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Richa Nandra, Lovely Professional University              Unit 11: Linear Differential Equations of First Order




              Unit 11: Linear Differential Equations of First Order                             Notes


            CONTENTS
            Objectives
            Introduction

            11.1 Linear Equations
            11.2 Equations Reducible to the Linear (Bernoulli’s Equation)
            11.3 Summary

            11.4 Keywords
            11.5 Review Questions
            11.6 Further Readings

          Objectives

          After studying this unit, you will be able to:

              Understand the concept of linear equations
              Discuss the equations reducible to linear form

          Introduction

          An equation is basically the mathematical manner to portray a relationship among two variables.
          The variables may be physical quantities, possibly temperature and position for instance, in
          which case the equation informs us how one quantity relies on the other, so how the temperature
          differs with position. The easiest type of relationship that two such variables can comprise is
          a linear relationship. This shows that to locate one quantity from the other you multiply the
          first by some number, then add a different  number to  the outcome.  In this  unit, you will
          understand the concept of linear equations and equations reducible to linear form.

          11.1 Linear Equations

          An equation of the form

                         dy
                            Py   Q                                              ….(1)
                         dx
          in which P & Q are functions of x alone or constant is called a linear equation of the first order.



             Did u know?  If you are provided a value of x, you can simply discover the value of y.
          The general solution of the above equation can be found as follows:

          Multiplying both sides of (1) by   e Pdx , we have

                  dy   Pdx   Pdx   Pdx
                    e    Pye   Qe
                  dx





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