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The Timpson Lyceum · University Physics I (2025)

Units and Vectors– Lecture 1 (University Physics I)

Overview

This lecture lays the mathematical groundwork for the entire course. It covers how we measure physical quantities (units, metric prefixes, and the discipline of significant figures) and how we represent quantities that have direction (vectors). By the end you should be able to convert between units by treating conversions as multiplication by 1, report answers with the correct precision, and add, scale, and decompose vectors using components and trigonometry. The vector tools introduced here — components, magnitude, the dot product, and the cross product — are used constantly throughout mechanics.

Key Concepts

The three base units (SI). Everything in this course is built from three quantities and their units:

Metric prefixes scale a unit by powers of ten. The ones used most often:

Dimensional analysis (unit consistency). A conversion factor such as 5280 ft1 mi\frac{5280\ \text{ft}}{1\ \text{mi}} equals 1, so multiplying by it changes the units without changing the quantity. Always carry units through a calculation and let them cancel — if the leftover units aren't what you expected, you made a mistake. This is the fastest sanity check available. (Watch cubed units: converting m3\text{m}^3 to cm3\text{cm}^3 requires the factor (100 cm1 m)3\left(\tfrac{100\ \text{cm}}{1\ \text{m}}\right)^3, not just one factor.)

Significant figures communicate how precisely a quantity was measured. Two rules:

Scientific notation writes a number as one nonzero digit before the decimal point times a power of ten, e.g. 6235.3=6.2353×1036235.3 = 6.2353 \times 10^{3}. The number of digits shown should match the significant figures.

Scalars vs. vectors.

Vector operations.

Components and trigonometry. If A⃗\vec{A} has magnitude AA and points at angle θ\theta from the x-axis, then ax=Acos⁡θa_x = A\cos\theta and ay=Asin⁡θa_y = A\sin\theta. Going the other way, the direction is θ=tan⁡−1 ⁣(ayax)\theta = \tan^{-1}\!\left(\dfrac{a_y}{a_x}\right). Tip: when in doubt, redraw the right triangle so the angle of interest sits at a corner, then read off opposite/adjacent directly.

Unit vectors. ı^,ȷ^,k^\hat{\imath}, \hat{\jmath}, \hat{k} point along +x,+y,+z+x, +y, +z and have length 1, so any vector can be written A⃗=axı^+ayȷ^+azk^\vec{A} = a_x\hat{\imath} + a_y\hat{\jmath} + a_z\hat{k}.

Two ways to multiply vectors.

Worked Example

(a) Unit conversion via dimensional analysis. Convert a land-speed record of 763.0 mi/h763.0\ \text{mi/h} to m/s.

  1. Chain conversion factors (each equal to 1) so the unwanted units cancel: 763.0 mih×5280 ft1 mi×12 in1 ft×2.54 cm1 in×1 m100 cm×1 h3600 s.763.0\ \frac{\text{mi}}{\text{h}} \times \frac{5280\ \text{ft}}{1\ \text{mi}} \times \frac{12\ \text{in}}{1\ \text{ft}} \times \frac{2.54\ \text{cm}}{1\ \text{in}} \times \frac{1\ \text{m}}{100\ \text{cm}} \times \frac{1\ \text{h}}{3600\ \text{s}}.
  2. Miles, feet, inches, centimeters, and hours all cancel, leaving m/s.
  3. Evaluating gives 341.0 m/s341.0\ \text{m/s} (4 significant figures, matching 763.0763.0). A quick sanity check — m/s is roughly half of mi/h — predicted "a few hundred," which fits.

(b) Magnitude and direction of a displacement. A skier travels 1.00 km1.00\ \text{km} north and then 2.00 km2.00\ \text{km} east. How far, and in what direction, is she from the start?

  1. The two legs are perpendicular, so the straight-line distance is the hypotenuse: d=(1.00)2+(2.00)2=5≈2.24 km.d = \sqrt{(1.00)^2 + (2.00)^2} = \sqrt{5} \approx 2.24\ \text{km}.
  2. For the direction, measure the angle north of east: θ=tan⁡−1 ⁣(1.002.00)≈26.6∘.\theta = \tan^{-1}\!\left(\frac{1.00}{2.00}\right) \approx 26.6^{\circ}.
  3. So she is 2.24 km2.24\ \text{km} away, 26.6∘26.6^{\circ} north of east — equivalently 63.4∘63.4^{\circ} east of north (the two angles are complementary, summing to 90∘90^{\circ}).

Summary