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Year 11 Specialist (Unit 1 & 2) Algebra of vectors

Applications of vectors - relative velocity

20 practice questions 0 video lessons Theory + worked examples

Explore relative velocity in Year 11 Specialist Mathematics in Queensland (QCAA), where vectors describe how one moving object appears from another and how a craft moves through a current or a wind. It is the applied heart of the algebra of vectors topic.

You will learn to find the velocity of one object relative to another by subtracting vectors, and the true ground velocity of a boat or plane by adding the current or wind — then read off ground speed, bearings, crossing times and drift for real navigation problems.

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Theory

Relative velocity asks how one moving object appears from another, and how a craft’s velocity combines with the medium it moves through. In Year 11 Specialist Mathematics (QCAA, Queensland) you use vector subtraction for the velocity of one object relative to another, and vector addition to find the true (ground) velocity of a boat in a current or a plane in a wind.

The velocity of \(A\) relative to \(B\) is how \(A\) appears to move to an observer travelling with \(B\). It is found by subtracting the velocities: \(\mathbf{v}_{A\text{ rel }B}=\mathbf{v}_A-\mathbf{v}_B\). Reversing the objects reverses the vector: \(\mathbf{v}_{B\text{ rel }A}=-\mathbf{v}_{A\text{ rel }B}\).

A resultant (actual) velocity is what you get when a craft moves through a moving medium. The craft’s velocity relative to the ground equals its velocity relative to the medium plus the velocity of the medium: \(\mathbf{v}_{\text{craft/ground}}=\mathbf{v}_{\text{craft/medium}}+\mathbf{v}_{\text{medium/ground}}\). The current or wind is always added, never subtracted.

The heading is the direction the craft is pointed (its velocity through the water or air); the track or course is the direction it actually travels over the ground. When the two velocities are perpendicular, combine their magnitudes with Pythagoras and find the direction with a tangent ratio.

Two everyday tasks fall out of this: steering a boat upstream so its resultant runs straight across a river, and finding the ground speed and bearing of a plane blown off a heading by wind. Speeds use metric units (m/s or km/h) and directions use compass bearings or “east of north” style descriptions.

Resultant velocity triangle A right-angled velocity triangle. The current points 4 units east, the boat points 3 units north through the water, and the resultant ground velocity is the hypotenuse of length 5 from the start to the far corner. current 4 boat 3 ground 5
Resultant velocity: a boat heading north at \(3\) through a current of \(4\) east gives a ground velocity of \(5\) (head-to-tail addition).
Velocity of A relative to B Vectors vA=(4,1) and vB=(1,3) are drawn from the origin. The velocity of A relative to B, equal to vA minus vB = (3,-2), is the dashed arrow from the head of vB to the head of vA. v_A v_B v_A - v_B
Velocity of \(A\) relative to \(B\): \(\mathbf{v}_A-\mathbf{v}_B\) is the arrow from the head of \(\mathbf{v}_B\) to the head of \(\mathbf{v}_A\).

Velocity of one object relative to another (subtract the velocity of the observer):

\[ \mathbf{v}_{A\text{ rel }B}=\mathbf{v}_A-\mathbf{v}_B \]
vAB=vAvB

Resultant (ground) velocity of a craft in a moving medium — add the medium’s velocity:

\[ \mathbf{v}_{\text{craft/ground}}=\mathbf{v}_{\text{craft/medium}}+\mathbf{v}_{\text{medium/ground}} \]
vg=vm+vw

For perpendicular components, the resultant speed and its direction \(\theta\) are:

\[ |\mathbf{v}|=\sqrt{v_x^{\,2}+v_y^{\,2}}, \qquad \tan\theta=\dfrac{v_x}{v_y} \]
|v|=vx2+vy2
Add the medium, subtract the observer. To combine a craft with a current or wind you add the medium’s velocity; to find how one object looks from another you subtract the observer’s velocity. Keep exact answers exact — a resultant of \(\sqrt{45}\) is written \(3\sqrt{5}\), not a rounded decimal.

How to solve a relative-velocity problem

  1. Set axes and write each velocity as a vector. Take \(\mathbf{i}\) as east and \(\mathbf{j}\) as north (or across and along the bank), and write every speed and direction in component form.
  2. Choose subtract or add. For “\(A\) relative to \(B\)” compute \(\mathbf{v}_A-\mathbf{v}_B\); for a true/ground velocity add the current or wind to the craft’s own velocity.
  3. Combine the components. Add or subtract the \(\mathbf{i}\) and \(\mathbf{j}\) parts separately to get the resultant vector.
  4. Extract speed and direction. Use \(|\mathbf{v}|=\sqrt{v_x^{\,2}+v_y^{\,2}}\) for the speed and a tangent ratio for the angle, then read off the bearing, crossing time or drift the question asks for.
Example 1 — Velocity of one drone relative to another
Two drones fly with velocities \(\mathbf{v}_A=6\mathbf{i}+8\mathbf{j}\) m/s and \(\mathbf{v}_B=2\mathbf{i}+5\mathbf{j}\) m/s. Find the velocity of \(A\) relative to \(B\), and its magnitude.
Solution

Subtract the observer’s velocity: \(\mathbf{v}_A-\mathbf{v}_B\).

\(\mathbf{v}_A-\mathbf{v}_B\)\(=\)\((6\mathbf{i}+8\mathbf{j})-(2\mathbf{i}+5\mathbf{j})\)
\(=\)\((6-2)\mathbf{i}+(8-5)\mathbf{j}\)
\(=\)\(4\mathbf{i}+3\mathbf{j}\)

Take the magnitude of that vector with Pythagoras.

\(|\mathbf{v}_A-\mathbf{v}_B|\)\(=\)\(\sqrt{4^2+3^2}\)
\(=\)\(\sqrt{16+9}\)
\(=\)\(\sqrt{25}\)
\(=\)\(5\)

\(A\) moves at \(4\mathbf{i}+3\mathbf{j}\) m/s relative to \(B\), a speed of \(5\) m/s.

Example 2 — Ferry pushed off course
A ferry heads due north across a river at \(12\) m/s relative to the water. The current flows due east at \(9\) m/s. Find the ferry’s actual speed over the ground and the angle its track makes east of north.
Solution

The northward and eastward velocities are perpendicular, so add head to tail and use Pythagoras.

\(|\mathbf{v}|\)\(=\)\(\sqrt{12^2+9^2}\)
\(=\)\(\sqrt{144+81}\)
\(=\)\(\sqrt{225}\)
\(=\)\(15\)

The track angle east of north uses \(\tan\theta=\dfrac{\text{east}}{\text{north}}\).

\(\tan\theta\)\(=\)\(\dfrac{9}{12}\)
\(\theta\)\(=\)\(\tan^{-1}\!\left(\dfrac{9}{12}\right)\)
\(=\)\(36.87^\circ\)
\(\approx\)\(37^\circ\)

The ferry travels at \(15\) m/s along a track about \(37^\circ\) east of north.

Example 3 — Steering upstream to cross straight
A boat can travel at \(10\) m/s in still water and must cross a \(240\) m wide river that flows at \(6\) m/s, landing directly opposite its start. Find the across-speed of the boat and the time to cross.
Solution

Point the boat upstream so its along-bank part cancels the current: \(10\sin\theta=6\).

\(\sin\theta\)\(=\)\(\dfrac{6}{10}\)
\(\theta\)\(=\)\(\sin^{-1}(0.6)\)
\(\approx\)\(37^\circ \text{ upstream}\)

The across-speed is the remaining side of the right triangle.

\(v_{\text{across}}\)\(=\)\(\sqrt{10^2-6^2}\)
\(=\)\(\sqrt{100-36}\)
\(=\)\(\sqrt{64}\)
\(=\)\(8\)

Crossing time uses only the across-speed.

\(t\)\(=\)\(\dfrac{\text{width}}{v_{\text{across}}}\)
\(=\)\(\dfrac{240}{8}\)
\(=\)\(30\)

The boat crosses at \(8\) m/s and takes \(30\) s (steering about \(37^\circ\) upstream).

Example 4 — Plane in a crosswind
A light plane is steered due east with an airspeed of \(160\) km/h. A wind blows toward the north at \(120\) km/h. Taking \(\mathbf{i}\) as east and \(\mathbf{j}\) as north, find the ground velocity, the ground speed, and the bearing of the actual track.
Solution

Add the eastward airspeed and the northward wind to get the ground velocity.

\(\mathbf{v}_g\)\(=\)\((160\mathbf{i}+0\mathbf{j})+(0\mathbf{i}+120\mathbf{j})\)
\(=\)\(160\mathbf{i}+120\mathbf{j}\)

Ground speed is the magnitude of that vector.

\(|\mathbf{v}_g|\)\(=\)\(\sqrt{160^2+120^2}\)
\(=\)\(\sqrt{25600+14400}\)
\(=\)\(\sqrt{40000}\)
\(=\)\(200\)

East is \(090^\circ\); the wind turns the track north of east by \(\alpha\).

\(\alpha\)\(=\)\(\tan^{-1}\!\left(\dfrac{120}{160}\right)\)
\(=\)\(36.87^\circ\)
\(\text{bearing}\)\(=\)\(090^\circ-37^\circ\)
\(=\)\(053^\circ\)

The ground velocity is \(160\mathbf{i}+120\mathbf{j}\) km/h, a ground speed of \(200\) km/h on a bearing of about \(053^\circ\).

Common pitfalls

Adding when you should subtract (or the reverse). Watch out: the velocity of \(A\) relative to \(B\) is \(\mathbf{v}_A-\mathbf{v}_B\), a subtraction; the true velocity of a craft in a current is \(\mathbf{v}_{\text{craft/medium}}+\mathbf{v}_{\text{medium/ground}}\), an addition. Decide which task you have before touching the components.
Getting the subtraction order backwards. \(\mathbf{v}_A-\mathbf{v}_B\) and \(\mathbf{v}_B-\mathbf{v}_A\) point opposite ways. “\(A\) relative to \(B\)” means subtract \(B\)’s velocity from \(A\)’s.
Measuring the angle from the wrong direction. An angle “east of north” is measured from north, so \(\tan\theta=\dfrac{\text{east}}{\text{north}}\); a bearing is measured clockwise from north. Draw the triangle before choosing the ratio.
Rounding an exact answer. Watch out: if a resultant is a surd such as \(\sqrt{45}\), leave it as \(3\sqrt{5}\) unless the question asks for a decimal.

Frequently asked questions

How do you find the velocity of A relative to B?

Subtract the velocities: \(\mathbf{v}_{A\text{ rel }B}=\mathbf{v}_A-\mathbf{v}_B\). It is how \(A\) appears to move to an observer travelling with \(B\).

When do you add and when do you subtract velocities?

Add to find a true (ground) velocity of a craft in a current or wind: craft-in-medium plus medium. Subtract to find how one object looks from another (relative velocity).

How do you find a boat’s actual speed across a river?

When the boat’s velocity and the current are perpendicular, combine their speeds with Pythagoras: \(|\mathbf{v}|=\sqrt{v_x^{\,2}+v_y^{\,2}}\).

How do you steer a boat so it goes straight across a current?

Point upstream at an angle \(\theta\) so the upstream part cancels the current, using \(\sin\theta=\dfrac{\text{current}}{\text{boat speed}}\); the across-speed is then \(\sqrt{\text{boat}^2-\text{current}^2}\).

What is the difference between heading and track?

The heading is the direction the craft is pointed (its velocity through the water or air); the track is the direction it actually travels over the ground once the current or wind is added.

How do you find the crossing time and drift?

The crossing time is the river width divided by the across-component of the velocity; the downstream drift is the current speed multiplied by that time.