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    • 1.9.27: Math-vector basics and diffrential equations
      https://phys.libretexts.org/Courses/Georgia_State_University/GSU-TM-Physics_I_(2211)/01%3A_Introduction_to_Physics_Measurements_and_Mathematics_Tools/1.09%3A_Math_Review_of_Other_Topics/1.9.27%3A_Math-vector_basics_and_diffrential_equations
      Note that this is the most general form: if there is a coefficient (constant or otherwise) in front of the second derivative, we simply divide the whole equation by that coefficient and redefine the c...Note that this is the most general form: if there is a coefficient (constant or otherwise) in front of the second derivative, we simply divide the whole equation by that coefficient and redefine the coefficients to match Equation ???. Now suppose we have a solution y1(x) of the homogeneous equation (so for the case that r(x)=0 ).
    • 1.9.27: Math-vector basics and diffrential equations
      https://phys.libretexts.org/Courses/Georgia_State_University/GSU-TM-Physics_II_(2212)/01%3A_Introduction_to_Physics_Measurements_and_Mathematics_Tools/1.09%3A_Math_Review_of_Other_Topics/1.9.27%3A_Math-vector_basics_and_diffrential_equations
      Note that this is the most general form: if there is a coefficient (constant or otherwise) in front of the second derivative, we simply divide the whole equation by that coefficient and redefine the c...Note that this is the most general form: if there is a coefficient (constant or otherwise) in front of the second derivative, we simply divide the whole equation by that coefficient and redefine the coefficients to match Equation ???. Now suppose we have a solution y1(x) of the homogeneous equation (so for the case that r(x)=0 ).

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