| .\" Copyright (c) 1991 The Regents of the University of California. |
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| .\" from: @(#)atan2.3 5.1 (Berkeley) 5/2/91 |
| .\" $FreeBSD: src/lib/msun/man/atan2.3,v 1.14 2005/01/28 21:13:34 ru Exp $ |
| .\" |
| .Dd January 14, 2005 |
| .Dt ATAN2 3 |
| .Os |
| .Sh NAME |
| .Nm atan2 , |
| .Nm atan2f |
| .Nd arc tangent functions of two variables |
| .Sh LIBRARY |
| .Lb libm |
| .Sh SYNOPSIS |
| .In math.h |
| .Ft double |
| .Fn atan2 "double y" "double x" |
| .Ft float |
| .Fn atan2f "float y" "float x" |
| .Sh DESCRIPTION |
| The |
| .Fn atan2 |
| and the |
| .Fn atan2f |
| functions compute the principal value of the arc tangent of |
| .Fa y/ Ns Ar x , |
| using the signs of both arguments to determine the quadrant of |
| the return value. |
| .Sh RETURN VALUES |
| The |
| .Fn atan2 |
| and the |
| .Fn atan2f |
| functions, if successful, |
| return the arc tangent of |
| .Fa y/ Ns Ar x |
| in the range |
| .Bk -words |
| .Bq \&- Ns \*(Pi , \&+ Ns \*(Pi |
| .Ek |
| radians. |
| Here are some of the special cases: |
| .Bl -column atan_(y,x)_:=____ sign(y)_(Pi_atan2(Xy_xX))___ |
| .It Fn atan2 y x No := Ta |
| .Fn atan y/x Ta |
| if |
| .Ar x |
| > 0, |
| .It Ta sign( Ns Ar y Ns )*(\*(Pi - |
| .Fn atan "\\*(Bay/x\\*(Ba" ) Ta |
| if |
| .Ar x |
| < 0, |
| .It Ta |
| .No 0 Ta |
| if x = y = 0, or |
| .It Ta |
| .Pf sign( Ar y Ns )*\\*(Pi/2 Ta |
| if |
| .Ar x |
| = 0 \(!= |
| .Ar y . |
| .El |
| .Sh NOTES |
| The function |
| .Fn atan2 |
| defines "if x > 0," |
| .Fn atan2 0 0 |
| = 0 despite that previously |
| .Fn atan2 0 0 |
| may have generated an error message. |
| The reasons for assigning a value to |
| .Fn atan2 0 0 |
| are these: |
| .Bl -enum -offset indent |
| .It |
| Programs that test arguments to avoid computing |
| .Fn atan2 0 0 |
| must be indifferent to its value. |
| Programs that require it to be invalid are vulnerable |
| to diverse reactions to that invalidity on diverse computer systems. |
| .It |
| The |
| .Fn atan2 |
| function is used mostly to convert from rectangular (x,y) |
| to polar |
| .if n\ |
| (r,theta) |
| .if t\ |
| (r,\(*h) |
| coordinates that must satisfy x = |
| .if n\ |
| r\(**cos theta |
| .if t\ |
| r\(**cos\(*h |
| and y = |
| .if n\ |
| r\(**sin theta. |
| .if t\ |
| r\(**sin\(*h. |
| These equations are satisfied when (x=0,y=0) |
| is mapped to |
| .if n \ |
| (r=0,theta=0). |
| .if t \ |
| (r=0,\(*h=0). |
| In general, conversions to polar coordinates |
| should be computed thus: |
| .Bd -unfilled -offset indent |
| .if n \{\ |
| r := hypot(x,y); ... := sqrt(x\(**x+y\(**y) |
| theta := atan2(y,x). |
| .\} |
| .if t \{\ |
| r := hypot(x,y); ... := \(sr(x\u\s82\s10\d+y\u\s82\s10\d) |
| \(*h := atan2(y,x). |
| .\} |
| .Ed |
| .It |
| The foregoing formulas need not be altered to cope in a |
| reasonable way with signed zeros and infinities |
| on a machine that conforms to |
| .Tn IEEE 754 ; |
| the versions of |
| .Xr hypot 3 |
| and |
| .Fn atan2 |
| provided for |
| such a machine are designed to handle all cases. |
| That is why |
| .Fn atan2 \(+-0 \-0 |
| = \(+-\*(Pi |
| for instance. |
| In general the formulas above are equivalent to these: |
| .Bd -unfilled -offset indent |
| .if n \ |
| r := sqrt(x\(**x+y\(**y); if r = 0 then x := copysign(1,x); |
| .if t \ |
| r := \(sr(x\(**x+y\(**y);\0\0if r = 0 then x := copysign(1,x); |
| .Ed |
| .El |
| .Sh SEE ALSO |
| .Xr acos 3 , |
| .Xr asin 3 , |
| .Xr atan 3 , |
| .Xr cos 3 , |
| .Xr cosh 3 , |
| .Xr math 3 , |
| .Xr sin 3 , |
| .Xr sinh 3 , |
| .Xr tan 3 , |
| .Xr tanh 3 |
| .Sh STANDARDS |
| The |
| .Fn atan2 |
| function conforms to |
| .St -isoC . |