Measured g = 9.72 against 9.81
- Calculate
- Percent error
- Measured value
- 9.72
- Accepted (true) value
- 9.81
- Percent error
- 0.9174%
- Signed percent error
- -0.9174%
- Absolute error
- 0.09
核验来源:Python 3.8 decimal: |9.72 − 9.81| / 9.81 × 100 = 0.9174312
Percent error from measured and accepted values, and uncertainty propagation through sums, products, quotients and powers, in quadrature or worst case.
更新于 已验证的示例:7
The measurement is 0.9174% below the accepted value.
Percent error compares a measurement with an accepted value: |measured − accepted| / |accepted| × 100. Uncertainty propagation works out how the ± uncertainties of inputs carry into a calculated result. For sums and differences the absolute uncertainties combine; for products and quotients the relative uncertainties combine; a power aⁿ multiplies the relative uncertainty by |n|. Independent random errors combine in quadrature (the square root of the sum of squares), and the worst-case option adds them linearly.
The default, a measured g of 9.72 m/s² against the accepted 9.81 m/s², is 0.917% low. Multiplying (2.0 ± 0.1) by (3.0 ± 0.2) gives relative uncertainties of 5% and 6.7%, which combine in quadrature to 8.3%, so the product is reported as 6.0 ± 0.5.
Results are rounded as Taylor's An Introduction to Error Analysis recommends: the uncertainty to one significant figure, or two when it starts with 1, and the value to the same decimal place. The formulas are first-order, so they assume each uncertainty is small compared with its value.
核验来源:Python 3.8 decimal: |9.72 − 9.81| / 9.81 × 100 = 0.9174312
核验来源:Taylor §3.5: √(0.3² + 0.4²) = 0.5
核验来源:Taylor §3.3: δa + δb = 0.7
核验来源:Python 3.8 decimal: 6 × √(0.05² + 0.0667²) = 6 × 0.083333 = 0.5
Percent error = |measured − accepted| / |accepted| × 100. Measuring g as 9.72 m/s² against an accepted 9.81 m/s² gives 0.09/9.81 × 100 = 0.917%. Keep the sign when the direction matters: −0.917% says the measurement came out low. The formula fails when the accepted value is 0; report the absolute error instead.
Combine the relative uncertainties in quadrature: δq/|q| = √((δa/a)² + (δb/b)²). For (2.0 ± 0.1) × (3.0 ± 0.2) the relative uncertainties are 5% and 6.7%, giving 8.3% of 6.0, so q = 6.0 ± 0.5. Division follows the same rule: (10 ± 0.5) ÷ (4 ± 0.2) = 2.50 ± 0.18.
Combine the absolute uncertainties: δq = √(δa² + δb²) when the errors are independent and random, or δa + δb for a worst-case bound. (10.0 ± 0.3) + (5.0 ± 0.4) = 15.0 ± 0.5 in quadrature, or 15.0 ± 0.7 worst case. Subtraction uses the same rule, so the difference of two close values can carry a large relative uncertainty.
When the errors in the inputs are independent and random, the assumption behind the combined standard uncertainty in NIST Technical Note 1297 and the GUM. Quadrature never exceeds the linear sum: 0.3 and 0.4 combine to 0.5 rather than 0.7. Use the linear worst case when errors may be correlated, such as two readings taken with the same miscalibrated instrument.
One, or two when its leading digit is 1, following Taylor's An Introduction to Error Analysis (§2.2); the value is then rounded to the same decimal place. So 0.1768 becomes 0.18 and the result is written 2.50 ± 0.18, while 0.52 becomes 0.5 and the result 6.0 ± 0.5. Writing 6.0 ± 0.5234 claims more precision than the measurement has.
准确性取决于输入值和方法的假设。十进制运算使用50位有效数字,但估算、数值方法和源数据的精度可能较低;显示时的舍入并不能消除这些限制。 已按独立来源核验的计算示例:7。 例如,“Measured g = 9.72 against 9.81”根据Python 3.8 decimal: |9.72 − 9.81| / 9.81 × 100 = 0.9174312进行核验。
Taylor, An Introduction to Error Analysis (2nd ed., 1997), ch. 2–3 (rules for reporting and propagating uncertainties); NIST Technical Note 1297 — Guidelines for evaluating and expressing the uncertainty of NIST measurement results.
此计算器包含 7 个已解示例,答案来自独立来源。这些示例会在测试套件中运行,你也可以在此运行验证。
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