The moment of inertial I of a metre rule of rectengular cross-section is \[ I=\frac{b d^{2}}{12} \] alculate I and its standard error (se) if \( b=2.66 \pm 0.01 \mathrm{~cm}\langle \) (s.e). \( d=0.65 \pm 004 \) .e.).
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To calculate the moment of inertia \( I \) for the given rectangular cross-section, you can substitute the values directly into the formula: \[ I = \frac{b d^{2}}{12} \] Convert the dimensions from centimeters to meters for consistency: - \( b = 2.66 \, \text{cm} = 0.0266 \, \text{m} \) - \( d = 0.65 \, \text{cm} = 0.0065 \, \text{m} \) Now, plug in the values into the formula: \[ I = \frac{0.0266 \times (0.0065)^2}{12} \] Next, let’s calculate the standard error of \( I \). The formula for calculating the standard error \( se \) based on the propagation of uncertainty will involve both partial derivatives and the uncertainties in \( b \) and \( d \). Using the standard error propagation formula: \[ se(I) = I \sqrt{\left(\frac{se(b)}{b}\right)^2 + \left(2 \frac{se(d)}{d}\right)^2} \] Here, - \( se(b) = 0.01 \, \text{cm} = 0.0001 \, \text{m} \) - \( se(d) = 0.04 \, \text{cm} = 0.0004 \, \text{m} \) After performing the calculations, we can find the values for \( I \) and its associated standard error. Be sure to carefully walk through the calculations to ensure accuracy.