| symbolic | R Documentation |
Returns a character string representing k-tensor and
k-form objects in symbolic form. Used by the print method if
either option kform_symbolic_print or
ktensor_symbolic_print is non-null.
as.symbolic(M,symbols=letters,d="")
M |
Object of class |
symbols |
A character vector giving the names of the symbols |
d |
String specifying the appearance of the differential operator |
Spivak (p89), in archetypically terse writing, states:
A function f is considered to be a 0-form and
f\cdot\omega is also written
f\wedge\omega. If
f\colon\mathbb{R}^n\longrightarrow\mathbb{R} is
differentiable, then
Df(p)\in\Lambda^1\left(\mathbb{R}^n\right).
By a minor modification we therefore obtain a 1-form
\mathrm{d}f, defined by
\mathrm{d}f(p)\left(v_p\right)=Df(p)(v).
Let us consider in particular the 1-forms
\mathrm{d}\pi^i. It is customary to let
x^i denote the function \pi^i (On \mathbb{R}^3 we often denote x^1,
x^2, and x^3 by x, y, and
z). This standard notation has obvious disadvantages but it
allows many classical results to be expressed by formulas of equally
classical appearance. Since
\mathrm{d}x^i(p)(v_p)=\mathrm{d}\pi^i(p)(v_p)=D\pi^i(p)(v)=v^i, we see that
\mathrm{d}x^1(p),\ldots,\mathrm{d}x^n(p)
is just the dual basis to
(e_1)_p,\ldots,(e_n)_p. Thus every
k-form \omega can be written
\omega=\sum_{i_1 < \cdots < i_k}\omega_{i_1,\ldots,i_k}
\mathrm{d}x^{i_1}\wedge\cdots\wedge\mathrm{d}x^{i_k}.
Function as.symbolic() uses this format. For completeness, we
add (p77) that k-tensors may be expressed in the form
\sum_{i_1,\ldots, i_k=1}^n a_{i_1,\ldots,i_k}\cdot
\phi_{i_1}\otimes\cdots\otimes\phi_{i_k}.
and this form is used for k-tensors. The print method for
tensors, print.ktensor(), writes d1 for \phi_1,
d2 for \phi_2 [where \phi_i(x^j)=\delta_i^j].
Returns a “noquote” character string.
Robin K. S. Hankin
print.stokes,dx
(o <- kform_general(3,2,1:3))
as.symbolic(o,d="d",symbols=letters[23:26])
(a <- rform(n=50))
as.symbolic(a,symbols=state.abb)
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