The inverse cotangent function, in modern notation written as arccot(x), gives the angle θ, so that:
Due to the periodical nature of the cotangent function, there are many angles θ that can give the same cotangent value (i.e. θ+π, θ+3π, etc.). As a result, it is impossible to define a single inverse function, unless the range of the return values is restricted, so that a one-to-one relationship between θ and cotθ can be established. Therefore, multiple branches of the arccot function can be defined. Commonly, the desired range of θ values spans between 0 and π. The branch of arccot, in that case, is called the principal branch.
The arccot function can be defined in a Taylor series form, like this:
From the expanded form of the series, it can be seen that the higher terms become insignificant, for values of x close to zero, resulting in the following quite useful approximation:
The derivative of the arccot function is:
The integral of the arccot function is given by:
The following properties are also valid for the arccot function: