diff --git a/HISTORY.txt b/HISTORY.txt
index 3de1d0e5a..4a3c2887f 100644
--- a/HISTORY.txt
+++ b/HISTORY.txt
@@ -2,7 +2,7 @@ v1.10.2 (expected around 2025-03-01)
 ====================
 
  - Implemented the IAS15 integrator of Rein & Spiegel 2015.
- 
+
  - Combine the drift calculations in the Python leapfrog integrator (#365).
 
  - Move the checks for non-axisymmetric and dissipative potentials from internal to
diff --git a/doc/source/orbit.rst b/doc/source/orbit.rst
index ee1444ddd..a0e79ac51 100644
--- a/doc/source/orbit.rst
+++ b/doc/source/orbit.rst
@@ -1016,8 +1016,8 @@ the ``orbit.integrate`` method. Currently available integrators are
 * dop853_c
 * ias15_c
 
-which are Runge-Kutta, Dormand-Prince methods and the IAS15 
-integrator in `Rein & Spiegel (2014) <https://doi.org/10.1093/mnras/stu2164>`_. 
+which are Runge-Kutta, Dormand-Prince methods and the IAS15
+integrator in `Rein & Spiegel (2014) <https://doi.org/10.1093/mnras/stu2164>`_.
 There are also a number of symplectic integrators available
 
 * leapfrog_c
@@ -1047,7 +1047,7 @@ which are speedy and reliable. For example, compare
 >>> timeit(o.integrate(ts,mp,method='dop853_c'))
 # 4.65 ms ± 86.8 µs per loop (mean ± std. dev. of 7 runs, 100 loops each)
 
-The ``ias15_c`` method uses adaptive timestepping under the hood, and 
+The ``ias15_c`` method uses adaptive timestepping under the hood, and
 can be used in cases where very high precision is required.
 
 If the C extensions are unavailable for some reason, I recommend using