The inertia tensor for a solid sphere with radius \( b \) and mass \( m \) rotated about the center of mass is \( \left[\begin{array}{ccc}\frac{2}{5} m b^{2} & 0 & 0 \\ 0 & \frac{2}{5} m b^{2} & 0 \\ 0 & 0 & \frac{2}{5} m b^{2}\end{array}\right] \). What are the eigenvalues of the tensor if \( b=5 \) and \( m=4 \) ? Enter the eigenvalues from smallest to largest. \( I_{1}= \) Ex: 1.23 \( I_{2}= \) Ex: 1.23 \( I_{3}= \) Ex: 1.23
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To calculate the eigenvalues of the inertia tensor for the solid sphere given \( b = 5 \) and \( m = 4 \), we first compute the values from the inertia tensor: The components are: \[ I_{1} = I_{2} = I_{3} = \frac{2}{5} m b^{2} \] Substituting in the values for \( m \) and \( b \): \[ I_{1} = I_{2} = I_{3} = \frac{2}{5} \cdot 4 \cdot (5)^2 = \frac{2}{5} \cdot 4 \cdot 25 = \frac{200}{5} = 40 \] The eigenvalues from smallest to largest are: \[ I_{1} = 40.00, \quad I_{2} = 40.00, \quad I_{3} = 40.00 \]