The solution of the differential equation dy = (1 + y 2) dx is
y = tan (x + c)
We are asked to find the solution to the differential equation given by \(dy = (1 + y^2) dx\). This is a first-order differential equation.
The given differential equation can be rewritten as:
\(\frac{dy}{dx} = 1 + y^2\)
This is a separable differential equation because we can separate the variables \(y\) and \(x\) on opposite sides of the equation.
To separate the variables, we can move the term involving \(y\) to the left side and the term involving \(x\) (which is just \(dx\)) to the right side:
\(\frac{dy}{1 + y^2} = dx\)
Now, we integrate both sides of the separated equation:
\(\int \frac{dy}{1 + y^2} = \int dx\)
The integral of \(\frac{1}{1 + y^2}\) with respect to \(y\) is a standard integral, which is \(\tan^{-1}(y)\) or \(\arctan(y)\). The integral of \(1\) with respect to \(x\) is \(x\). Remember to add a constant of integration, let's call it \(c\), to one side (usually the side with the independent variable, \(x\)).
So, integrating both sides gives:
\(\tan^{-1}(y) = x + c\)
The solution is currently in the form \(\tan^{-1}(y) = x + c\). To express \(y\) explicitly in terms of \(x\), we take the tangent of both sides of the equation:
\(\tan(\tan^{-1}(y)) = \tan(x + c)\)
This simplifies to:
\(y = \tan(x + c)\)
This is the general solution to the given differential equation \(dy = (1 + y^2) dx\).
Let's compare our derived solution \(y = \tan(x + c)\) with the provided options:
Therefore, the correct solution is \(y = \tan (x + c)\).
| Step | Description | Application to \(dy = (1 + y^2) dx\) |
|---|---|---|
| 1 | Rewrite the equation as \(\frac{dy}{dx} = f(x)g(y)\). | \(\frac{dy}{dx} = 1 \cdot (1 + y^2)\) |
| 2 | Separate variables: \(\frac{dy}{g(y)} = f(x) dx\). | \(\frac{dy}{1 + y^2} = dx\) |
| 3 | Integrate both sides: \(\int \frac{dy}{g(y)} = \int f(x) dx\). | \(\int \frac{dy}{1 + y^2} = \int dx\) |
| 4 | Solve the integrals and add a constant of integration \(c\). | \(\tan^{-1}(y) = x + c\) |
| 5 | Solve for \(y\) (if possible) to get the general solution. | \(y = \tan(x + c)\) |
A differential equation is an equation that relates a function with one or more of its derivatives. The order of a differential equation is the order of the highest derivative appearing in it. The given equation \(dy/dx = 1 + y^2\) is a first-order ordinary differential equation.
A solution to a differential equation is a function that satisfies the equation when substituted into it. A general solution contains arbitrary constants (like \(c\) in our case), which arise from the integration process. A particular solution is obtained from the general solution by assigning specific values to the constants, usually based on initial or boundary conditions.
Separation of variables is a common technique used to solve first-order differential equations that can be written in the form \(\frac{dy}{dx} = f(x)g(y)\). This method works because the terms involving \(y\) can be moved to one side with \(dy\), and the terms involving \(x\) can be moved to the other side with \(dx\), allowing for independent integration.
The function \(\tan^{-1}(y)\) (or arctan y) is the inverse tangent function. Its derivative with respect to \(y\) is \(\frac{1}{1+y^2}\). This is why integrating \(\frac{1}{1+y^2}\) gives \(\tan^{-1}(y)\).
What is the general solution of the differential equation ydx – (x + 2y 2) dy = 0?
If xdy = y(dx + ydy) ; y(1) = 1 and y(x) > 0, then what is y(-3) equal to?
A particle starts from origin with a velocity (in m/s) given by the equation \(\rm \frac{dx}{dt}=x+1\) . The time (in seconds) taken by the particle to traverse a distance of 24 m is:
What is the solution of the differential equation (dy − dx) + cos x(dy + dx) = 0 ?
What is the solution of the following differential equation?
\(\rm \ln\left(\frac{dy}{dx}\right)+y = x\)
The solution of the differential equation \(\frac{{dy}}{{dx}} = \cos \left( {y - x} \right) + 1\) is
What is the solution of the differential equation x dy – y dx = 0?
What is the general solution of the differential equation \(\frac{{dy}}{{dx}} + \frac{x}{y} = 0\) ?
What is the solution of the differential equation \(\ln \left( {\frac{{{\rm{dy}}}}{{{\rm{dx}}}}} \right) - {\rm{a}} = 0?\)
The equation of motion of a one-dimensional forced harmonic oscillator in the presence of a dissipative force is described by \(\frac{{{{\rm{d}}^{\rm{2}}}{\rm{x}}}}{{{\rm{d}}{{\rm{t}}^{\rm{2}}}}}\,{\rm{ + }}\,{\rm{10}}\frac{{{\rm{dx}}}}{{{\rm{dt}}}}\,{\rm{ + }}\,{\rm{16x}}\,{\rm{ = }}\,{\rm{6t}}{{\rm{e}}^{{\rm{ - 8t}}}}{\rm{ + }}\,{\rm{4}}{{\rm{t}}^{\rm{2}}}{{\rm{e}}^{{\rm{ - 2t}}}}\) The general form of the particular solution, in terms of constants A, B etc., is
What is the general solution of the differential equation ydx – (x + 2y 2) dy = 0?
If xdy = y(dx + ydy) ; y(1) = 1 and y(x) > 0, then what is y(-3) equal to?
If y(x) is a solution of the differential equation \(\frac{{dy}}{{dx}} + 4xy = {x^3},y(0) = 0\) then \(\mathop {\lim }\limits_{x \to 0} y(x)\) is