A final experimental result is rarely built from a single measured quantity -- it usually combines several quantities, each measured (possibly with a different instrument, and hence a different error). The error in the final result depends on (i) the individual errors in each measured quantity, and (ii) the mathematical operation used to combine them -- so different operations propagate error differently.
i) Sum, Z=A+B. If A=A±ΔA and B=B±ΔB, the worst case is when both errors add in the same direction: Z±ΔZ=(A±ΔA)+(B±ΔB)=(A+B)±(ΔA+ΔB), so
ΔZ=ΔA+ΔB.
Example: R1=(100±3)Ω and R2=(150±2)Ω in series: R=R1+R2=(250±5)Ω.
ii) Difference, Z=A−B. Again the worst case adds the two absolute errors: Z±ΔZ=(A±ΔA)−(B±ΔB)=(A−B)±(ΔA+ΔB), so
ΔZ=ΔA+ΔB.
Example: t1=(20±0.5)∘C, t2=(50±0.5)∘C: t=t2−t1=(30±1)∘C.
Whether the quantities are added or subtracted, the maximum possible absolute error in the result is the sum of the individual absolute errors -- errors never cancel in the worst-case bound.
iii) Product, Z=AB. Z±ΔZ=(A±ΔA)(B±ΔB)=AB±AΔB±BΔA±ΔAΔB. Dividing by Z=AB and dropping the doubly-small term AΔA⋅BΔB, the maximum fractional error is
ZΔZ=AΔA+BΔB.
Example: length A=(5.7±0.1) cm, breadth b=(3.4±0.2) cm: area =A×b=19.4 cm2 (3 sig. figs.), AareaΔAarea=5.70.1+3.40.2=0.0175+0.0588=0.0763, so ΔAarea=0.0763×19.4≈1.5 cm2; area =(19.4±1.5) cm2.
iv) Quotient, Z=A/B. Using (1+x)n≈1+nx for small x, the same style of derivation gives the identical rule as for a product:
ZΔZ=AΔA+BΔB.
Example (Ohm's law): V=(100±5) V, I=(10±0.2) A: R=V/I=10Ω; RΔR=1005+100.2=0.05+0.02=0.07, so ΔR=0.7Ω; R=(10±0.7)Ω.
v) Power, Z=An. Since An is really A multiplied by itself n times, applying the product rule n times gives
ZΔZ=nAΔA.
The fractional error in the n-th power of a quantity is n times the fractional error in the quantity itself. …