Merge pull request #663 from vaerksted/master

fix typos
SciML · Mar 14, 2023 · eadca99 · eadca99
2 parents 696a955 + 33c7bdf
commit eadca99
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diff --git a/docs/src/basics/faq.md b/docs/src/basics/faq.md
@@ -54,7 +54,7 @@ may be deceiving. For example, `u' = -sqrt(u)` with `u(0)=1` cannot hit zero
 because its derivative shrinks to zero, right? Wrong! [It will hit zero in a finite
 time, after which the solution is undefined and does not have a purely real solution](https://www.wolframalpha.com/input/?i=u%27%3D-sqrt%28u%29).
 `u' = u^2 - 100u` will “usually” go to zero, but if `u(0)>10` then it will go to
-infinity. Plot out your diverging solution and see whether the asymtopics are
+infinity. Plot out your diverging solution and see whether the asymptotics are
 correct: if `u[i]` gets big, do your equations make `u'[i]` positive and growing?
 That would be a problem!
 

diff --git a/docs/src/examples/beeler_reuter.md b/docs/src/examples/beeler_reuter.md
@@ -59,8 +59,8 @@ mutable struct BeelerReuterCpu
     C::Array{Float32, 2}    # intracellular calcium concentration
     M::Array{Float32, 2}    # sodium current activation gate (m)
     H::Array{Float32, 2}    # sodium current inactivation gate (h)
-    J::Array{Float32, 2}    # sodium current slow inactivaiton gate (j)
-    D::Array{Float32, 2}    # calcium current activaiton gate (d)
+    J::Array{Float32, 2}    # sodium current slow inactivation gate (j)
+    D::Array{Float32, 2}    # calcium current activation gate (d)
     F::Array{Float32, 2}    # calcium current inactivation gate (f)
     XI::Array{Float32, 2}   # inward-rectifying potassium current (iK1)
 
@@ -411,8 +411,8 @@ mutable struct BeelerReuterGpu <: Function
     d_C::CuArray{Float32, 2}    # intracellular calcium concentration
     d_M::CuArray{Float32, 2}    # sodium current activation gate (m)
     d_H::CuArray{Float32, 2}    # sodium current inactivation gate (h)
-    d_J::CuArray{Float32, 2}    # sodium current slow inactivaiton gate (j)
-    d_D::CuArray{Float32, 2}    # calcium current activaiton gate (d)
+    d_J::CuArray{Float32, 2}    # sodium current slow inactivation gate (j)
+    d_D::CuArray{Float32, 2}    # calcium current activation gate (d)
     d_F::CuArray{Float32, 2}    # calcium current inactivation gate (f)
     d_XI::CuArray{Float32, 2}   # inward-rectifying potassium current (iK1)
 

diff --git a/docs/src/examples/diffusion_implicit_heat_equation.md b/docs/src/examples/diffusion_implicit_heat_equation.md
@@ -95,7 +95,7 @@ For the interior domain, a central and second-order finite difference stencil is
 ∇² = \left[\frac{1}{Δz²}, \frac{-2}{Δz²}, \frac{1}{Δz²}\right] \\
 ```
 
-At the boundaries, we need to modify the stencil to account for Dirichlet and Neumann BCs. Using the following index denotion:
+At the boundaries, we need to modify the stencil to account for Dirichlet and Neumann BCs. Using the following index denotation:
 
   - `i` first interior index
   - `b` boundary index

diff --git a/docs/src/examples/kepler_problem.md b/docs/src/examples/kepler_problem.md
@@ -116,7 +116,7 @@ sol_ = solve(prob2, RK4(), dt = 1 // 5, adaptive = false)
 analysis_plot2(sol_, H, L)
 ```
 
-There is a significant fluctuation in the first integrals, when there is no mainfold projection.
+There is a significant fluctuation in the first integrals, when there is no manifold projection.
 
 ```@example kepler
 function first_integrals_manifold(residual, u, p, t)

diff --git a/docs/src/features/callback_functions.md b/docs/src/features/callback_functions.md
@@ -287,9 +287,9 @@ Lastly, we can wrap it in a nice little constructor:
 ```@example callback3
 function AutoAbstol(save = true; init_curmax = 1e-6)
     affect! = AutoAbstolAffect(init_curmax)
-    condtion = (u, t, integrator) -> true
+    condition = (u, t, integrator) -> true
     save_positions = (save, false)
-    DiscreteCallback(condtion, affect!, save_positions = save_positions)
+    DiscreteCallback(condition, affect!, save_positions = save_positions)
 end
 ```