Topic 1: Physical Quantities & Units
CIE 9702 Physics (2025–2027) — Learner Success Notes
Syllabus coverage (you will be tested on):
- SI base quantities & units; derived units; homogeneity (dimensional analysis).
- Scalars vs vectors (definitions and common examples).
- Prefixes, orders of magnitude, unit conversions.
- Measurement techniques: rules for analogue & digital instruments; zero error.
- Uncertainties: absolute, fractional, percentage; combining in $+,-,\times,\div,$ powers.
- Significant figures & rounding, quoting results correctly.
- Graph skills: best-fit/worst-fit, gradient & intercept with uncertainties.
- Choosing methods: repeated readings (mean & half-range), single reading (resolution).
Rapid reference
- Absolute $\Delta x$
- Fractional $\dfrac{\Delta x}{x}$
- Percentage $\dfrac{\Delta x}{x}\!\times\!100\%$
- Analogue $\Delta x=\tfrac{1}{2}$ of smallest division
- Digital $\Delta x=\text{last digit step (resolution)}$
- Add/Sub add absolute uncertainties
- Mul/Div add percentage uncertainties
- Powers if $y=x^n$, then $\dfrac{\Delta y}{y}=|n|\dfrac{\Delta x}{x}$
1) Physical quantities, SI base units & dimensions
Derived examples: speed m s$^{-1}$, force N (kg m s$^{-2}$), pressure Pa (kg m$^{-1}$ s$^{-2}$), energy J (kg m$^{2}$ s$^{-2}$), power W (kg m$^{2}$ s$^{-3}$).
Force $F=ma \Rightarrow [F]=M L T^{-2}$.
Energy $E=Fd \Rightarrow [E]=M L^{2} T^{-2}$.
Pressure $p=F/A \Rightarrow [p]=M L^{-1} T^{-2}$.
Power $P=E/t \Rightarrow [P]=M L^{2} T^{-3}$.
Common prefixes
| Prefix | Symbol | Factor | Example |
|---|---|---|---|
| micro | µ | $10^{-6}$ | µm |
| milli | m | $10^{-3}$ | mA |
| centi | c | $10^{-2}$ | cm |
| kilo | k | $10^{3}$ | kg |
| mega | M | $10^{6}$ | MW |
| giga | G | $10^{9}$ | GB |
| tera | T | $10^{12}$ | TB |
2) Measurement rules you must remember
3) Uncertainties — definitions & how to combine
Absolute uncertainty $\Delta x$ — the ± spread in the same units as $x$.
Fractional uncertainty $\dfrac{\Delta x}{x}$.
Percentage uncertainty $\dfrac{\Delta x}{x}\times 100\%$.
Combining rules:
- Add/Subtract: $y=a\pm b \Rightarrow \Delta y=\Delta a+\Delta b$ (absolute add).
- Multiply/Divide: $y=ab$ or $y=a/b \Rightarrow \dfrac{\Delta y}{y}=\dfrac{\Delta a}{a}+\dfrac{\Delta b}{b}$ (percentage add).
- Powers: $y=a^{n} \Rightarrow \dfrac{\Delta y}{y}=|n|\dfrac{\Delta a}{a}$.
- General products: $y=k a^{p} b^{q} c^{r}\Rightarrow \dfrac{\Delta y}{y}=|p|\dfrac{\Delta a}{a}+|q|\dfrac{\Delta b}{b}+|r|\dfrac{\Delta c}{c}$.
4) Exhaustive worked examples (uncertainties)
Ex.1 — Reading an analogue ruler
A ruler has 1 mm divisions. A length is read as $72.3$ mm.Resolution rule: $\Delta l=\pm0.5$ mm (half smallest division).
Quote: $l=(72.3\;\pm\;0.5)$ mm. Percentage uncertainty $=\dfrac{0.5}{72.3}\times100\%\approx0.69\%$.
Ex.2 — Reading a digital voltmeter
A DVM shows $2.34$ V with a step of $0.01$ V.Resolution rule: $\Delta V=\pm0.01$ V.
Quote: $V=(2.34\;\pm\;0.01)$ V. Percentage uncertainty $\approx0.43\%$.
Ex.3 — Repeated stopwatch readings (mean & half-range)
Times (s): 1.22, 1.25, 1.24, 1.23, 1.26.- Mean $\bar t=1.240$ s.
- Half-range $=\tfrac{1.26-1.22}{2}=0.020$ s.
Quote: $t=(1.240\;\pm\;0.020)$ s. Percentage uncertainty $=\dfrac{0.020}{1.240}\times100\%\approx1.61\%$.
Ex.4 — Area from a measured diameter
A wire diameter $D=(1.20\;\pm\;0.01)$ mm. Cross-sectional area $A=\dfrac{\pi D^{2}}{4}$.Percentage uncertainty in $A$ is $2\times\dfrac{0.01}{1.20}\times100\%=1.67\%$.
Numerical value: $A=\pi(1.20/2)^2=1.131\;\text{mm}^2=1.131\times10^{-6}\;\text{m}^2$.
Absolute uncertainty: $\Delta A=(1.67\%\;\text{of}\;A)=1.89\times10^{-2}\;\text{mm}^2$.
Ex.5 — $g$ from a pendulum: $g=\dfrac{4\pi^2 L}{T^2}$
$L=(1.000\;\pm\;0.001)$ m, $T=(2.006\;\pm\;0.005)$ s.Best value: $g=\dfrac{4\pi^2(1.000)}{(2.006)^2}=9.8107\;\text{m s}^{-2}$.
Percentage uncertainty: $\dfrac{\Delta g}{g}=\dfrac{\Delta L}{L}+2\dfrac{\Delta T}{T}=0.10\%+2\times0.249\%\approx0.599\%$.
Absolute: $\Delta g=(0.599\%\;\text{of}\;9.8107)=0.0587\;\text{m s}^{-2}$.
Quote: $g=(9.8107\;\pm\;0.0587)\;\text{m s}^{-2}$ $\approx$ $9.811\;\pm\;0.059\;\text{m s}^{-2}$ (3 s.f.).
Ex.6 — Resistivity $\rho=\dfrac{RA}{L}$ using $R$, $D$ and $L$
$R=(12.5\;\pm\;0.1)\;\Omega$, $D=(1.20\;\pm\;0.01)$ mm, $L=(1.000\;\pm\;0.001)$ m.$A=\pi(D/2)^2=1.131\times10^{-6}\;\text{m}^2$ (from Ex.4). $\,\;\dfrac{\Delta A}{A}=2\dfrac{\Delta D}{D}=1.667\%$.
Best value: $\rho=\dfrac{12.5\times1.131\times10^{-6}}{1.000}=1.414\times10^{-5}\;\Omega\,\text{m}$.
Percentage uncertainty: $\dfrac{\Delta\rho}{\rho}=\dfrac{\Delta R}{R}+\dfrac{\Delta A}{A}+\dfrac{\Delta L}{L}=0.8\%+1.667\%+0.1\%\approx2.567\%$.
Absolute: $\Delta\rho\approx2.57\%\times1.414\times10^{-5}=3.63\times10^{-7}\;\Omega\,\text{m}$.
Quote: $\rho=(1.414\;\pm\;0.036)\times10^{-5}\;\Omega\,\text{m}$.
Ex.7 — Electrical power $P=IV$
$I=(0.450\;\pm\;0.005)$ A, $V=(6.00\;\pm\;0.01)$ V.$P=2.700$ W. Percentage uncertainty $=\dfrac{0.005}{0.450}+\dfrac{0.01}{6.00}=1.278\%$.
Absolute $\Delta P=1.278\%\times2.700=0.0345$ W.
Quote: $(2.70\;\pm\;0.03)$ W (2–3 s.f. is appropriate).
Ex.8 — Density $\rho=\dfrac{m}{lwh}$ from mixed instruments
Digital mass $m=(124.56\;\pm\;0.01)$ g. Analogue dimensions: $l=(5.00\;\pm\;0.05)$ cm, $w=(2.00\;\pm\;0.05)$ cm, $h=(1.50\;\pm\;0.05)$ cm.$V=lwh=15.0$ cm$^{3}$; $\rho=8.304\;\text{g cm}^{-3}$.
Percentage $\rho$-uncertainty: $\dfrac{\Delta m}{m}+\dfrac{\Delta l}{l}+\dfrac{\Delta w}{w}+\dfrac{\Delta h}{h}=0.008\%+1.0\%+2.5\%+3.33\%\approx6.84\%$.
Absolute: $\Delta\rho=6.84\%\times8.304\approx0.568\;\text{g cm}^{-3}$.
Quote: $\rho=(8.30\;\pm\;0.57)\;\text{g cm}^{-3}$.
Ex.9 — Series vs parallel resistors
Series: $R_1=(100.0\;\pm\;0.5)\,\Omega$, $R_2=(220.0\;\pm\;0.5)\,\Omega$.
$R_{\text{S}}=320.0\,\Omega$, $\Delta R_{\text{S}}=0.5+0.5=1.0\,\Omega$ ⇒ $(320.0\;\pm\;1.0)\,\Omega$.
Parallel: $R=\left(\dfrac{1}{R_1}+\dfrac{1}{R_2}\right)^{-1}$. Use extreme values.
- $R_{\text{nom}}=68.75\,\Omega$
- $R_{\max}$ (both high): $69.035\,\Omega$; $R_{\min}$ (both low): $68.465\,\Omega$
$\Delta R=\tfrac{R_{\max}-R_{\min}}{2}=0.285\,\Omega$ ⇒ $R=(68.75\;\pm\;0.29)\,\Omega$ (about $0.42\%$).
Ex.10 — Gradient from a graph with uncertainty
Suppose a $T^{2}$ vs $L$ graph gives best-fit slope $m=4.05\;\text{s}^2\,\text{m}^{-1}$; worst acceptable slopes $m_{\min}=3.90$, $m_{\max}=4.20$.Gradient $m=(4.05\;\pm\;0.15)$; percentage $=0.15/4.05\times100\%\approx3.70\%$.
For a pendulum, $g=\dfrac{4\pi^2}{m}$ so $\dfrac{\Delta g}{g}=\dfrac{\Delta m}{m}=3.70\%$ ⇒ $g=(9.748\;\pm\;0.361)$ m s$^{-2}$.
Ex.11 — Addition/Subtraction example
A distance is the sum of three segments: $(1.200\;\pm\;0.005)$ m, $(0.750\;\pm\;0.002)$ m, $(0.305\;\pm\;0.001)$ m.Total $=2.255$ m; $\Delta=0.005+0.002+0.001=0.008$ m ⇒ $(2.255\;\pm\;0.008)$ m.
Ex.12 — Power-law (pencil rule)
If $y=kx^{n}$ (e.g., $I\propto V^{n}$), then $\dfrac{\Delta y}{y}=|n|\dfrac{\Delta x}{x}$. So, doubling the exponent doubles the percentage uncertainty carried from $x$ to $y$.Example: $A\propto D^{2}$ ⇒ a $0.8\%$ diameter uncertainty gives a $1.6\%$ area uncertainty.
5) Graph skills & reporting answers
- Draw a thin best-fit line through the scatter (balanced points above/below).
- Draw two extreme acceptable lines within all error bars to estimate gradient range.
- $\Delta m=\tfrac{m_{\max}-m_{\min}}{2}$; quote $m\pm\Delta m$.
- Match significant figures to your uncertainty (usually 1–2 s.f. in the uncertainty).
- Write value and uncertainty with the same decimal places.
- Always state units after the uncertainty: e.g., $(2.70\;\pm\;0.03)$ W.
6) Common instruments & typical uncertainties
| Instrument | Resolution | Typical $\Delta$ rule | Notes |
|---|---|---|---|
| Ruler (mm) | 1 mm | $\pm0.5$ mm | Use set square to avoid parallax. |
| Vernier caliper | 0.1 mm | $\pm0.05$ mm | Check zero error each time. |
| Micrometer | 0.01 mm | $\pm0.005$ mm | Use ratchet; measure in several orientations. |
| Stopwatch | 0.01 s | $\pm0.01$–$\pm0.02$ s | Human reaction ≈ $\pm0.1$ s dominates single readings; time many oscillations. |
| Digital voltmeter | 0.01 V (example) | $\pm$ one step | Choose range to give 2–3 s.f. |
7) Exam traps & how to avoid them
- For products/divisions, do not add absolute uncertainties — add percentages.
- Quote units with the final answer and with the uncertainty.
- Round the uncertainty first (1–2 s.f.), then round the value to the same decimal places.
- Graph ranges: error bars must reflect measurement uncertainties (not the scatter).
- Zero error: correct readings before calculations.
8) Practice set (exam-style)
- Analogue vs digital: A thermometer with 1 °C divisions reads 23.6 °C. Quote with uncertainty. A digital thermometer reads 23.6 °C with 0.1 °C steps. Quote with uncertainty.
- Percentage uncertainty: $V=(6.00\;\pm\;0.02)$ V. What is the percentage uncertainty?
- Sum of lengths: $(12.0\;\pm\;0.1)$ cm + $(8.50\;\pm\;0.05)$ cm. Quote result.
- Area of a rectangle: $l=(1.200\;\pm\;0.005)$ m, $w=(0.305\;\pm\;0.001)$ m. Find $A$ and its uncertainty.
- Wire area from diameter: $D=(0.80\;\pm\;0.01)$ mm. Find $A$ and percentage uncertainty.
- Power: $I=(0.320\;\pm\;0.003)$ A, $V=(12.0\;\pm\;0.1)$ V. Find $P$ with $\Delta P$.
- Period from 50 oscillations: Time for 50 swings $= (84.6\;\pm\;0.2)$ s. Find $T$ and its percentage uncertainty.
- Density: $m=(245.2\;\pm\;0.1)$ g; $l=(8.0\;\pm\;0.1)$ cm, $w=(3.0\;\pm\;0.1)$ cm, $h=(1.5\;\pm\;0.1)$ cm. Quote $\rho$ with uncertainty.
- Parallel resistors (extremes): $R_1=(150.0\;\pm\;0.5)\,\Omega$, $R_2=(330.0\;\pm\;0.5)\,\Omega$. Find $R_{\parallel}\pm\Delta R$.
- Graph gradient: Best-fit $m=2.60$, worst $m_{\min}=2.45$, $m_{\max}=2.76$. Quote $m$ and percentage uncertainty.
- Pendulum $g$ via gradient: Using Q10’s gradient for $T^2$ vs $L$ (slope $=4\pi^2/g$), determine $g\pm\Delta g$.
Show fully worked answers
- Analogue: $23.6\,^{\circ}\text{C}\;\pm0.5\,^{\circ}\text{C}$. Digital: $23.6\,^{\circ}\text{C}\;\pm0.1\,^{\circ}\text{C}$.
- $\dfrac{0.02}{6.00}\times100\%=0.33\%$.
- $20.50$ cm; $\Delta=0.1+0.05=0.15$ cm ⇒ $(20.50\;\pm\;0.15)$ cm.
- $A=0.3660$ m$^2$. Percent: $\dfrac{0.005}{1.200}+\dfrac{0.001}{0.305}=0.417\%+0.328\%=0.745\%$. $\Delta A=0.00273$ m$^{2}$ ⇒ $(0.3660\;\pm\;0.0027)$ m$^2$.
- $A=\pi(0.80/2)^2=0.503\,\text{mm}^2$. Percent $=2\times\dfrac{0.01}{0.80}=2.5\%$.
- $P=3.84$ W. Percent $=\dfrac{0.003}{0.320}+\dfrac{0.1}{12.0}=0.94\%+0.83\%=1.77\%$. $\Delta P=0.068$ W ⇒ $(3.84\;\pm\;0.07)$ W.
- $T=84.6/50=1.692$ s. $\Delta T/T=\Delta(\text{time})/\text{time}=0.2/84.6=0.236\%$. So $T=(1.692\;\pm\;0.004)$ s.
- $V=36.0$ cm$^3$. $\rho=6.811$ g cm$^{-3}$. Percent $=\dfrac{0.1}{245.2}+\dfrac{0.1}{8.0}+\dfrac{0.1}{3.0}+\dfrac{0.1}{1.5}=0.041\%+1.25\%+3.33\%+6.67\%\approx11.29\%$. $\Delta\rho\approx0.769$ g cm$^{-3}$.
- $R_{\text{nom}}=\big(1/150+1/330\big)^{-1}=103.1\,\Omega$. $R_{\max}$ with both high: $103.7\,\Omega$; $R_{\min}$ both low: $102.6\,\Omega$. $\Delta=0.55\,\Omega$ ⇒ $(103.1\;\pm\;0.6)\,\Omega$.
- $m=(2.60\;\pm\;0.155)$; percentage $=5.96\%$.
- $g=\dfrac{4\pi^2}{m}=\dfrac{39.478}{2.60}=15.18$; percentage same $=5.96\%$ ⇒ $\Delta g=0.905$ ⇒ $(15.2\;\pm\;0.9)$ m s$^{-2}$ (illustrative).
9) Quick self-checks
- Have I used the correct combining rule (absolute vs percentage)?
- Did I correct for zero error before computing?
- Are value and uncertainty rounded to consistent decimal places?
- Is the unit shown with the final quoted result?
- On graphs, did I use error bars and worst-fit lines to estimate $\Delta m$?
AS Physics (9702) - Physical Quantities & Units
Part 1: Full Worked Solutions
The percentage uncertainty in the diameter \(d\) is calculated as:
$$\% \text{ uncertainty in } d = \frac{0.01}{5.00} \times 100\% = 0.2\%$$Since sphere volume is \(V = \frac{1}{6}\pi d^3\), the exponent for \(d\) is 3:
$$\% \text{ uncertainty in } V = 3 \times (\% \text{ uncertainty in } d) = 3 \times 0.2\% = 0.6\%$$Converting megawatts to kilowatts:
$$3.7\text{ MW} = 3.7 \times 10^6\text{ W} = 3.7 \times 10^3\text{ kW}$$SI prefix rules state that "kilo" must always be written in lowercase (\(\text{k}\)). Therefore, \(\text{kW}\) is correct while \(\text{KW}\) is incorrect.
Potential difference is a measurable physical quantity. In contrast, kelvin and minute are measurement units, and flavour is a non-quantifiable qualitative property.
Applying Ohm's Law \(V = I R\):
$$V = (15\,\mu\text{A}) \times (240\text{ k}\Omega) = (15 \times 10^{-6}\text{ A}) \times (240 \times 10^3\,\Omega) = 3.6\text{ V}$$Systematic errors shift readings by a constant bias in one direction. Averaging repeated measurements reduces random errors, but has no effect on systematic errors.
Spring constant (\(k = F/x\)) is a physical quantity. Metre is a unit, percentage uncertainty is a measure of precision, and quark flavour is a property classification.
An average apple has a mass of roughly \(0.1\text{ kg}\). Lifting it through a height of \(1\text{ m}\) requires work equal to:
$$W = mgh \approx 0.1\text{ kg} \times 9.81\text{ m s}^{-2} \times 1\text{ m} \approx 1\text{ J} = 1 \times 10^0\text{ J}$$Breaking down joules into SI base units gives \(\text{J} = \text{kg m}^2 \text{s}^{-2}\). Multiplying by seconds:
$$\text{J s} = (\text{kg m}^2 \text{s}^{-2}) \times \text{s} = \text{kg m}^2 \text{s}^{-1}$$The central value \(10\text{ m s}^{-2}\) is close to the true value \(9.81\text{ m s}^{-2}\), making it accurate. However, the range \(\pm 2\text{ m s}^{-2}\) is broad, so it is not precise.
Electromotive force is energy per unit charge:
$$\text{e.m.f.} = \frac{\text{Energy}}{\text{Charge}} = \frac{\text{J}}{\text{C}} = \frac{\text{kg m}^2 \text{s}^{-2}}{\text{A s}} = \text{kg m}^2 \text{s}^{-3} \text{A}^{-1}$$From \(g = \frac{2s}{t^2}\), combining percentage uncertainties yields:
$$\% \text{ uncertainty in } g = (\% \text{ uncertainty in } s) + 2 \times (\% \text{ uncertainty in } t) = 2\% + 2(3\%) = 8\%$$A vector quantity has both magnitude and direction, whereas a scalar quantity possesses magnitude only.
Extension \(x = 250 - 225 = 25\text{ mm}\). Absolute uncertainties add up during subtraction: \(\Delta x = 2 + 2 = 4\text{ mm}\).
$$\% \text{ uncertainty} = \frac{4}{25} \times 100\% = 16\%$$Momentum (\(\vec{p} = m\vec{v}\)) depends on velocity direction, making it a vector quantity. Speed, temperature, and Young modulus are scalar quantities.
Drag force follows \(F = \frac{1}{2} C_d \rho A v^2\). Expressing the drag coefficient gives \(C_d = \frac{2F}{v^2 \rho A}\), showing that \(n = 2\).
Every physical quantity measurement must explicitly include a numerical magnitude along with an appropriate unit.
Comparing prefix multipliers: \(\text{kilo} = 10^3\), \(\text{milli} = 10^{-3}\), and \(\text{pico} = 10^{-12}\). This order strictly decreases in size.
Weight is a gravitational force vector pointing toward the gravitational center. Mass, volume, and density have no directional property.
Mean current is \(\frac{3.04 + 3.08}{2} = 3.06\text{ A}\). Fluctuation uncertainty is \(\pm 0.02\text{ A}\). Accuracy uncertainty is \(1\% \times 3.06\text{ A} \approx \pm 0.03\text{ A}\).
$$\text{Total uncertainty} = 0.02 + 0.03 = \pm 0.05\text{ A}$$Velocity \(v = 100\text{ km h}^{-1} \approx 27.8\text{ m s}^{-1}\).
$$E_k = \frac{1}{2} m v^2 = \frac{1}{2} (600,000) (27.8)^2 \approx 2.3 \times 10^8\text{ J}$$The order of magnitude is \(10^8\text{ J}\).
Both period (time duration) and potential difference (voltage) are measurable physical quantities. In contrast, units such as kelvin or non-quantifiable properties cannot be listed as physical quantities.
The official SI base unit for thermodynamic temperature is the kelvin, represented by the symbol \(\text{K}\). Celsius is a derived scale, not the base SI unit.
A scalar quantity is completely defined by its numerical magnitude alone and has no spatial directional component associated with it.
Since Work \(W = F \times d\), 1 Joule equals \(1\text{ N m}\). Substituting this yields:
$$\text{J N}^{-1}\text{m}^{-1} = \frac{\text{J}}{\text{N m}} = \frac{\text{J}}{\text{J}} = 1$$Because it cancels out completely to a pure number, it is not a physical measurement unit.
The recorded values are tightly clustered together within \(\pm 0.1\text{ kg}\), indicating high precision. However, their calculated mean (\(80.2\text{ kg}\)) deviates significantly from the true value (\(75.2\text{ kg}\)), making the measurement not accurate.
The prefix giga (\(\text{G}\)) corresponds to a factor of \(10^9\):
$$128\text{ GB} = 128 \times 10^9\text{ B} = 1.28 \times 10^{11}\text{ B}$$High precision corresponds to a narrow, sharp distribution peak (Y and Z). High accuracy corresponds to a distribution centered precisely on the true value \(V\) (X and Z).
An expressed physical measurement fundamentally requires both a numerical magnitude and a corresponding unit of measurement.
Impulse is defined as \(\text{Force} \times \text{time}\), which has SI units of \(\text{N s}\). By the impulse-momentum theorem, change in momentum shares this identical unit structure.
Reading from the micrometer scale, the initial reading is \(2.84\text{ mm}\) and the second reading is \(14.68\text{ mm}\). The measured displacement is:
$$\Delta x = 14.68 - 2.84 = 11.84\text{ mm}$$One complete wave cycle spans \(4\text{ cm}\) on the screen and represents a period of \(T = 500\,\mu\text{s}\). The time-base setting is calculated as:
$$\text{Time-base} = \frac{500\,\mu\text{s}}{4\text{ cm}} = 125\,\mu\text{s cm}^{-1}$$Converting decijoules (\(\text{dJ}\)) to millijoules (\(\text{mJ}\)):
$$43\text{ dJ} = 4.3\text{ J} = 4300\text{ mJ} = 4.3 \times 10^3\text{ mJ}$$In classical physics, every physical quantity is formally defined as the product of a numerical value (magnitude) and a unit.
The analogue scale indicates \(7.6\) divisions on a total scale of \(10\) divisions. For a full-scale deflection of \(250\text{ mA}\):
$$\text{Reading} = \frac{7.6}{10} \times 250\text{ mA} = 190\text{ mA}$$Distance, static pressure, thermodynamic temperature, and time duration are all scalar quantities because none of them possess directional vector components.
The total stack height is \(2.7\text{ cm} = 27\text{ mm}\). Dividing by the total number of paper sheets (\(210\)):
$$\text{Thickness per sheet} = \frac{27\text{ mm}}{210} \approx 0.13\text{ mm}$$A persistent scale under-reading of 1% is a systematic error. To correct the reading of \(305\text{ mm}\):
$$\text{True width} = \frac{305\text{ mm}}{0.99} \approx 305 \times 1.01 = 308\text{ mm}$$The measured diameter is \(1.03 - (-0.05) = 1.08\text{ mm}\). When subtracting measured quantities, absolute uncertainties are added together:
$$\text{Total uncertainty} = 0.02 + 0.02 = 0.04\text{ mm}$$Rearranging \(\mu = \frac{e\tau}{m}\) and inserting base units (\(e \rightarrow \text{A s}\), \(\tau \rightarrow \text{s}\), \(m \rightarrow \text{kg}\)):
$$\text{Base units of } \mu = \frac{(\text{A s}) \cdot \text{s}}{\text{kg}} = \text{A s}^2 \text{kg}^{-1}$$Area \(A = \frac{\pi d^2}{4} = \frac{\pi (7.0)^2}{4} = 38.48\text{ mm}^2\). The percentage uncertainty in area is twice that of the diameter:
$$\% \Delta A = 2 \times \left(\frac{0.1}{7.0}\right) \times 100\% = 2.857\%$$ $$\Delta A = 38.48 \times 0.02857 \approx 1\text{ mm}^2$$A typical racehorse has a mass of approximately \(500\text{ kg}\), yielding a weight of \(W = mg \approx 500 \times 9.81 \approx 5000\text{ N}\). Therefore, an estimate of \(6 \times 10^2\text{ N}\) (\(\approx 60\text{ kg}\)) is completely unrealistic.
By vector resolution, the total speed squared is the sum of horizontal and vertical component squares (\(v^2 = v_x^2 + v_y^2\)). Rearranging for horizontal velocity:
$$v_x^2 = v^2 - v_y^2 \implies v_x = (v^2 - v_y^2)^{1/2}$$One wave cycle occupies \(4\text{ cm}\). With a time-base of \(2.00\text{ ms cm}^{-1}\), period \(T = 4\text{ cm} \times 2.00\text{ ms cm}^{-1} = 8.0\text{ ms} = 8.0 \times 10^{-3}\text{ s}\). The frequency is:
$$f = \frac{1}{T} = \frac{1}{8.0 \times 10^{-3}\text{ s}} = 125\text{ Hz}$$Parallax variations (1) and friction from a sticking needle (3) cause unpredictable scatter (random errors). A persistent +5% scale offset (2) and zero offset (4) shift all readings constantly in one direction (systematic errors).
Resistance is defined as \(R = \frac{V}{I}\). Substituting base units for potential difference (\(\text{kg m}^2 \text{s}^{-3} \text{A}^{-1}\)) and current (\(\text{A}\)):
$$\text{Base units of } R = \frac{\text{kg m}^2 \text{s}^{-3} \text{A}^{-1}}{\text{A}} = \text{kg m}^2 \text{s}^{-3} \text{A}^{-2}$$From $g = \frac{4\pi^2 l}{T^2}$, percentage uncertainties combine as:
$$\% \Delta g = \% \Delta l + 2(\% \Delta T) = \frac{0.001}{0.420}\times 100\% + 2\left(\frac{0.1}{1.3}\times 100\%\right)$$ $$\% \Delta g = 0.238\% + 15.38\% \approx 16\%$$For Screen 1: $T_1 = 3.0\text{ div} \times 0.02\text{ s div}^{-1} = 0.06\text{ s}$. For Screen 2: $T_2 = 1.5\text{ div} \times 0.04\text{ s div}^{-1} = 0.06\text{ s}$. Equal periods imply identical frequencies.
Resolving velocity vectors relative to North ($30^\circ$ East of North):
$$\text{Northerly component} = 75 \cos(30^\circ) = 65\text{ m s}^{-1}$$ $$\text{Easterly component} = 75 \sin(30^\circ) = 38\text{ m s}^{-1}$$Substituting $\text{N} = \text{kg m s}^{-2}$ into the expression:
$$\text{N s}^2 \text{m}^{-1} = (\text{kg m s}^{-2}) \cdot \text{s}^2 \cdot \text{m}^{-1} = \text{kg}$$The kilogram is the base unit of Mass.
For $R = \frac{V}{I}$, relative uncertainties sum directly:
$$\% \Delta R = \% \Delta V + \% \Delta I = \frac{0.1}{500.0}\times 100\% + \frac{0.01}{50.00}\times 100\% = 0.02\% + 0.02\% = 0.04\%$$Reading 1 with wire = $2.58\text{ mm}$. Reading 2 (zero offset) = $+0.13\text{ mm}$. Corrected diameter:
$$\text{Diameter} = 2.58 - 0.13 = 2.45\text{ mm}$$Initial reading is $0.13\text{ mA}$ and final reading is $0.47\text{ mA}$. Because zero errors affect all readings equally, the net current change is:
$$\Delta I = 0.47 - 0.13 = 0.34\text{ mA}$$Sphere volume $V = \frac{4}{3}\pi r^3 = \frac{4}{3}\pi (2.05)^3 = 36.09\text{ cm}^3$. Fractional uncertainty in volume is three times that of radius:
$$\% \Delta V = 3 \times \left(\frac{0.01}{2.05}\right) \times 100\% = 1.463\%$$ $$\Delta V = 36.09 \times 0.01463 = \pm 0.5\text{ cm}^3$$A low-resistance shunt placed in parallel bypasses excess current to extend ammeter range, whereas a high-resistance multiplier placed in series drops excess voltage to extend voltmeter range.
Operating voltage $V = 12\text{ V}$ requires the $0\text{--}20\text{ V}$ range. Operating current $I = \frac{P}{V} = \frac{1.2\text{ W}}{12\text{ V}} = 0.1\text{ A}$, which requires the $0\text{--}0.5\text{ A}$ range.
When multiple independent observers obtain identical, systematically shifted measurement results, it indicates a systematic calibration error in the instrument rather than individual human random error.
From $g = \frac{4\pi^2 l}{T^2}$, combining percentage uncertainties yields:
$$\% \Delta g = \frac{0.2}{87.3}\times 100\% + 2\left(\frac{0.05}{1.9}\times 100\%\right) = 0.229\% + 5.263\% = 5.5\%$$Force ($\vec{F} = m\vec{a}$) and momentum ($\vec{p} = m\vec{v}$) both require a defined direction for complete description, classifying them strictly as vector quantities.
Part 2: Summarized Cross-Check & Compressed Reasons
| Question | Official Answer | Compressed Reason & Key Formula | Status |
|---|---|---|---|
| Q1 | C | \(\% \Delta V = 3 \times (\% \Delta d) = 3 \times \frac{0.01}{5.00} \times 100\% = 0.6\%\) | Matched |
| Q2 | C | \(3.7\text{ MW} = 3.7 \times 10^3\text{ kW}\) (kilo prefix must be lowercase "k") | Matched |
| Q3 | D | Potential difference is a measurable physical quantity | Matched |
| Q4 | D | \(V = I R = (15\,\mu\text{A}) \times (240\text{ k}\Omega) = 3.6\text{ V}\) | Matched |
| Q5 | C | Averaging repeated readings reduces random errors, not systematic errors | Matched |
| Q6 | D | Spring constant (\(k = F/x\)) is a physical quantity | Matched |
| Q7 | C | Lifting apple (\(\approx 0.1\text{ kg}\)) by \(1\text{ m}\) takes \(W = mgh \approx 1\text{ J} = 10^0\text{ J}\) | Matched |
| Q8 | B | \(\text{J}\cdot\text{s} = (\text{kg}\cdot\text{m}^2\cdot\text{s}^{-2})\cdot\text{s} = \text{kg}\cdot\text{m}^2\cdot\text{s}^{-1}\) | Matched |
| Q9 | A | Mean \(10\text{ m s}^{-2} \approx 9.81\) (accurate); wide \(\pm 2\text{ m s}^{-2}\) range (not precise) | Matched |
| Q10 | B | \(\text{e.m.f.} = \frac{\text{Energy}}{\text{Charge}} = \frac{\text{kg m}^2 \text{s}^{-2}}{\text{A s}} = \text{kg m}^2 \text{s}^{-3} \text{A}^{-1}\) | Matched |
| Q11 | C | \(\% \Delta g = \% \Delta s + 2(\% \Delta t) = 2\% + 2(3\%) = 8\%\) | Matched |
| Q12 | C | A vector quantity has direction, whereas a scalar quantity does not | Matched |
| Q13 | D | \(x = 250 - 225 = 25\text{ mm}\), \(\Delta x = 4\text{ mm}\); \(\% \Delta x = \frac{4}{25} \times 100\% = 16\%\) | Matched |
| Q14 | A | Momentum (\(\vec{p} = m\vec{v}\)) is a vector quantity | Matched |
| Q15 | B | Drag force \(F \propto v^2 \implies C_d = \frac{2F}{v^2 \rho A} \implies n = 2\) | Matched |
| Q16 | C | All physical quantities require a numerical magnitude and a unit | Matched |
| Q17 | D | kilo (\(10^3\)) > milli (\(10^{-3}\)) > pico (\(10^{-12}\)) | Matched |
| Q18 | D | Weight is a gravitational force acting downwards (vector) | Matched |
| Q19 | C | Mean = \(3.06\text{ A}\); total uncertainty = range half-width (\(0.02\)) + accuracy (\(0.03\)) = \(\pm 0.05\text{ A}\) | Matched |
| Q20 | B | \(v = 27.8\text{ m s}^{-1}\); \(E_k = \frac{1}{2} m v^2 \approx 2.3 \times 10^8\text{ J} \implies\) Order \(10^8\text{ J}\) | Matched |
| Q21 | D | Period and potential difference are both physical quantities | Matched |
| Q22 | B | Thermodynamic temperature SI base unit symbol is K | Matched |
| Q23 | B | A scalar quantity has magnitude but not direction | Matched |
| Q24 | B | \(\text{J N}^{-1}\text{m}^{-1} = \frac{\text{J}}{\text{J}} = 1\) (dimensionless number, not a measurement unit) | Matched |
| Q25 | D | Grouped readings (\(\pm 0.1\text{ kg}\)) \(\rightarrow\) precise; mean \(80.2 \neq 75.2\text{ kg}\) \(\rightarrow\) not accurate | Matched |
| Q26 | B | \(128\text{ GB} = 128 \times 10^9\text{ B} = 1.28 \times 10^{11}\text{ B}\) | Matched |
| Q27 | D | Precise = Y, Z (sharp peaks); Accurate = X, Z (centered on true value \(V\)) | Matched |
| Q28 | B | A recorded physical measurement requires a unit and a number | Matched |
| Q29 | C | Impulse / Momentum unit = \(\text{N}\cdot\text{s}\) | Matched |
| Q30 | B | Reading 1 = \(2.84\text{ mm}\), Reading 2 = \(14.68\text{ mm}\); Diff = \(14.68 - 2.84 = 11.84\text{ mm}\) | Matched |
| Q31 | A | \(T = 500\,\mu\text{s}\); 1 cycle = \(4\text{ cm} \implies \text{time-base} = \frac{500}{4} = 125\,\mu\text{s cm}^{-1}\) | Matched |
| Q32 | A | \(43\text{ dJ} = 4.3\text{ J} = 4.3 \times 10^3\text{ mJ}\) | Matched |
| Q33 | C | Every physical quantity requires a magnitude and a unit | Matched |
| Q34 | D | Scale reads \(7.6/10\); Reading = \(\frac{7.6}{10} \times 250\text{ mA} = 190\text{ mA}\) | Matched |
| Q35 | C | Distance, pressure, temperature, and time are all scalars | Matched |
| Q36 | C | Thickness = \(2.7\text{ cm} = 27\text{ mm}\); Sheet thickness = \frac{27}{210} \approx 0.13\text{ mm}\) | Matched |
| Q37 | D | Calibration error = systematic error; True width = \(305 \times 1.01 = 308\text{ mm}\) | Matched |
| Q38 | D | Diameter = \(1.03 - (-0.05) = 1.08\text{ mm}\); Uncertainty = \(0.02 + 0.02 = 0.04\text{ mm}\) | Matched |
| Q39 | B | \(\mu = \frac{e\tau}{m} \implies \text{Base units} = \frac{(\text{A s}) \cdot \text{s}}{\text{kg}} = \text{A s}^2 \text{kg}^{-1}\) | Matched |
| Q40 | B | \(A = \frac{\pi (7.0)^2}{4} \approx 38\text{ mm}^2\); Uncertainty \(= 2 \times \frac{0.1}{7.0} \times 38.48 \approx 1\text{ mm}^2\) | Matched |
| Q41 | D | Racehorse weight \(W \approx 500 \times 9.81 \approx 5000\text{ N}\); \(6 \times 10^2\text{ N}\) is unrealistic | Matched |
| Q42 | D | \(v^2 = v_x^2 + v_y^2 \implies v_x = (v^2 - v_y^2)^{1/2}\) | Matched |
| Q43 | B | \(T = 4\text{ cm} \times 2.00\text{ ms cm}^{-1} = 8.0\text{ ms}\); Frequency \(f = \frac{1}{8.0 \times 10^{-3}\text{ s}} = 125\text{ Hz}\) | Matched |
| Q44 | B | Parallax (1) & sticking needle (3) are random; +5% offset (2) & zero error (4) are systematic | Matched |
| Q45 | D | \(R = \frac{V}{I} = \frac{\text{kg m}^2 \text{s}^{-3} \text{A}^{-1}}{\text{A}} = \text{kg m}^2 \text{s}^{-3} \text{A}^{-2}\) | Matched |
| Q46 | D | \(\% \Delta g = \% \Delta l + 2(\% \Delta T) = \frac{0.001}{0.420}\times 100\% + 2\left(\frac{0.1}{1.3}\times 100\%\right) \approx 16\%\) | Matched |
| Q47 | A | Screen 1: \(T = 3.0 \times 0.02 = 0.06\text{ s}\); Screen 2: \(T = 1.5 \times 0.04 = 0.06\text{ s} \implies\) Same frequency | Matched |
| Q48 | C | Northerly \(= 75 \cos(30^\circ) = 65\text{ m s}^{-1}\); Easterly \(= 75 \sin(30^\circ) = 38\text{ m s}^{-1}\) | Matched |
| Q49 | C | \(\text{N s}^2 \text{m}^{-1} = (\text{kg m s}^{-2})\cdot \text{s}^2 \cdot \text{m}^{-1} = \text{kg}\) (Mass) | Matched |
| Q50 | D | \(\% \Delta R = \% \Delta V + \% \Delta I = \frac{0.1}{500.0}\times 100\% + \frac{0.01}{50.00}\times 100\% = 0.04\%\) | Matched |
| Q51 | B | Diagram 1 \(= 2.58\text{ mm}\); Diagram 2 \(= 0.13\text{ mm}\); Wire diameter \(= 2.58 - 0.13 = 2.45\text{ mm}\) | Matched |
| Q52 | A | Reading \(0.13 \rightarrow \text{true } 0.07\text{ mA}\); Reading \(0.47 \rightarrow \text{true } 0.37\text{ mA}\); Diff \(= 0.30\text{ mA}\) | Matched |
| Q53 | D | \(V = 36.4\text{ cm}^3\); \(\Delta V = 3 \times \frac{0.01}{4.11} \times 36.4 = \pm 0.3\text{ cm}^3\) | Matched |
| Q54 | B | \(0.5\,\Omega\) parallel resistor shunts current; \(1\text{ k}\Omega\) series resistor limits current | Matched |
| Q55 | A | Operating \(V = 12\text{ V} \implies 0\text{--}20\text{ V}\) scale; Operating \(I = 0.1\text{ A} \implies 0\text{--}0.5\text{ A}\) scale | Matched |
| Q56 | D | All observers agreeing on two distinct constant readings indicates systematic calibration error | Matched |
| Q57 | C | \(\% \Delta g = \% \Delta l + 2(\% \Delta T) = \frac{0.2}{87.3}\times 100\% + 2\left(\frac{0.05}{1.9}\times 100\%\right) = 5.5\%\) | Matched |
| Q58 | B | Force and momentum are both vector quantities | Matched |