3.1.3 - Estimation of Physical Quantities

3.1.3 - Estimation of Physical Quantities

Estimation uses approximate inputs and a physical model to predict a useful scale. Learn to state reasonable assumptions, keep powers of ten under control, and use a rough answer to test whether a detailed calculation makes sense.

Orders of magnitude and reference scales

An order of magnitude expresses scale using a power of ten. A factor of ten is one order of magnitude; a factor of one thousand is three. Always state the unit: a length of 103 mm10^3\,\mathrm{mm} is the same as 100 m10^0\,\mathrm m.

A value such as 2.0×105 m2.0\times10^5\,\mathrm m is of order 105 m10^5\,\mathrm m. When a task asks for the nearest power of ten, compare multiplicative factors. For 8.0×105 m8.0\times10^5\,\mathrm m, the value is eight times 105 m10^5\,\mathrm m, but only a factor of 1.25 below 106 m10^6\,\mathrm m, so 106 m10^6\,\mathrm m is nearer on a logarithmic scale.

The boundary for this convention is 10≈3.16\sqrt{10}\approx3.16: in a×10na\times10^n, choose 10n10^n below that boundary and 10n+110^{n+1} above it. This is a precise way to interpret “nearest”; an estimate's defensible assumptions matter more than a boundary decision for a poorly known quantity. Avoid throwing away the coefficient until the end of a calculation.

Useful reference scales include:

QuantityApproximate scale
Nuclear diameter10−1510^{-15} to 10−14 m10^{-14}\,\mathrm m
Atomic diameter10−10 m10^{-10}\,\mathrm m
Paper thickness or hair width10−4 m10^{-4}\,\mathrm m
Person's height11 to 2 m2\,\mathrm m
Earth's diameter107 m10^7\,\mathrm m
Earth–Sun distance1011 m10^{11}\,\mathrm m

These are approximate reference values, not exact measurements of every atom, hair or person.

Reading mathematical comparisons

The symbols in a physical statement tell you how strong a claim it makes:

SymbolMeaning and example
==Equal to: 1 cm=10−2 m1\,\mathrm{cm}=10^{-2}\,\mathrm m is an exact unit conversion.
≈\approxApproximately equal to: π≈3\pi\approx3 is a useful estimate, not an exact identity.
<<, >>Less than, greater than: 2 mm<3 mm2\,\mathrm{mm}<3\,\mathrm{mm}, so 3 mm>2 mm3\,\mathrm{mm}>2\,\mathrm{mm}.
≪\ll, ≫\ggMuch less than, much greater than: a 0.1 mm0.1\,\mathrm{mm} sheet thickness is much less than its 200 mm200\,\mathrm{mm} length, so t≪lt\ll l and l≫tl\gg t. There is no universal numerical cutoff; whether a small contribution may be neglected depends on the required accuracy.
∝\proptoProportional to: at fixed width and length, a cuboid's volume obeys V∝hV\propto h. The ratio V/hV/h stays constant, so doubling hh doubles VV.
Δ\DeltaA change in a quantity: Δh=hfinal−hinitial\Delta h=h_{\mathrm{final}}-h_{\mathrm{initial}}. A fall gives a negative change. In an uncertainty expression such as h±Δhh\pm\Delta h, the context instead defines Δh\Delta h as a positive absolute uncertainty.

Compare quantities in the same units before judging their relative size. A small numerical value in metres can be the same physical length as a large value in millimetres.

Choosing a model and reasonable assumptions

A useful estimate answers a clear physical question with assumptions you can explain. Start with the relationship connecting the desired quantity to quantities you can estimate; then choose a simple model and approximate inputs.

For the volume of a classroom, a cuboid model gives V=lwhV=lwh. Dimensions such as 10 m10\,\mathrm m, 8 m8\,\mathrm m and 3 m3\,\mathrm m give V≈240 m3V\approx240\,\mathrm{m^3}. This ignores furniture, but is a reasonable starting estimate of the enclosed volume. A height of 30 m30\,\mathrm m would need a very different building, so it would be a poor default assumption.

Keep one or two significant figures in the inputs rather than rounding every input to a power of ten. Multiplication, and especially squaring or cubing, can magnify early rounding. Calculate with units and round the final estimate to the precision the question asks for. An estimate of 240 m3240\,\mathrm{m^3} and its nearest power 102 m310^2\,\mathrm{m^3} serve different purposes; neither is a claim of exact volume.

Test the assumption that matters most

If the room height could reasonably be between 2.52.5 and 3.5 m3.5\,\mathrm m, keeping the floor dimensions fixed gives volumes from 200200 to 280 m3280\,\mathrm{m^3}. Both remain of order 102 m310^2\,\mathrm{m^3}. This checks that the scale conclusion is robust without pretending the assumptions are measured uncertainties.

State assumptions that influence the result, not irrelevant details. A different sensible assumption can earn full credit when the physical relationship, arithmetic and conclusion remain consistent with it.

Estimating areas and volumes

A geometrical model turns an estimated length into an area or volume, but the power of the length must also apply to its unit and numerical scale.

A circular cross-section

Treat a fine thread with diameter 1.0×10−4 m1.0\times10^{-4}\,\mathrm m as circular. Its radius is 5.0×10−5 m5.0\times10^{-5}\,\mathrm m, so

A=πr2≈3×(5×10−5)2=7.5×10−9 m2.A=\pi r^2\approx3\times(5\times10^{-5})^2 =7.5\times10^{-9}\,\mathrm{m^2}.

The nearest power is 10−8 m210^{-8}\,\mathrm{m^2}. Using the diameter in place of the radius would make the area four times too large. Squaring 10−510^{-5} gives 10−1010^{-10}, not 10−2510^{-25}.

A spherical body

Taking Earth's diameter as 1.3×107 m1.3\times10^7\,\mathrm m, its radius is 6.5×106 m6.5\times10^6\,\mathrm m. A spherical model gives

V=43πr3≈4(6.5×106)3≈1.1×1021 m3.V=\frac43\pi r^3 \approx4(6.5\times10^6)^3 \approx1.1\times10^{21}\,\mathrm{m^3}.

This is of order 1021 m310^{21}\,\mathrm{m^3}. Rounding the radius prematurely to 107 m10^7\,\mathrm m would give roughly 4×1021 m34\times10^{21}\,\mathrm{m^3}, enough to change the nearest-power decision. A rough model does not justify avoidable arithmetic distortion.

Covering every external surface

Surface area estimates how much coating or insulation is needed; volume estimates how much space an object occupies. A rectangular block has three pairs of equal faces, with areas lwlw, lhlh and whwh, so its total surface area is

A=2(lw+lh+wh).A=2(lw+lh+wh).

A box roughly 0.40 m0.40\,\mathrm m by 0.30 m0.30\,\mathrm m by 0.20 m0.20\,\mathrm m needs

A≈2(0.12+0.08+0.06)=0.52 m2A\approx2(0.12+0.08+0.06)=0.52\,\mathrm{m^2}

of film to cover all six faces, or about half a square metre before allowing for overlaps and waste. Using lwhlwh would give cubic metres, the wrong quantity for a covering.

For a closed cylinder, imagine unrolling the curved surface into a rectangle. Its width is the circumference 2πr2\pi r and its height is hh, giving curved area 2πrh2\pi rh. The two circular ends add 2πr22\pi r^2, so

A=2πrh+2πr2.A=2\pi rh+2\pi r^2.

A cylindrical container with radius about 0.30 m0.30\,\mathrm m and height 0.80 m0.80\,\mathrm m therefore needs a coating area of 0.48π+0.18π=0.66π≈2.1 m20.48\pi+0.18\pi=0.66\pi\approx2.1\,\mathrm{m^2}, of order 100 m210^0\,\mathrm{m^2}, for its curved side and both ends. If only the curved side is coated, use 2πrh2\pi rh; if one end is open, include only one circular end. Decide which surfaces are present before substituting numbers.

Estimating mass, rates and accumulated totals

A derived estimate combines approximate values with a physical relationship. The model must connect the inputs to the required quantity, rather than merely producing a large or small number.

Mass of air in a classroom

Using the 240 m3240\,\mathrm{m^3} classroom and an approximate air density ρ≈1.2 kg m−3\rho\approx1.2\,\mathrm{kg\,m^{-3}},

m=ρV≈1.2×240≈290 kg.m=\rho V\approx1.2\times240\approx290\,\mathrm{kg}.

The nearest power is 102 kg10^2\,\mathrm{kg}. Air is much less dense than water, but hundreds of cubic metres still have substantial mass. Furniture and different room dimensions affect the estimate; a few hundred kilograms is a more honest description than an exact mass of 288 kg.

Total from a rate

To estimate the number of heartbeats in a lifetime, suppose the average rate is 70 per minute and the lifetime is 80 years. There are about 5.3×1055.3\times10^5 minutes in a year, so

N≈70×80×5.3×105≈3×109 beats.N\approx70\times80\times5.3\times10^5 \approx3\times10^9\text{ beats}.

The units cancel: beats per minute multiplied by minutes gives beats. The assumed rate is a lifetime average, not a claim that the heart always beats at that rate. Different reasonable assumptions can move the result across a nearest-power boundary; show the working that supports your answer.

Comparing scales and checking an answer

A comparison uses a ratio of quantities expressed in the same unit. If an atomic diameter is about 10−10 m10^{-10}\,\mathrm m and a nuclear diameter about 10−15 m10^{-15}\,\mathrm m, their ratio is 10510^5: the atom is about five orders of magnitude wider. The factor is 10510^5, while the number of orders is 5.

[DIAGRAM: asset_name: 1.3 - Estimation of Physical Quantities - Diagram 1; asset_slug: 1.3 - Estimation of Physical Quantities - Diagram 1; recommended_method: matplotlib; caption: Equal intervals on this length scale represent multiplication by ten.; description: Approximate length scales positioned accurately on a logarithmic axis, with each small interval representing a factor of ten.]
Equal intervals on this length scale represent multiplication by ten.

Equal distances along this logarithmic axis mean equal multiplication factors. Five small intervals represent multiplication by 10510^5, regardless of where you start.

Use a ratio to catch unit errors

A metal block of approximate mass 50 g50\,\mathrm g and volume 6 cm36\,\mathrm{cm^3} has density about 8 g cm−38\,\mathrm{g\,cm^{-3}}. Since 1 g cm−3=103 kg m−31\,\mathrm{g\,cm^{-3}}=10^3\,\mathrm{kg\,m^{-3}}, this is about 8×103 kg m−38\times10^3\,\mathrm{kg\,m^{-3}}. A calculator result of 8×108 kg m−38\times10^8\,\mathrm{kg\,m^{-3}} is larger by 10510^5, so a conversion or power-of-ten error is likely. The estimate identifies the size of the discrepancy; it does not by itself prove which input was wrong.

For ratios not equal to an exact power of ten, state the ratio first. For example, 700 nm/0.1 nm=7000700\,\mathrm{nm}/0.1\,\mathrm{nm}=7000, approximately four orders of magnitude when rounded to the nearest power. The more precise logarithmic difference is log⁡10(7000)≈3.85\log_{10}(7000)\approx3.85; it is unnecessary unless requested. Comparing the actual ratio avoids errors from separately rounding both quantities first.