1A1
Note: Accept equivalent forms using modulus signs.
t=10, v=−100
10=−15ln(490)+c M1
c=10+15ln(490) A1
t=10+15ln490−15ln(−10−5v) A1
Note: Accept equivalent forms using modulus signs.
t=10+15ln(98−2−v) AG
Note: Accept use of definite integrals.
METHOD 2
t=∫1−10−5vdv=−15∫12+vdv=−15ln|2+v|(+c) M1A1
Note: Accept equivalent forms.
t=10, v=−100
10=−15ln|−98|+c M1
Note: If ln(−98) is seen do not award further A marks.
c=10+15ln98 A1
t=10+15ln98−15ln|2+v| A1
Note: Accept equivalent forms.
t=10+15ln(98−2−v) AG
Note: Accept use of definite integrals.
[5 marks]
5(t−10)=ln98(−2−v)
2+v98=−e−5(t−10) (M1)
v=−2−98e−5(t−10) A1
[2 marks]
dsdt=−2−98e−5(t−10)
s=−2t+985e−5(t−10)(+k) M1A1
at t=10, s=500⇒500=−20+985+k⇒k=500.4 M1A1
s=−2t+985e−5(t−10)+500.4 A1
Note: Accept use of definite integrals.
[5 marks]
t=250 for s=0 (M1)A1
[2 marks]
Total [21 marks]
Examiners report
Parts (i) and (ii) were well answered by most candidates.
In (iii) the constant of integration was often forgotten. Most candidates calculated the displacement and then used different strategies, mostly incorrect, to remove the negative sign from −500.
Surprisingly part (b) was not well done as the question stated the method. Many candidates simply wrote down dvdt while others seemed unaware that dvdt was the acceleration.
Part (c) was not always well done as it followed from (b) and at times there was very little to allow follow through. Once again some candidates started with what they were trying to prove. Among the candidates that attempted to integrate many did not consider the constant of integration properly.
In part (d) many candidates ignored the answer given in (c) and attempted to manipulate different expressions.
Part (e) was poorly answered: the constant of integration was often again forgotten and some inappropriate uses of Physics formulas assuming that the acceleration was constant were used. There was unclear thinking with the two sides of an equation being integrated with respect to different variables.
Although part (e) was often incorrect, some follow through marks were gained in part (f).