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Unit 11: Linear Differential Equations of First Order




              To locate one quantity from the other you multiply the first by some number, then add a  Notes
               different number to the outcome.

              On integration, we get  ye  Pdx    Qe  Pdx  dx  , c  as the required general solution.

              Linear differential equation is commonly known as Leibnitz’s linear equation.
              The system is said to be consistent if it contains a solution. Or else the system is said to be
               inconsistent.

              When concerning with two or more equations, it is fortunate to have a methodical technique
               of determining if the system is consistent and to discover all solutions.

                                   dy        n
              An equation of the form     Py   Qy , where P and Q are functions of x only or constants
                                   dx
               is known as Bernoulli’s  equation which can be made linear.

          11.4 Keywords


                                                dy        n
          Bernoulli’s Equation: An equation of the form     Py   Qy , where P and Q are functions of x
                                                dx
          only or constants is known as Bernoulli’s  equation.

                                            dy
          Linear Equation: An equation of the form     Py   Q , in which P & Q are functions of x alone
                                            dx
          or constant is called a linear equation of the first order.

          11.5 Review Questions

          Solve the following differential equations:

                     3  dy
                    y
          1.   (x   2 )     y
                        dx
                d   dy  2y 
          2.                0
               dx dx     x 
                  

                dy       2 ( 3/2)   x  1  x 2
                           
                      
          3.        (1 x  )    y       2 2
               dx                    (1 x  )
                                       
                dy        e x
          4.        y   e
                dx

                      dy        2
                                           x
          5.   cosh x      y sinh x   2cosh sinh x
                      dx
                dy    2      1     1 
                           x
          6.          y    sin    2 
               dx     x      x     x 




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