How to derive a symmetric tensor?

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SUMMARY

The discussion focuses on deriving the symmetric tensor \( Q_{ij} = \frac{m}{2} \dot{x}_i \dot{x}_j + \frac{k}{2} x_i x_j \) with respect to time. The tensor represents a physical quantity related to total energy, where \( m \) denotes mass and \( k \) represents a spring constant. The symmetry in the tensor is crucial for ensuring that the physical interpretations remain consistent across different coordinate systems. Understanding the derivation process is essential for applications in mechanics and physics.

PREREQUISITES
  • Understanding of tensor notation and operations
  • Familiarity with classical mechanics concepts, particularly energy
  • Knowledge of calculus, specifically differentiation with respect to time
  • Basic understanding of physical systems involving mass and spring constants
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  • Study the derivation of tensors in classical mechanics
  • Explore the physical significance of symmetric tensors in energy calculations
  • Learn about the application of tensors in advanced physics, such as continuum mechanics
  • Investigate the role of indices in tensor formulations and their implications
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Physicists, mechanical engineers, and students studying classical mechanics who seek to deepen their understanding of tensor calculus and its applications in energy systems.

Cathr
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Let ##Q_ik## be a symetric tensor, so that ##Q_ik= \frac{m}{2} \dot x_i \dot x_j + \frac{k}{2} x_i x_j## (here k is also a sub, couldn't do it better with LaTeX).
How do we derive such a tensor, with respect to time? And what could such a tensor mean in a physical sense? It really looks like the tensor for the total energy, except that I don't understand the need for adding indices to create a symmetrical form.
 
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I apologize, the formula is actually ##Q_{ij}= \frac{m}{2} \dot x_i \dot x_j + \frac{k}{2} x_i x_j## .
 

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