discrete physics · from the differential formulation, wlmch is the most usual, we get back to the...

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Page 1: Discrete Physics · From the differential formulation, wlmch is the most usual, we get back to the variational One When the differ- ential operator, which forms the equation, has
Page 2: Discrete Physics · From the differential formulation, wlmch is the most usual, we get back to the variational One When the differ- ential operator, which forms the equation, has
Page 3: Discrete Physics · From the differential formulation, wlmch is the most usual, we get back to the variational One When the differ- ential operator, which forms the equation, has
Page 4: Discrete Physics · From the differential formulation, wlmch is the most usual, we get back to the variational One When the differ- ential operator, which forms the equation, has
Page 5: Discrete Physics · From the differential formulation, wlmch is the most usual, we get back to the variational One When the differ- ential operator, which forms the equation, has
Page 6: Discrete Physics · From the differential formulation, wlmch is the most usual, we get back to the variational One When the differ- ential operator, which forms the equation, has
Page 7: Discrete Physics · From the differential formulation, wlmch is the most usual, we get back to the variational One When the differ- ential operator, which forms the equation, has
Page 8: Discrete Physics · From the differential formulation, wlmch is the most usual, we get back to the variational One When the differ- ential operator, which forms the equation, has