Solving the Differential Equation: (tan(x) − sin(x) sin(y)) dx + cos(x) cos(y) dy = 0
This differential equation is of the form M(x, y) dx + N(x, y) dy = 0, where:
- M(x, y) = tan(x) − sin(x) sin(y)
- N(x, y) = cos(x) cos(y)
To solve this, we can check if it's an exact differential equation. This means that the partial derivative of M with respect to y should be equal to the partial derivative of N with respect to x. Let's check:
- ∂M/∂y = -sin(x) cos(y)
- ∂N/∂x = -sin(x) cos(y)
Since ∂M/∂y = ∂N/∂x, the equation is exact. This means there exists a function F(x, y) such that:
- ∂F/∂x = M(x, y)
- ∂F/∂y = N(x, y)
To find F(x, y), we integrate M(x, y) with respect to x, treating y as a constant:
F(x, y) = ∫ (tan(x) − sin(x) sin(y)) dx = ln|sec(x)| + cos(x) sin(y) + g(y)
Here, g(y) is an arbitrary function of y. Now, we differentiate F(x, y) with respect to y and compare it to N(x, y):
∂F/∂y = cos(x) cos(y) + g'(y)
Comparing this with N(x, y) = cos(x) cos(y), we find that g'(y) = 0. Integrating this gives us:
g(y) = C, where C is an arbitrary constant.
Therefore, the general solution to the differential equation is:
F(x, y) = ln|sec(x)| + cos(x) sin(y) + C = 0
This solution represents a family of curves that are implicitly defined by the equation.