Difference between revisions of "LlEuler2Rot"
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|caveats | |caveats | ||
|constants | |constants | ||
|examples=<lsl> | |examples=<lsl>default | ||
default | |||
{ | { | ||
state_entry() | state_entry() | ||
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llSay(0,"The Euler2Rot of "+(string)input+" is: "+(string)rot ); | llSay(0,"The Euler2Rot of "+(string)input+" is: "+(string)rot ); | ||
} | } | ||
} | }</lsl> | ||
</lsl> | |||
|helpers | |helpers | ||
|also_functions={{LSL DefineRow||[[llRot2Euler]]|}} | |also_functions={{LSL DefineRow||[[llRot2Euler]]|}} | ||
Revision as of 09:34, 25 December 2007
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Summary
Function: rotation llEuler2Rot( vector v );| 16 | Function ID |
| 0.0 | Forced Delay |
| 10.0 | Energy |
Returns a rotation representation of Euler Angles v.
| • vector | v |
Specification
The Euler angle vector is converted to a rotation by doing the rotations around the 3 axes in Z, Y, X order. So llRot2Euler(<1.0, 2.0, 3.0> * DEG_TO_RAD) generates a rotation by taking the zero rotation, a vector pointing along the X axis, first rotating it 3 degrees around the global Z axis, then rotating the resulting vector 2 degrees around the global Y axis, and finally rotating that 1 degree around the global X axis.
Caveats
Examples
<lsl>default {
state_entry()
{
vector input = <73.0, -63.0, 20.0> * DEG_TO_RAD;//not advised to make your own quaternion
rotation rot = llEuler2Rot(input);
llSay(0,"The Euler2Rot of "+(string)input+" is: "+(string)rot );
}
}</lsl>
Notes
<lsl>v/=2; rotation k = <0,0,llSin(v.z),llCos(v.z)> * <0,llSin(v.y),0,llCos(v.y)> * <llSin(v.x),0,0,llCos(v.x)>;</lsl>
