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Unit 1: Kinematics

Scalars and Vectors

Tell scalars from vectors, write any vector in unit-vector notation or as magnitude and direction, and add vectors by components.

Topic 1.1 · 8 min read

Walk 3 m east, then 4 m north. Your feet covered 7 m, but you are only 5 m from where you started, and "5 m" alone doesn't say where you are: you need "5 m, 53° north of east". The first number is a scalar and the second is a vector, and nearly every quantity in mechanics is one or the other.

Magnitude only, or magnitude and direction

A scalar is a quantity that a single number with a unit describes completely: mass (2.0 kg2.0\ \text{kg}), time (3.5 s3.5\ \text{s}), temperature, energy. A vector needs a size, called its magnitude, and a direction. Pushing a stalled car with 300 N300\ \text{N} forward and pushing it with 300 N300\ \text{N} backward have the same magnitude and opposite effects, so force must be a vector.

The kinematics quantities split like this:

Scalar (how much)Vector (how much, and which way)
distance: total length of path coveredposition: where the object is relative to an origin
speed: how fast, in any directiondisplacement: change in position, start to finish
velocity: rate of change of position
acceleration: rate of change of velocity

Speed is the magnitude of velocity. Distance is not the magnitude of displacement, because distance counts every back-and-forth while displacement only compares the start and finish. In the opening walk, distance is 7 m7\ \text{m} and the magnitude of the displacement is 5 m5\ \text{m}.

You draw a vector as an arrow: it points in the vector's direction, and its length is proportional to its magnitude, using whatever scale the diagram states. A velocity arrow twice as long as another means twice the speed. In print, a vector gets an arrow over its symbol, A⃗\vec{A}, and its magnitude is written AA or ∣A⃗∣|\vec{A}|. A magnitude is never negative.

In one dimension, there are only two directions, so a sign does the job of the arrow. Pick a positive direction (say, right or up); then the opposite direction is negative. A car that moves from x=+5 mx = +5\ \text{m} to x=−3 mx = -3\ \text{m} has displacement Δx=−3−5=−8 m\Delta x = -3 - 5 = -8\ \text{m}: 8 m8\ \text{m} in the negative direction. The minus sign is direction, not a "smaller" quantity. Reverse your choice of positive direction and every sign flips, but the physics is unchanged.

Components and unit-vector notation

In two or three dimensions, you describe a vector by how far it reaches along each axis. Those numbers are its components. To name the directions, use the unit vectors i^\hat{i}, j^\hat{j} and k^\hat{k}: arrows of magnitude 1 (no units) pointing along +x+x, +y+y and +z+z. Any vector is the sum of three vectors parallel to the axes:

A⃗=Ax i^+Ay j^+Az k^.\vec{A} = A_x\,\hat{i} + A_y\,\hat{j} + A_z\,\hat{k}.

The components AxA_x, AyA_y, AzA_z carry the units and the signs. A displacement (−3.0 i^+4.0 j^) m(-3.0\,\hat{i} + 4.0\,\hat{j})\ \text{m} means 3.0 m3.0\ \text{m} in the −x-x direction and 4.0 m4.0\ \text{m} in the +y+y direction.

The vector A drawn from the origin to the point (-3, 4), in the second quadrant. A dashed horizontal segment of length 3 runs along the negative x-axis, labeled A sub x = -3, and a dashed vertical segment of length 4 rises to the arrow's tip, labeled A sub y = 4. The vector has magnitude 5. The angle theta sub A = 126.9 degrees is measured counterclockwise from the positive x-axis to the vector.

Going between the two descriptions is right-triangle trigonometry. If θ\theta is the angle measured counterclockwise from the +x+x axis to the vector, the projections onto the axes, and the way back, are:

For the vector in the figure, A=(−3.0)2+(4.0)2=5.0A = \sqrt{(-3.0)^2 + (4.0)^2} = 5.0. A calculator's inverse tangent gives tan⁡−1(4.0−3.0)=−53.1∘\tan^{-1}\left(\frac{4.0}{-3.0}\right) = -53.1^\circ, which points into the fourth quadrant, the wrong one. The inverse tangent can't tell 4−3\frac{4}{-3} from −43\frac{-4}{3}, so it always answers between −90∘-90^\circ and 90∘90^\circ. When AxA_x is negative, add 180∘180^\circ: θ=126.9∘\theta = 126.9^\circ, or equivalently 53.1∘53.1^\circ above the −x-x axis.

The position vector r⃗\vec{r} points from the origin to the object: r⃗=x i^+y j^+z k^\vec{r} = x\,\hat{i} + y\,\hat{j} + z\,\hat{k}. Its magnitude is the object's distance from the origin, and dividing r⃗\vec{r} by that magnitude gives the unit vector r^=r⃗∣r⃗∣\hat{r} = \frac{\vec{r}}{|\vec{r}|}, which has length 1 and points the same way. For a particle at r⃗=(2.0 i^−2.0 j^+1.0 k^) m\vec{r} = (2.0\,\hat{i} - 2.0\,\hat{j} + 1.0\,\hat{k})\ \text{m}, the distance is 4+4+1=3.0 m\sqrt{4 + 4 + 1} = 3.0\ \text{m} and

r^=23 i^−23 j^+13 k^.\hat{r} = \tfrac{2}{3}\,\hat{i} - \tfrac{2}{3}\,\hat{j} + \tfrac{1}{3}\,\hat{k}.

You will use r^\hat{r} whenever a quantity points straight away from or toward a center, as gravity does in topic 2.6 (it points along −r^-\hat{r}, toward the center).

Adding vectors by components

The resultant of several vectors is their vector sum. Geometrically, you place them tip to tail, and the resultant runs from the first tail to the last tip. Algebraically, you add the components axis by axis:

This works because the i^\hat{i} parts of the arrows lie along one line, where adding is ordinary 1D addition with signs, and the same is true for j^\hat{j} and k^\hat{k} separately. What you can't do is add magnitudes. Two displacements of 3 m3\ \text{m} and 4 m4\ \text{m} have a resultant anywhere from 1 m1\ \text{m} (opposite directions) to 7 m7\ \text{m} (same direction); only when they are perpendicular is it 5 m5\ \text{m}. In general, ∣A⃗+B⃗∣≤A+B|\vec{A} + \vec{B}| \le A + B, with equality only for parallel vectors.

Worked examples

Worked exampleExample 1: from magnitude and direction to components

A hockey puck slides at 8.0 m/s8.0\ \text{m/s} in the direction 35∘35^\circ south of west. With +x+x east and +y+y north, write its velocity in unit-vector notation.

Show solution

Draw it first: west is −x-x, and 35∘35^\circ south of west tips the arrow below the −x-x axis, into the third quadrant. So both components are negative. The 35∘35^\circ is measured from the xx-axis, so the xx-component gets the cosine:

vx=−(8.0 m/s)cos⁡35∘=−6.55 m/s,vy=−(8.0 m/s)sin⁡35∘=−4.59 m/s.v_x = -(8.0\ \text{m/s})\cos 35^\circ = -6.55\ \text{m/s}, \qquad v_y = -(8.0\ \text{m/s})\sin 35^\circ = -4.59\ \text{m/s}.
v⃗=(−6.55 i^−4.59 j^) m/s.\vec{v} = (-6.55\,\hat{i} - 4.59\,\hat{j})\ \text{m/s}.

Check by going back: 6.552+4.592=8.0 m/s\sqrt{6.55^2 + 4.59^2} = 8.0\ \text{m/s}, and measured counterclockwise from +x+x the direction is 180∘+35∘=215∘180^\circ + 35^\circ = 215^\circ. Putting the signs in from the sketch, instead of trusting cos⁡215∘\cos 215^\circ to produce them, is the move that catches quadrant mistakes.

Worked exampleExample 2: the leg that closes the trip

A sailboat leaves its dock and sails 6.0 km6.0\ \text{km} at 30∘30^\circ north of east, then 4.0 km4.0\ \text{km} due north. (a) What single displacement takes it straight back to the dock? Give it in unit-vector notation and as a magnitude and direction. (b) Compare the total distance sailed with the displacement for the whole round trip.

Show solution

(a) Take +x+x east and +y+y north. Resolve each leg:

d⃗1=(6.0cos⁡30∘ i^+6.0sin⁡30∘ j^) km=(5.20 i^+3.00 j^) km,d⃗2=4.00 j^ km.\vec{d}_1 = (6.0\cos 30^\circ\,\hat{i} + 6.0\sin 30^\circ\,\hat{j})\ \text{km} = (5.20\,\hat{i} + 3.00\,\hat{j})\ \text{km}, \qquad \vec{d}_2 = 4.00\,\hat{j}\ \text{km}.

After two legs the boat is at d⃗1+d⃗2=(5.20 i^+7.00 j^) km\vec{d}_1 + \vec{d}_2 = (5.20\,\hat{i} + 7.00\,\hat{j})\ \text{km} from the dock. Returning means undoing that, so the return leg is its negative:

d⃗3=(−5.20 i^−7.00 j^) km.\vec{d}_3 = (-5.20\,\hat{i} - 7.00\,\hat{j})\ \text{km}.

Its magnitude is 5.202+7.002=8.72 km\sqrt{5.20^2 + 7.00^2} = 8.72\ \text{km}. Both components are negative, so it points south of west, at tan⁡−1(7.005.20)=53.4∘\tan^{-1}\left(\frac{7.00}{5.20}\right) = 53.4^\circ south of west.

(b) The distance sailed is 6.0+4.0+8.72=18.7 km6.0 + 4.0 + 8.72 = 18.7\ \text{km}, a scalar that only grows. The displacement for the round trip is d⃗1+d⃗2+d⃗3=0⃗\vec{d}_1 + \vec{d}_2 + \vec{d}_3 = \vec{0}, because the boat ends where it began.

Worked exampleExample 3: how the angle controls the resultant (derivation)

Two displacements each have magnitude LL. The first points along +x+x; the second makes an angle ϕ\phi with the first, measured counterclockwise.

(a) Derive an expression for the magnitude RR of their resultant in terms of LL and ϕ\phi.

(b) Find the angle ϕ\phi for which the resultant has the same magnitude LL as each displacement.

(c) A student claims that the resultant of two equal-length vectors is always longer than either one. Use your expression to evaluate the claim.

Show solution

(a) Write both in components: A⃗=L i^\vec{A} = L\,\hat{i} and B⃗=Lcos⁡ϕ i^+Lsin⁡ϕ j^\vec{B} = L\cos\phi\,\hat{i} + L\sin\phi\,\hat{j}. Add axis by axis:

Rx=L(1+cos⁡ϕ),Ry=Lsin⁡ϕ.R_x = L(1 + \cos\phi), \qquad R_y = L\sin\phi.
R2=L2(1+cos⁡ϕ)2+L2sin⁡2ϕ=L2(1+2cos⁡ϕ+cos⁡2ϕ+sin⁡2ϕ)=2L2(1+cos⁡ϕ),R^2 = L^2(1 + \cos\phi)^2 + L^2\sin^2\phi = L^2\left(1 + 2\cos\phi + \cos^2\phi + \sin^2\phi\right) = 2L^2(1 + \cos\phi),

using cos⁡2ϕ+sin⁡2ϕ=1\cos^2\phi + \sin^2\phi = 1. So R=L2(1+cos⁡ϕ)R = L\sqrt{2(1 + \cos\phi)}. Check the limits: ϕ=0\phi = 0 gives 2L2L (parallel, magnitudes add), ϕ=90∘\phi = 90^\circ gives 2 L\sqrt{2}\,L (the Pythagorean case), and ϕ=180∘\phi = 180^\circ gives 00 (they cancel).

(b) Set R=LR = L: 2(1+cos⁡ϕ)=12(1 + \cos\phi) = 1, so cos⁡ϕ=−12\cos\phi = -\frac{1}{2} and ϕ=120∘\phi = 120^\circ. Tip to tail, the three arrows form an equilateral triangle.

(c) The claim is false. R>LR > L requires 2(1+cos⁡ϕ)>12(1 + \cos\phi) > 1, that is cos⁡ϕ>−12\cos\phi > -\frac{1}{2}, or ϕ<120∘\phi < 120^\circ. For angles between 120∘120^\circ and 180∘180^\circ the resultant is shorter than either vector, because their components along xx largely cancel.

Where students lose points

On the exam

A vector answer needs both parts: unit-vector components with units, or a magnitude with a direction stated relative to an axis or a compass direction ("8.72 km8.72\ \text{km}, 53.4∘53.4^\circ south of west"). When a question asks for a "magnitude", give a positive number and no direction. Answers in one dimension may use a sign for direction, as long as the positive direction is clear from the question or from your work.

Check yourself

  1. Question 1

    Which list contains only vector quantities?

    1. A

      distance, displacement, velocity

    2. B

      position, velocity, acceleration

    3. C

      speed, velocity, acceleration

    4. D

      displacement, speed, time

    Show answer

    B

    Position, velocity and acceleration all need a direction to be complete. Choice A includes distance, and choice C includes speed: both are scalars, since they say how much without saying which way.

  2. Question 2

    A displacement is d⃗=(−5.0 i^+12.0 j^) m\vec{d} = (-5.0\,\hat{i} + 12.0\,\hat{j})\ \text{m}. Give its magnitude and its direction measured counterclockwise from the +x+x axis.

    Show answer

    13.0 m13.0\ \text{m} at 112.6∘112.6^\circ from the +x+x axis (that is, 67.4∘67.4^\circ above the −x-x axis).

    d=5.02+12.02=13.0 md = \sqrt{5.0^2 + 12.0^2} = 13.0\ \text{m}. The inverse tangent of 12.0−5.0\frac{12.0}{-5.0} gives −67.4∘-67.4^\circ, but dx<0d_x < 0 puts the vector in the second quadrant, so add 180∘180^\circ to get 112.6∘112.6^\circ.

  3. Question 3

    Two displacements have magnitudes 3.0 m3.0\ \text{m} and 5.0 m5.0\ \text{m}, in directions you can choose. Which magnitude could their resultant NOT have?

    1. A

      2.0 m2.0\ \text{m}

    2. B

      5.8 m5.8\ \text{m}

    3. C

      8.0 m8.0\ \text{m}

    4. D

      8.5 m8.5\ \text{m}

    Show answer

    D

    The resultant ranges from 5.0−3.0=2.0 m5.0 - 3.0 = 2.0\ \text{m} (opposite directions) to 5.0+3.0=8.0 m5.0 + 3.0 = 8.0\ \text{m} (same direction), so 8.5 m8.5\ \text{m} is impossible. Choice B, 5.8 m5.8\ \text{m}, is what perpendicular vectors give, one possibility among many.

  4. Question 4

    A particle is at r⃗=(6.0 i^−8.0 j^) m\vec{r} = (6.0\,\hat{i} - 8.0\,\hat{j})\ \text{m}. Write the unit vector r^\hat{r} that points from the origin toward the particle.

    Show answer

    r^=0.60 i^−0.80 j^\hat{r} = 0.60\,\hat{i} - 0.80\,\hat{j} (no units).

    Divide the position vector by its magnitude, ∣r⃗∣=6.02+8.02=10.0 m|\vec{r}| = \sqrt{6.0^2 + 8.0^2} = 10.0\ \text{m}. The meters cancel, so r^\hat{r} has no units and a magnitude of exactly 1: 0.602+0.802=1\sqrt{0.60^2 + 0.80^2} = 1.

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