dovs()
function in the
stokes
packagefunction (K)
{
if (is.zero(K) || is.scalar(K)) {
return(0)
}
else {
return(max(index(K)))
}
}
To cite the stokes
package in publications, please use
Hankin (2022). Function
dovs()
returns the dimensionality of the underlying vector
space of a k-form. Recall that
a k-form is an alternating
linear map from Vk to ℝ, where V = ℝn (Spivak 1965).
Function dovs()
returns n [compare arity()
,
which returns k]. As seen
above, the function is very simple, essentially being
max(index(K))
, but its use is not entirely straightforward
in the context of stokes
idiom. Consider the following:
## An alternating linear map from V^2 to R with V=R^4:
## val
## 2 4 = 9
## 1 4 = 8
## 2 3 = 1
## 1 3 = -3
## 3 4 = -2
## 1 2 = 2
Now object a
is notionally a map from (ℝ4)2 to ℝ:
## [,1] [,2]
## [1,] 1 5
## [2,] 2 6
## [3,] 3 7
## [4,] 4 8
## [1] -148
However, a
can equally be considered to be a map from
(ℝ5)2 to ℝ:
## [,1] [,2]
## [1,] 1 5
## [2,] 2 6
## [3,] 3 7
## [4,] 4 8
## [5,] 1454 -9564
## [1] -148
If we view a [or indeed
f()
] in this way, that is a: (ℝ5)2 → ℝ,
we observe that row 5 is ignored: e5 = (0, 0, 0, 0, 1)T
maps to zero in the sense that f(e5, v) = f(v, e5) = 0,
for any v ∈ ℝ5.
## [,1] [,2]
## [1,] 0 0.3800352
## [2,] 0 0.7774452
## [3,] 0 0.9347052
## [4,] 0 0.2121425
## [5,] 1 0.6516738
## [1] 0
(above we see that rows 1-4 of M
are ignored because of
the zero in column 1; row 5 is ignored because the index of
a
does not include the number 5). Because a
is
alternating, we could have put e5 in the second column
with the same result. Alternatively we see that the k-form a
, evaluated
with e5 as one of
its arguments, returns zero because the index matrix of a
does not include the number 5. Most of the time, this kind of
consideration does not matter. However, consider this:
## An alternating linear map from V^1 to R with V=R^1:
## val
## 1 = 1
Now, we know that dx
is supposed to be a map
from (ℝ3)1 to
ℝ; but:
## [1] 1
So according to stokes
, dx : (ℝ1)1 → ℝ. This
does not really matter numerically, until we consider the Hodge star
operator. We know that ⋆dx = dy ∧ dz , but
## [1] 1
Above we see the package giving, correctly, that the Hodge star of
dx is the zero-dimensional volume
element (otherwise known as “1”). To get the answer appropriate if dx is considered as a map from (ℝ3)1 to ℝ [that is, dx : (ℝ3)1 → ℝ], we
need to specify dovs
explicitly:
## An alternating linear map from V^2 to R with V=R^3:
## val
## 2 3 = 1
Actually this looks a lot better with a more appropriate print method:
## An alternating linear map from V^2 to R with V=R^3:
## + dy^dz