| 1. | Let Y ( n ) be the solution to the differential equation
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| 2. | This differential equation is the classic equation of motion for charged particles.
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| 3. | The equation of motion for \ psi is the time differential equation:
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| 4. | His specialisms included nonlinear partial differential equations and calculus of variations.
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| 5. | Returning to differential equations, Hamming studied means of numerically integrating them.
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| 6. | The same year he used equivalent circuits to solve differential equations.
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| 7. | The six partial differential equations above represent six independent Reynolds stresses.
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| 8. | This partial differential equation may be solved by separation of variables.
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| 9. | The equation itself is a fourth order non linear differential equation.
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| 10. | Then you can apply those boundary conditions to this differential equation:
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