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6.3 Initial conditions

In the equation y′=f⁢(x)y^{\prime}=f(x), yy is the dependent variable and xx is the independent variable. In many physical applications, the independent variable is denoted tt and represents time. Then the equation

d⁢zd⁢t=f⁢(t)\frac{dz}{dt}=f(t)

describes the rate of change of zz, which here depends only on time. Often we want to find a solution z⁢(t)z(t) to the equation which has a certain value ξ∈ℝ\xi\in{\mathbb{R}} at a particular time t0t_{0}, i.e. such that z⁢(t0)=ξz(t_{0})=\xi. This is known as an initial condition. In the previous slide, an initial condition y⁢(x0)=ξy(x_{0})=\xi uniquely specifies the value of the constant cc (unless x0=2x_{0}=2).

Example.

Find the solution to d⁢yd⁢x=1x-2\frac{dy}{dx}=\frac{1}{x-2} which satisfies y⁢(1)=1y(1)=1.

Solution. We have log⁡|1-2|+c=1\log|1-2|+c=1, thus c=1.c={1.}