The International System of Units — Question 3

Section 1-2 · Physics pages 36–37

Question 3 A unit check can reject a formula, but can it prove one? A cart starts from rest. For this idealized experiment its acceleration a is constant and its displace- ment after elapsed time t is known independently to obey x = 1 2at2. Use [x] = m, [a] = m s−2, and [t] = s. Three software routines propose A: x = at, B: x = at2, C: x = at2 + b. t x at2 1 2at2 Both curves have dimensions of length; dimensions do not fix the coefficient. (a) Which routines can be rejected by units alone? What unit must b have for C to pass a unit check? (b) With a = 2.0 m s−2 and t = 3.0 s, compare B with the stated physical relation. Explain what this establishes about unit checks. (c) Suppose C uses one fixed value of b. Can it reproduce the stated relation both at t = 0 and at t = 3.0 s? Justify without assuming that dimensional consistency guarantees the answer. This is an exercise in evaluating equations, not a request to derive the motion law. Treat the given values as exact within the model.
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Question 3 - Solution A unit check can reject a formula, but can it prove one? t x at2 1 2at2 (a) Check products and sums separately. [at] = m s−1, [at2] = m, [b] = m. Routine A gives [at] = m s−1, a speed unit rather than a displacement unit, so A fails. In B, [at2] = m, so B passes a unit check. For C, the first term has unit metre. Quantities being added must have compatible dimensions; hence [b] = m . With this choice C passes the unit check, although its physical validity remains untested. The number zero can represent a zero displacement; it does not require adding a new kind of quantity. (b) Test the numerical coefficient. The supplied physical relation gives x = 1 2(2.0)(3.0)2 m = 9.0 m , whereas B gives 18.0 m. The factor 1/2 has no units, so unit analysis cannot detect its absence. Dimensional consistency is necessary for a physically meaningful equation in this form, but it is not sufficient to establish the physical law. (c) Test one parameter at two times. b t=0 = 0, b t=3 s = 9 m −18 m = −9 m. At t = 0, the stated displacement is zero. Routine C then requires b = 0 m. At t = 3.0 s, C would consequently predict 18.0 m, not 9.0 m. Alternatively, fitting only the latter time would require b = −9.0 m, which fails at t = 0. No single constant b satisfies both conditions. A constant offset cannot correct this time-dependent error in the coefficient of t2.

Question 3

A unit check can reject a formula, but can it prove one?

A cart starts from rest. For this idealized experiment its acceleration aa is constant and its displacement after elapsed time tt is known independently to obey x=12at2.x=\tfrac12 at^2. Use [x]=m[x]=\mathrm{m}, [a]=ms−2[a]=\mathrm{m\,s^{-2}}, and [t]=s[t]=\mathrm{s}. Three software routines propose A: x=at,B: x=at2,C: x=at2+b.\text{A: }x=at,\qquad \text{B: }x=at^2,\qquad \text{C: }x=at^2+b.

Diagram shown in the original SVG worksheet.

  1. Which routines can be rejected by units alone? What unit must bb have for C to pass a unit check?

  2. With a=2.0ms−2a=2.0\ \mathrm{m\,s^{-2}} and t=3.0st=3.0\ \mathrm{s}, compare B with the stated physical relation. Explain what this establishes about unit checks.

  3. Suppose C uses one fixed value of bb. Can it reproduce the stated relation both at t=0t=0 and at t=3.0st=3.0\ \mathrm{s}? Justify without assuming that dimensional consistency guarantees the answer.

This is an exercise in evaluating equations, not a request to derive the motion law. Treat the given values as exact within the model.

Question 3 - Solution

A unit check can reject a formula, but can it prove one?

Diagram shown in the original SVG worksheet.

(a) Check products and sums separately.

[at]=ms−1,[at2]=m,[b]=m.[at]=\mathrm{m\,s^{-1}},\qquad[at^2]=\mathrm m,\qquad[b]=\mathrm m.

Routine A gives [at]=ms−1[at]=\mathrm{m\,s^{-1}}, a speed unit rather than a displacement unit, so A fails. In B, [at2]=m[at^2]=\mathrm{m}, so B passes a unit check.

For C, the first term has unit metre. Quantities being added must have compatible dimensions; hence [b]=m\boxed{[b]=\mathrm{m}}. With this choice C passes the unit check, although its physical validity remains untested. The number zero can represent a zero displacement; it does not require adding a new kind of quantity.

(b) Test the numerical coefficient.

The supplied physical relation gives x=12(2.0)(3.0)2m=9.0m,x=\tfrac12(2.0)(3.0)^2\ \mathrm{m}=\boxed{9.0\ \mathrm{m}}, whereas B gives 18.0m18.0\ \mathrm{m}. The factor 1/21/2 has no units, so unit analysis cannot detect its absence. Dimensional consistency is necessary for a physically meaningful equation in this form, but it is not sufficient to establish the physical law.

(c) Test one parameter at two times.

b|t=0=0,b|t=3s=9m−18m=−9m.b\big|_{t=0}=0,\qquad b\big|_{t=3\,\mathrm s}=9\ \mathrm m-18\ \mathrm m=-9\ \mathrm m.

At t=0t=0, the stated displacement is zero. Routine C then requires b=0mb=0\ \mathrm{m}. At t=3.0st=3.0\ \mathrm{s}, C would consequently predict 18.0m18.0\ \mathrm{m}, not 9.0m9.0\ \mathrm{m}.

Alternatively, fitting only the latter time would require b=−9.0mb=-9.0\ \mathrm{m}, which fails at t=0t=0. No single constant bb satisfies both conditions. A constant offset cannot correct this time-dependent error in the coefficient of t2t^2.