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ORTHOVEC is a collection of REDUCE procedures and operations which provide a simple-to-use environment for the manipulation of scalars and vectors. Operations include addition, subtraction, dot and cross products, division, modulus, div, grad, curl, laplacian, differentiation, integration, and Taylor expansion.
Version 2 is summarized in [Eas91]. It differs from the original ([Eas87]) in revised notation and extended capabilities.
The revised version of ORTHOVEC ([Eas91]) is, like the original ([Eas87]), a collection of REDUCE procedures and operators designed to simplify the machine aided manipulation of vectors and vector expansions frequently met in many areas of applied mathematics. The revisions have been introduced for two reasons: firstly, to add extra capabilities missing from the original and secondly, to tidy up input and output to make the package easier to use.
The changes from Version 1 include:
The LISP vector primitives are again used to store vectors, although with the introduction of LIST types in algebraic mode in REDUCE 3.4, the implementation may have been more simply achieved using lists to store vector components.
The philosophy used in Version 2 follows that used in the original: namely, algebraic mode is used wherever possible. The view is taken that some computational inefficiencies are acceptable if it allows coding to be intelligible to (and thence adaptable by) users other than LISP experts familiar with the internal workings of REDUCE.
Procedures and operators in ORTHOVEC fall into the five classes: initialisation, input-output, algebraic operations, differential operations and integral operations. Definitions are given in the following sections, and a summary of the procedure names and their meanings are give in Table 1. The final section discusses test examples.
The procedure vstart initialises ORTHOVEC. It may be called after ORTHOVEC has been loaded to reset coordinates. vstart provides a menu of standard coordinate systems:
which the user selects by number. Selecting options (1)-(4) automatically sets up the coordinates and scale factors. Selection option (5) shows the user how to select another coordinate system. If vstart is not called, then the default cartesian coordinates are used. ORTHOVEC may be re-initialised to a new coordinate system at any time during a given REDUCE session by typing
vstart $
ORTHOVEC assumes all quantities are either scalars or 3 component vectors. To define a vector \(a\) with components \((c_1, c_2, c_3)\) use the procedure svec as follows
a := svec(c1, c2, c3);
The standard REDUCE output for vectors when using the terminator “\(;\)” is to list the three components inside square brackets \([\cdots ]\), with each component in prefix form. A replacement for the standard REDUCE procedure maprin is included in the package to change the output of LISP vector components to algebraic notation. The procedure vout (which returns the value of its argument) can be used to give labelled output of components in algebraic form: e.g.,
b := svec (sin(x)**2, y**2, z)$ vout(b)$
The operator _ can be used to select a particular component (1, 2 or 3) for output e.g.
b _1 ;
Note the space before the _ operator: otherwise this would be read as identifier b_1.
Six infix operators, sum, difference, quotient, times, exponentiation and cross product, and four prefix operators, plus, minus, reciprocal and modulus are defined in ORTHOVEC. These operators can take suitable combinations of scalar and vector arguments, and in the case of scalar arguments reduce to the usual definitions of \( +, -, *, /, \) etc.
The operators are represented by symbols
+, -, /, *, ^, ><
The composite >< is an attempt to represent the cross product symbol \(\times \) in ASCII
characters. If we let \(\mathbf {v}\) be a vector and \(s\) be a scalar, then valid combinations of arguments of
the procedures and operators and the type of the result are as summarised below. The
notation used is
result :=procedure(left argument, right argument) or
result :=(left operand) operator (right operand) .
v | := | vectorplus(v) | or | v | := | + v |
s | := | vectorplus(s) | or | s | := | + s |
v | := | vectoradd(v,v) | or | v | := | v + v |
s | := | vectoradd(s,s) | or | s | := | s + s |
v | := | vectorminus(v) | or | v | := | - v |
s | := | vectorminus(s) | or | s | := | - s |
v | := | vectordifference(v,v) | or | v | := | v - v |
s | := | vectordifference(s,s) | or | s | := | s - s |
v | := | vectorrecip(v) | or | v | := | / v |
s | := | vectorrecip(s) | or | s | := | / s |
v | := | vectorquotient(v,v) | or | v | := | v / v |
v | := | vectorquotient(v, s ) | or | v | := | v / s |
v | := | vectorquotient( s ,v) | or | v | := | s / v |
s | := | vectorquotient(s,s) | or | s | := | s / s |
v | := | vectortimes( s ,v) | or | v | := | s * v |
v | := | vectortimes(v, s ) | or | v | := | v * s |
s | := | vectortimes(v,v) | or | s | := | v * v |
s | := | vectortimes( s , s ) | or | s | := | s * s |
v | := | vectorcross(v,v) | or | v | := | v \(\times \) v |
s | := | vectorexpt (v, s ) | or | s | := | v ^ s |
s | := | vectorexpt ( s , s ) | or | s | := | s ^ s |
s | := | vmod (s) |
s | := | vmod (v) |
All other combinations of operands for these operators lead to error messages being issued. The first two instances of vector multiplication are scalar multiplication of vectors, the third is the product of two scalars and the last is the inner (dot) product. The unary operators +, -, / can take either scalar or vector arguments and return results of the same type as their arguments. vmod returns a scalar.
In compound expressions, parentheses may be used to specify the order of combination. If parentheses are omitted the ordering of the operators, in increasing order of precedence is
+ | - | dotgrad | * | >< | ^ | _
and these are placed in the precedence list defined in REDUCE after \(<\). The differential operator dotgrad is defined in the following section, and the component selector _ was introduced in section 3.
Vector divisions are defined as follows: If \(\mathbf {a}\) and \(\mathbf {b}\) are vectors and \(c\) is a scalar, then \begin {align*} \mathbf {a} / \mathbf {b} & = \frac {\mathbf {a} \cdot \mathbf {b}}{ \mid \mathbf {b} \mid ^2}\\ c / \mathbf {a} & = \frac {c \mathbf {a} }{ \mid \mathbf {a} \mid ^2} \end {align*}
Both scalar multiplication and dot products are given by the same symbol, braces are advisable to ensure the correct precedences in expressions such as \((\mathbf {a} \cdot \mathbf {b}) (\mathbf {c} \cdot \mathbf {d})\).
Vector exponentiation is defined as the power of the modulus:
\(\mathbf {a}^n \equiv \f {vmod}(a)^n = \mid \mathbf {a} \mid ^n\)
Differential operators provided are div, grad, curl, delsq, and dotgrad. All but the last of these are prefix operators having a single vector or scalar argument as appropriate. Valid combinations of operator and argument, and the type of the result are shown in table 20.11.
s | := | div (v) |
v | := | grad(s) |
v | := | curl(v) |
v | := | delsq(v) |
s | := | delsq(s) |
v | := | v dotgrad v |
s | := | v dotgrad s |
All other combinations of operator and argument type cause error messages to be issued. The differential operators have their usual meanings [Spi59]. The coordinate system used by these operators is set by invoking vstart (cf. Sec. 20.39.2). The names h1, h2 and h3 are reserved for the scale factors, and u1, u2 and u3 are used for the coordinates.
A vector extension, vdf, of the REDUCE procedure DF allows the differentiation of a vector (scalar) with respect to a scalar to be performed. Allowed forms are vdf(v, s) \(\rightarrow \) v and vdf(s, s) \(\rightarrow \) s , where, for example \begin {equation*} \texttt {vdf( B,x)} \equiv \frac {\partial \textbf {B}}{\partial x} \end {equation*}
The standard REDUCE declarations depend and nodepend have been redefined to allow dependences of vectors to be compactly defined. For example
a := svec(a1,a2,a3)$; depend a,x,y;
causes all three components a1,a2 and a3 of a to be treated as functions of x and y. Individual component dependences can still be defined if desired.
depend a3,z;
The procedure vtaylor gives truncated Taylor series expansions of scalar or vector functions:
vtaylor(vex,vx,vpt,vorder);
returns the series expansion of the expression VEX with respect to variable VX about point VPT to order VORDER. Valid combinations of argument types are shown in table 20.12.
VEX | VX | VPT | VORDER |
v | v | v | v |
v | v | v | s |
v | s | s | s |
s | v | v | v |
s | v | v | s |
s | s | s | s |
Any other combinations cause error messages to be issued. Elements of VORDER must be non-negative integers, otherwise error messages are issued. If scalar VORDER is given for a vector expansion, expansions in each component are truncated at the same order, VORDER.
The new version of Taylor expansion applies l’Hôpital’s rule in evaluating coefficients, so handle cases such as \(\sin (x) / (x) \) , etc. which the original version of ORTHOVEC could not. The procedure used for this is ov_limit, which can be used directly to find the limit of a scalar function ex of variable x at point pt:-
ans := ov_limit(ex,x,pt);
Definite and indefinite vector, volume and scalar line integration procedures are included in ORTHOVEC. They are defined as follows: \begin {align*} \f {vint} (\mathbf {v},x) & = \int \mathbf {v}(x)dx\\ \f {dvint} (\mathbf {v},x, a, b) & = \int ^{b}_{a} \mathbf {v} (x) dx\\ \f {volint} (\mathbf {v}) & = \int \mathbf {v} h_{1} h_{2} h_{3} du_{1} du_{2} du_{3}\\ \f {dvolint}(\mathbf {v},\mathbf {l},\mathbf {u},n) & = \int ^{\mathbf {u}}_{\mathbf {l}} \mathbf {v} h_{1} h_{2} h_{3} du_{1} du_{2} du_{3}\\ \f {lineint} (\mathbf {v, \omega }, t) & = \int \mathbf {v} \cdot \mathbf {dr} \equiv \int v_{i} h_{i} \frac {\partial \omega _{i}}{\partial t} dt\\ \f {dlineint} (\mathbf {v, \omega } t, a, b) & = \int ^{b}_{a} v_i h_i \frac {\partial \omega _{i}}{\partial t} dt \end {align*}
In the vector and volume integrals, \(\mathbf {v}\) are vector or scalar, \(a, b,x\) and \(n\) are scalar. Vectors \(\mathbf {l}\) and \(\mathbf {u}\) contain expressions for lower and upper bounds to the integrals. The integer index \(n\) defines the order in which the integrals over \(u_1, u_2\) and \(u_3\) are performed in order to allow for functional dependencies in the integral bounds:
n | order |
1 | \(u_1~u_2~u_3\) |
2 | \(u_3~u_1~u_2\) |
3 | \(u_2~u_3~u_1\) |
4 | \(u_1~u_3~u_2\) |
5 | \(u_2~u_1~u_3\) |
otherwise | \(u_3~u_2~u_1\) |
The vector \(\mathbf {\omega }\) in the line integral’s arguments contain explicit paramterisation of the coordinates \(u_1, u_2, u_3\) of the line \(\mathbf {u}(t)\) along which the integral is taken.
Procedures | Description
| |
vstart | select coordinate system | |
svec | set up a vector | |
vout | output a vector | |
vectorcomponent | _ | extract a vector component (1-3) |
vectoradd | + | add two vectors or scalars |
vectorplus | + | unary vector or scalar plus |
vectorminus | - | unary vector or scalar minus |
vectordifference | - | subtract two vectors or scalars |
vectorquotient | / | vector divided by scalar |
vectorrecip | / | unary vector or scalar division |
(reciprocal) | ||
vectortimes | * | multiply vector or scalar by |
vector/scalar | ||
vectorcross | \(><\) | cross product of two vectors |
vectorexpt | ^ | exponentiate vector modulus or scalar |
vmod | length of vector or scalar | |
Procedures | Description
|
div | divergence of vector |
grad | gradient of scalar |
curl | curl of vector |
delsq | laplacian of scalar or vector |
dotgrad | (vector).grad(scalar or vector) |
vtaylor | vector or scalar Taylor series of vector or scalar |
vptaylor | vector or scalar Taylor series of scalar |
taylor | scalar Taylor series of scalar |
limit | limit of quotient using l’Hôpital’s rule |
vint | vector integral |
dvint | definite vector integral |
volint | volume integral |
dvolint | definite volume integral |
lineint | line integral |
dlineint | definite line integral |
maprin | vector extension of REDUCE maprin |
depend | vector extension of REDUCE depend |
nodepend | vector extension of REDUCE nodepend |
To use the REDUCE source version of ORTHOVEC, initiate a REDUCE session and then load the package with the command load_package orthovec; (see section 23.2 of the REDUCE manual). If coordinate dependent differential and integral operators other than cartesian are needed, then vstart must be used to reset coordinates and scale factors.
Six simple examples are given in the Test Run Output file orthovec.rlg to illustrate the working of ORTHOVEC. The input lines were taken from the file orthovec.tst (the Test Run Input), but could equally well be typed in at the Terminal.
Show that \begin {equation*} (\mathbf {a} \times \mathbf {b}) \cdot (\mathbf {c} \times \mathbf {d}) - (\mathbf {a} \cdot \mathbf {c})(\mathbf {b} \cdot \mathbf {d}) + (\mathbf {a} \cdot \mathbf {d})(\mathbf {b} \cdot \mathbf {c}) \equiv 0 \end {equation*}
Write the equation of motion \begin {equation*} \frac {\partial \mathbf {v}}{\partial t} + \mathbf {v} \cdot \mathbf {\nabla v} + \mathbf {\nabla } p - curl (\mathbf {B}) \times \mathbf {B} \end {equation*} in cylindrical coordinates.
Taylor expand
\(\sin (x) \cos (y) +e^z\) about the point \((0,0,0)\) to third order in \(x\), fourth order in \(y\) and fifth order in \(z\).
\(\sin (x)/x\) about \(x\) to fifth order.
\(\mathbf {v}\) about \(\mathbf {x}=(x,y,z)\) to fifth order, where \(\mathbf {v} = (x/ \sin (x),(e^y-1)/y,(1+z)^{10})\).
Obtain the second component of the equation of motion in example 2, and the first component of the final vector Taylor series in example 3.
Evaluate the line integral \begin {equation*} \int ^{\mathbf {r}_2}_{\mathbf {r}_1} \mathbf {A} \cdot d\mathbf {r} \end {equation*} from point \(\mathbf {r}_1 = (1,1,1)\) to point \(\mathbf {r}_2 = (2,4,8)\) along the path \((x,y,z) = (s, s^2, s^3)\) where \begin {equation*} \mathbf {A} = (3x^2 + 5y) \mathbf {i} - 12xy\mathbf {j} + 2xyz^2\mathbf {k} \end {equation*} and \((\mathbf {i, j, k})\) are unit vectors in the (\(x,y,z\)) directions.
Find the volume \(V\) common to the intersecting cylinders \(x^2 + y^2 = r^2\) and \(x^2 + z^2 = r^2\) i.e. evaluate \begin {equation*} V = 8 \int ^r_0 dx \int ^{ub}_0 dy \int ^{ub}_0 dz \end {equation*} where \(ub = \overline {\sqrt { r^2 - x^2}}\)
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