QCAA Specialist Mathematics Alternative Sequence Modelling motion

9 sample questions with marking guides and sample answers

Q19
2022
QCAA
Paper 2
7 marks
Q19
7 marks

A research organisation plans to use a drone to drop a scientific instrument vertically from a stationary position above the ocean surface. The acceleration (m s2)\left(\text{m s}^{-2}\right) of the falling instrument can be modelled by 9.80.1v9.8 - 0.1v, where vv is its velocity (m s1)\left(\text{m s}^{-1}\right).

In order for the instrument sensors to activate, its speed as it hits the ocean surface must reach at least 20 m s120 \text{ m s}^{-1}. However, if it hits with a speed above 50 m s150 \text{ m s}^{-1}, the sensors will be damaged.

Determine the range of the drone's flying height above the ocean surface to ensure that the sensors are activated but not damaged.

Reveal Answer

Assume downwards as the positive direction
a=9.80.1va = 9.8 - 0.1v
vdvdx=9.80.1vv \frac{dv}{dx} = 9.8 - 0.1v
v9.80.1vdv=dx\int \frac{v}{9.8 - 0.1v} dv = \int dx
vv98dv=110dx\int \frac{v}{v - 98} dv = \int \frac{-1}{10} dx
1+98v98dv=110dx\int 1 + \frac{98}{v - 98} dv = \int \frac{-1}{10} dx
v+98lnv98=x10+cv + 98 \ln|v - 98| = \frac{-x}{10} + c

Assume the origin is at the point of release.
Given v(0)=0c=98ln(98)v(0) = 0 \Rightarrow c = 98 \ln(98)
v+98lnv98=x10+98ln(98)v + 98 \ln|v - 98| = \frac{-x}{10} + 98 \ln(98)

Let the distance to the ocean surface be hh metres.
Consider time of drop for each required velocity
When v=20 m s1,x=hv = 20 \text{ m s}^{-1}, x = h
20+98ln78=h10+98ln(98)20 + 98 \ln|-78| = \frac{-h}{10} + 98 \ln(98)
h=23.7 mh = 23.7 \text{ m}

When v=50 m s1,x=hv = 50 \text{ m s}^{-1}, x = h
50+98ln48=98ln(98)h1050 + 98 \ln|-48| = 98 \ln(98) - \frac{h}{10}
h=199.5 mh = 199.5 \text{ m}

The range of the drone's flying height above the ocean surface should be between 23.7 m and 199.5 m.

Marking Criteria
DescriptorMarks

correctly establishes a differential equation in terms of vv and xx

1

determines general solution of the differential equation

1

determines value for the constant

1

determines model for the velocity in terms of displacement

1

determines displacement of the drop for the minimum acceptable speed

1

determines displacement of the drop for the maximum acceptable speed

1

communicates range of the drone's flying height including units

1
Q3
2022
QCAA
Paper 1
1 mark
Q3
1 mark

A particle travels in a straight line over time, tt, with a constant acceleration, a(t)a(t).

Which function could represent the particle's displacement, x(t)x(t)?

A

x(t)=t3x(t) = t^3

B

x(t)=t2x(t) = t^2

C

x(t)=1tx(t) = \frac{1}{t}

D

x(t)=tx(t) = \sqrt{t}

Reveal Answer
A

x(t)=t3x(t) = t^3

If x(t)=t3x(t) = t^3, the acceleration is the second derivative, a(t)=6ta(t) = 6t. This represents an acceleration that changes with time, not a constant acceleration.

B

x(t)=t2x(t) = t^2

Correct Answer

Acceleration is the second derivative of displacement. For x(t)=t2x(t) = t^2, the first derivative (velocity) is 2t2t and the second derivative (acceleration) is 22, which is a constant.

C

x(t)=1tx(t) = \frac{1}{t}

If x(t)=1tx(t) = \frac{1}{t}, the second derivative is a(t)=2t3a(t) = \frac{2}{t^3}, which is not a constant value.

D

x(t)=tx(t) = \sqrt{t}

If x(t)=tx(t) = \sqrt{t}, the second derivative is a(t)=14t3/2a(t) = -\frac{1}{4t^{3/2}}, which means the acceleration is not constant.

Q14
2022
QCAA
Paper 2
5 marks
Q14

An object is moving in a straight line with an acceleration represented by the differential equation dvdt=(4+v2)\frac{dv}{dt} = -\left(4 + v^2\right), where vv is the object's velocity (m s1)\left(\text{m s}^{-1}\right) over time, t (s)t\text{ (s)}, where t0t \ge 0, until it comes to rest.

Q14a
3 marks

Determine the general solution of the differential equation.

Reveal Answer

dvdt=(4+v2)\frac{dv}{dt} = -(4 + v^2)
14+v2dvdt=1\frac{1}{4 + v^2} \frac{dv}{dt} = -1
14+v2dv=1dt\int \frac{1}{4 + v^2} dv = \int -1 dt
1224+v2dv=1dt\frac{1}{2} \int \frac{2}{4 + v^2} dv = \int -1 dt
12tan1(v2)=t+c\frac{1}{2} \tan^{-1} \left(\frac{v}{2}\right) = -t + c

Marking Criteria
DescriptorMarks

correctly establishes a suitable integration result based on the separation of variables technique

1

determines one side of the general solution in terms of vv

1

determines the other side of the general solution in terms of tt

1
Q14b
2 marks

The initial velocity of the object is 1.5 m s11.5 \text{ m s}^{-1}.

Determine the time when the particle comes to rest.

Reveal Answer

Given v(0)=1.5v(0) = 1.5
12tan1(1.52)=c\frac{1}{2} \tan^{-1} \left(\frac{1.5}{2}\right) = c
c0.32c \approx 0.32

When v=0v = 0:
12tan1(0)t+0.32\frac{1}{2} \tan^{-1}(0) \approx -t + 0.32
t0.32 st \approx 0.32 \text{ s}
The particle comes to rest after 0.32 s.

Marking Criteria
DescriptorMarks

determines an expression that represents the integration constant

1

determines the time when the particle is at rest

1
Q17
2020
QCAA
Paper 2
7 marks
Q17
7 marks

An object is released from rest at a height of 100 m above the ground.

The motion of the vertical descent of the object is modelled by

vdvdx=9.80.004v2(v0)v\frac{dv}{dx} = 9.8 - 0.004v^2 \quad (v \ge 0)

where vv is the velocity (m s1\text{m s}^{-1}) and xx is the displacement from the ground (m).

Determine the velocity of the object when it strikes the ground.

Reveal Answer

vdvdx=9.80.004v2,v>0v\frac{dv}{dx} = 9.8 - 0.004v^2, v > 0 v9.80.004v2dv=dx\int \frac{v}{9.8 - 0.004v^2} dv = \int dx 10.0080.008v9.80.004v2dv=dx\frac{-1}{0.008} \int \frac{-0.008v}{9.8 - 0.004v^2} dv = \int dx 125ln9.80.004v2=x+c-125\ln|9.8 - 0.004v^2| = x + c Given v=0 when x=100\text{Given } v = 0 \text{ when } x = -100 125ln9.8=100+c-125\ln|9.8| = -100 + c c185.298c \approx -185.298 125ln9.80.004v2=x185.298-125\ln|9.8 - 0.004v^2| = x - 185.298 Determining v when x=0\text{Determining } v \text{ when } x = 0 125ln9.80.004v2=185.298-125\ln|9.8 - 0.004v^2| = -185.298 Using graph facility of GDC\text{Using graph facility of GDC} v36.7 ms1 or v36.7 ms1v \approx -36.7 \text{ ms}^{-1} \text{ or } v \approx 36.7 \text{ ms}^{-1} As v>0, the negative solution is rejected\text{As } v > 0 \text{, the negative solution is rejected} v36.7 ms1\therefore v \approx 36.7 \text{ ms}^{-1}
Marking Criteria
DescriptorMarks

correctly uses separation of variables

1

correctly develops the general solution of the differential equation

1

correctly uses the given position of the origin

1

uses the given condition to determine value for c

1

substitutes the displacement at impact to form an equation in terms of v

1

determines one reasonable solution of v

1

shows logical organisation communicating key steps

1
Q15
2020
QCAA
Paper 1
4 marks
Q15

The motion of an object that moves in a straight line is given by v(x)=cos1(2x)v(x) = \cos^{-1}(2x) where vv is the velocity (m s1\text{m s}^{-1}) and xx is the displacement (m) from the origin.

Q15a
2 marks

Determine a(x)a(x) where aa is the acceleration (m s2\text{m s}^{-2}) of the object.

Reveal Answer

v(x)=cos1(2x)v(x)=\cos^{-1}(2x)
a=vdvdxa=v\frac{dv}{dx}
dvdx=10.25x2\frac{dv}{dx}=\frac{-1}{\sqrt{0.25-x^2}}
a=cos1(2x)0.25x2a=\frac{-\cos^{-1}(2x)}{\sqrt{0.25-x^2}}

Marking Criteria
DescriptorMarks

correctly determines dvdx\frac{dv}{dx}

1

determines an expression for acceleration as a function of displacement

1
Q15b
2 marks

Use the result from 15a) to determine a(0)a(0), given 2πa(0)0-2\pi \le a(0) \le 0. Express your answer in simplest form.

Reveal Answer

When x=0x=0
a=cos1(0)0.5a=\frac{-\cos^{-1}(0)}{0.5}
cos1(0)=π2\cos^{-1}(0)=\frac{\pi}{2}
a(0)=(π2)0.5a(0)= -\frac{\left(\frac{\pi}{2}\right)}{0.5}
=π (m s2)=-\pi\ (\text{m s}^{-2})

Marking Criteria
DescriptorMarks

determines a correct exact value for the inverse trigonometric expression on the numerator

1

determines a reasonable solution for a(0)a(0) based on the given range (2πa(0)0-2\pi\le a(0)\le 0)

1
Q4
2020
QCAA
Paper 2
1 mark
Q4
1 mark

A particle is moving with simple harmonic motion described by the equation x=1.32cos(πt2)x = 1.32 \cos\left(\frac{\pi t}{2}\right) where xx (m) is the displacement of the particle from a central position over time tt (s), t0t \ge 0.

The maximum speed of the particle is

A

2.07 m s12.07 \text{ m s}^{-1}

B

4.15 m s14.15 \text{ m s}^{-1}

C

4.30 m s14.30 \text{ m s}^{-1}

D

5.28 m s15.28 \text{ m s}^{-1}

Reveal Answer
A

2.07 m s12.07 \text{ m s}^{-1}

Correct Answer

The maximum speed of a particle in simple harmonic motion is given by vmax=Aωv_{max} = A\omega. With amplitude A=1.32A = 1.32 and angular frequency ω=π2\omega = \frac{\pi}{2}, the maximum speed is 1.32×π22.07 m s11.32 \times \frac{\pi}{2} \approx 2.07 \text{ m s}^{-1}.

B

4.15 m s14.15 \text{ m s}^{-1}

This incorrect answer comes from multiplying the amplitude by π\pi instead of π2\frac{\pi}{2}, effectively using the wrong angular frequency.

C

4.30 m s14.30 \text{ m s}^{-1}

This is an incorrect calculation. The maximum speed must be found using the derivative of the displacement function, which yields vmax=Aωv_{max} = A\omega.

D

5.28 m s15.28 \text{ m s}^{-1}

This value is 1.32×41.32 \times 4, which incorrectly multiplies the amplitude by a factor of 4 rather than the angular frequency ω=π2\omega = \frac{\pi}{2}.

Q1
2020
QCAA
Paper 2
1 mark
Q1
1 mark

The position xx (m) at time tt (s) of a 7 kg particle moving in a straight line is given by

x=3t35t2+2t4x = 3t^3 - 5t^2 + 2t - 4 for 0t100 \le t \le 10

Determine the time when the particle has a momentum of 620 kg m s1620 \text{ kg m s}^{-1}.

A

1.73 s

B

2.60 s

C

3.66 s

D

3.71 s

Reveal Answer
A

1.73 s

Incorrect. This value does not satisfy the momentum equation. You must find the velocity function by differentiating the position function, then solve mv(t)=620m v(t) = 620.

B

2.60 s

Incorrect. This result likely comes from a sign error in the quadratic formula, mistakenly using b=70-b = -70 instead of +70+70 when solving 63t270t606=063t^2 - 70t - 606 = 0.

C

3.66 s

Incorrect. This result comes from an algebraic error in the quadratic formula, specifically forgetting to square the bb term in the discriminant (b24acb^2 - 4ac).

D

3.71 s

Correct Answer

Correct. Velocity is the derivative of position, v(t)=9t210t+2v(t) = 9t^2 - 10t + 2. Setting momentum p=mv=7(9t210t+2)=620p = mv = 7(9t^2 - 10t + 2) = 620 and solving the resulting quadratic equation 63t270t606=063t^2 - 70t - 606 = 0 yields t3.71 st \approx 3.71 \text{ s}.

Q6
2022
QCAA
Paper 2
1 mark
Q6
1 mark

A 4 kg object moves in a straight line over time, t (s)t\text{ (s)}, where 0t50 \le t \le 5 with velocity v=9+8tt2(m s1)v = 9 + 8t - t^2 \left(\text{m s}^{-1}\right).

Determine the momentum of the object when t=3t = 3.

A

24 kg m s124 \text{ kg m s}^{-1}

B

27 kg m s127 \text{ kg m s}^{-1}

C

96 kg m s196 \text{ kg m s}^{-1}

D

100 kg m s1100 \text{ kg m s}^{-1}

Reveal Answer
A

24 kg m s124 \text{ kg m s}^{-1}

This is the velocity of the object at t=3t = 3, not the momentum. You must multiply the velocity by the mass to find the momentum.

B

27 kg m s127 \text{ kg m s}^{-1}

This is an incorrect calculation. To find the momentum, first calculate the velocity at t=3t = 3, then multiply by the mass of 4 kg4 \text{ kg}.

C

96 kg m s196 \text{ kg m s}^{-1}

Correct Answer

The velocity at t=3t = 3 is v=9+8(3)32=24 m s1v = 9 + 8(3) - 3^2 = 24 \text{ m s}^{-1}. Multiplying this velocity by the mass (4 kg4 \text{ kg}) gives the correct momentum of 96 kg m s196 \text{ kg m s}^{-1}.

D

100 kg m s1100 \text{ kg m s}^{-1}

This is the momentum of the object at t=4t = 4, not t=3t = 3. Ensure you substitute the correct time into the velocity equation.

Q17
2021
QCAA
Paper 2
7 marks
Q17
7 marks

An object with a mass of 2 kg is released from rest at the top of a 1 metre long frictionless plane inclined at 3030^\circ to the horizontal.

A force of P\boldsymbol{P} newtons acting parallel to the plane opposes the motion of the object as it travels down the plane.

When the object is xx metres from the top of the plane, its velocity is v m s1v\text{ m s}^{-1}.

Given P=44x2|\boldsymbol{P}| = \frac{4}{\sqrt{4-x^2}}, determine xx when v=2v = 2.

Reveal Answer

Method 1
Resolving net forces along the plane
Fnet=2gsin(30)44x2F_{\text{net}} = 2g \sin(30^\circ) - \frac{4}{\sqrt{4 - x^2}}

Fnet=maF_{\text{net}} = ma
g44x2=2ag - \frac{4}{\sqrt{4 - x^2}} = 2a

g44x2=2vdvdxg - \frac{4}{\sqrt{4 - x^2}} = 2v \frac{dv}{dx}

vdvdx=4.924x2v \frac{dv}{dx} = 4.9 - \frac{2}{\sqrt{4 - x^2}}

v dv=4.924x2 dx\int v \ dv = \int 4.9 - \frac{2}{\sqrt{4 - x^2}} \ dx

v22=4.9x2sin1(x2)+c\frac{v^2}{2} = 4.9x - 2 \sin^{-1} \left(\frac{x}{2}\right) + c

Given v=0v = 0 when x=0x = 0
0=02sin1(0)+c0 = 0 - 2 \sin^{-1}(0) + c
c=0c = 0
v2=9.8x4sin1(x2)\therefore v^2 = 9.8x - 4 \sin^{-1} \left(\frac{x}{2}\right)

When v=2v = 2
4=9.8x4sin1(x2)4 = 9.8x - 4 \sin^{-1} \left(\frac{x}{2}\right)

Solving for xx using GDC
x=0.51 mx = 0.51 \text{ m}

Marking Criteria
DescriptorMarks

correctly determines the net forces along the plane

1

determines equation for acceleration along the plane

1

determines differential equation in terms of velocity and displacement

1

determines general solution to a differential equation

1

determines value of arbitrary constant

1

establishes equation to solve for xx when v=2v = 2

1

determines xx

1

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