diff --git a/docs/pages.jl b/docs/pages.jl
index 1b6f547e..c8f3d72e 100644
--- a/docs/pages.jl
+++ b/docs/pages.jl
@@ -3,6 +3,7 @@
 pages = [
     "Home" => "index.md",
     "output_saving.md",
+    "integrating.md",
     "timed_callbacks.md",
     "steady_state.md",
     "step_control.md",
diff --git a/docs/src/integrating.md b/docs/src/integrating.md
new file mode 100644
index 00000000..2cd7a74a
--- /dev/null
+++ b/docs/src/integrating.md
@@ -0,0 +1,30 @@
+# Numerical Integration Callbacks
+
+Sometimes one may want to solve an integral simultaniously to the solution of a differential equation. For example,
+assume we want to solve:
+
+```math
+u^\prime = f(u,p,t)
+h = \int_{t_0}^{t_f} g(u,p,t) dt
+```
+
+While one can use the ODE solver's dense solution to call an integration scheme on `sol(t)` after the solve, this can
+be memory intensive. Another way one can solve this problem is by extending the system, i.e.:
+
+```math
+u^\prime = f(u,p,t)
+h^\prime = g(u,p,t)
+```
+
+with $h(t_0) = 0$, so then $h(t_f)$ would be the solution to the integral. However, many differential equation solvers
+scale superlinearly with the equation size and thus this could add an extra cost to the solver process.
+
+The `IntegratingCallback` allows one to be able to solve such definite integrals in a way that is both memory and compute
+efficient. It uses the free local interpolation of a given step in order to approximate the Gaussian quadrature for a given
+step to the order of the numerical differential equation solve, thus achieving accuracy while not requiring the post-solution
+dense interpolation to be saved. By doing this via a callback, this method is able to easily integrate with functionality
+that introduces discontinuities, like other callbacks, in a way that is more accurate than a direct integration post solve.
+
+```@docs
+IntegratingCallback
+```
\ No newline at end of file
diff --git a/src/integrating.jl b/src/integrating.jl
index bb133b14..3d802e64 100644
--- a/src/integrating.jl
+++ b/src/integrating.jl
@@ -189,10 +189,14 @@ returns Integral(integrand_func(u(t),t)dt over the problem tspan.
     `integrand_func(t, u, integrator)::integrandType`. It's specified via
     `IntegrandValues(integrandType)`, i.e. give the type
     that `integrand_func` will output (or higher compatible type).
-  - `gauss_points` are the Gauss-Legendre points, scaled for the correct limits of integration
 
 The outputted values are saved into `integrand_values`. Time points are found via
 `integrand_values.t` and the values are `integrand_values.integrand`.
+
+!!! note
+
+    This method is currently limited to ODE solvers of order 10 or lower. Open an issue if other
+    solvers are required.
 """
 function IntegratingCallback(integrand_func, integrand_values::IntegrandValues)
     affect! = SavingIntegrandAffect(integrand_func, integrand_values)