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How do we add quantities that have direction, and split them into components?

The difference between scalars and vectors, adding vectors by scale diagram and calculation, and resolving a vector into perpendicular components.

A CCEA A-Level Physics answer on the difference between scalars and vectors, adding vectors by scale drawing and by Pythagoras and trigonometry, and resolving a vector into perpendicular components, with worked calculations.

Generated by Claude Opus 4.89 min answer

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  1. What this dot point is asking
  2. Scalars versus vectors
  3. Adding vectors
  4. Resolving a vector
  5. Examples in context
  6. Try this

What this dot point is asking

CCEA wants you to distinguish scalar and vector quantities, add two or more vectors by scale diagram and by calculation, and resolve a single vector into two perpendicular components. This underpins every mechanics topic in AS 1, from equilibrium to projectile motion.

Scalars versus vectors

The practical consequence is that vectors must be combined with regard to their directions. Two forces of 5 N5\ \text{N} acting in the same line add to 10 N10\ \text{N}; the same two forces acting at right angles give a resultant of only about 7.1 N7.1\ \text{N}, and acting in opposite directions they cancel to zero.

Adding vectors

Vectors are added tip to tail: the tail of the second vector is placed at the tip of the first, and the single vector drawn from the start of the first to the end of the last is the resultant. For two perpendicular vectors of magnitudes AA and BB, the resultant magnitude is

R=A2+B2R = \sqrt{A^2 + B^2}

and its direction is θ=tan1 ⁣(BA)\theta = \tan^{-1}\!\left(\frac{B}{A}\right) measured from AA. For non-perpendicular vectors, draw a labelled scale diagram (for example 1 cm10 N1\ \text{cm} \equiv 10\ \text{N}) and measure the resultant's length and bearing with a ruler and protractor.

Resolving a vector

This is the key to inclined-plane and projectile problems, where weight is resolved along and perpendicular to a slope, or velocity is split into horizontal and vertical parts that obey separate equations of motion.

Examples in context

A free-kick in football is struck at 25 m s125\ \text{m s}^{-1} at 4040^{\circ} above the ground. Its horizontal velocity is 25cos40=19.2 m s125\cos 40^{\circ} = 19.2\ \text{m s}^{-1} and its vertical velocity is 25sin40=16.1 m s125\sin 40^{\circ} = 16.1\ \text{m s}^{-1}; the horizontal part stays roughly constant while gravity slows and reverses the vertical part. A plane flying north at 200 m s1200\ \text{m s}^{-1} in a crosswind of 30 m s130\ \text{m s}^{-1} from the west has a resultant ground velocity of 2002+302=202 m s1\sqrt{200^2 + 30^2} = 202\ \text{m s}^{-1} at 8.58.5^{\circ} east of north, which the pilot must correct for to stay on track.

Try this

Q1. A force of 20 N20\ \text{N} acts at 3030^{\circ} above the horizontal. Find its horizontal and vertical components. [2 marks]

  • Cue. Horizontal =20cos3017.3 N= 20\cos 30^{\circ} \approx 17.3\ \text{N}; vertical =20sin30=10 N= 20\sin 30^{\circ} = 10\ \text{N}.

Q2. Two perpendicular displacements of 3 m3\ \text{m} east and 4 m4\ \text{m} north are combined. State the magnitude of the resultant. [1 mark]

  • Cue. 32+42=5 m\sqrt{3^2 + 4^2} = 5\ \text{m}.

Q3. Explain why pulling a heavy case along on a strap at an angle reduces the upward force needed but does not give the largest horizontal pull. [2 marks]

  • Cue. The vertical component FsinθF\sin\theta supports part of the weight, but the useful horizontal component FcosθF\cos\theta shrinks as θ\theta grows; a flat pull gives the largest forward force.

Exam-style practice questions

Practice questions written in the style of CCEA exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

CCEA 20194 marksA boat heads due north across a river at 3.0 m s13.0\ \text{m s}^{-1} while the current carries it due east at 4.0 m s14.0\ \text{m s}^{-1}. Calculate the magnitude and direction of the resultant velocity of the boat.
Show worked answer →

The two velocities are perpendicular, so use Pythagoras for the magnitude:

v=3.02+4.02=9.0+16=25=5.0 m s1v = \sqrt{3.0^2 + 4.0^2} = \sqrt{9.0 + 16} = \sqrt{25} = 5.0\ \text{m s}^{-1}.

The direction is found from the angle east of north:

θ=tan1 ⁣(4.03.0)=53\theta = \tan^{-1}\!\left(\dfrac{4.0}{3.0}\right) = 53^{\circ} east of north.

Markers reward the Pythagoras step, the correct 5.0 m s15.0\ \text{m s}^{-1} result, and a clearly stated direction (an angle measured from a named reference such as north). A bare magnitude with no direction loses the direction mark because velocity is a vector.

CCEA 20213 marksA child pulls a sledge with a rope at 2525^{\circ} above the horizontal with a force of 80 N80\ \text{N}. Determine the horizontal and vertical components of this force.
Show worked answer →

Resolve the force into perpendicular components. The horizontal component is adjacent to the angle, so it uses cosine:

Fx=80cos25=80×0.906=72.5 NF_x = 80 \cos 25^{\circ} = 80 \times 0.906 = 72.5\ \text{N}.

The vertical component is opposite the angle, so it uses sine:

Fy=80sin25=80×0.423=33.8 NF_y = 80 \sin 25^{\circ} = 80 \times 0.423 = 33.8\ \text{N}.

Markers reward correct assignment of cosine to the horizontal component and sine to the vertical component, and the two numerical answers to a sensible number of significant figures. The vertical component reduces the normal contact force on the ground, which is why pulling at an angle eases the sledge along.

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