Differential Equations
Introduction

Basic Conceptions

First-Order Differential Equations

Directly Integrable Equations
  Motion of a Body - Problem 1
  Motion of a Body - Problem 2
  Motion of a Body - Problem 3
  The Spontaneous Radioactive of Substance

Separable Equations
  Motion of Particals in Viscous Fluid
  Newton's Model of Cooling
  Model of Population

Separable Equations
  Motion of Particals in Viscous Fluid
  Newton's Model of Cooling
  Model of Population

Homogeneous Equations

Linear Equations

Bernoulli Equations

Exact Differential Equations

Differential Equations of Higher Orders

Basic Conceptions
Equations of Special Kinds

Some Graphic Illustrations using MATLAB

Clich here to go to Indefinite Inegrals


Clich here to go to Definite Inegrals




Real-Life Problems:
Newton's Model of Cooling
Real-Life Problems:   Motion of a Body - Problem 1 » Motion of a Body - Problem 2 » Motion of a Body - Problem 3 » The Spontaneous Radioactive of Substance » Motion of Particals in Viscous Fluid » Newton's Model of Cooling » Model of Population

Let the temperature of some body at time  t  be  T(t), and let the ambient temperature have a time independent value  A.

  1. Assume that  T(0) = T0 > A.
    Then the cooling of a body can be described by Newton's Model of Cooling, which states that the time rate of change of the temperature is proportional to the difference between temperatures:
    .
    The value of the proportionality constant  k  is determined by the properties of the object and ambient. However, in any circumstances    > 0.

    Separation of variables and integration gives the general integral of the differential equation:

    .
    Since  T(0) = T0  then
    .
    and so
    .
    Therefore,
    .
    which yields the particular solution:

    .

    One can see that  T(t) approaches the limit  A  as   .
  2. Let us assume now that  T0 < A.
    Then the heating of a body is described by the following initial value problem:

    .

    In a similar way as above we obtain the particular solution, which obeys the initial condition:

    .

The solutions for both cases, the cooling and heating of a body, can be combined into the following expression:

.


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