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authorEric Anholt <[email protected]>2008-02-06 15:41:04 -0800
committerEric Anholt <[email protected]>2008-02-06 15:43:05 -0800
commit700a77fb48f364f85e013cf5fb68c04eb83317e7 (patch)
treef4e3f7d8aa38887da335c811d7ef8b07f83661d3 /src
parent2551a5ee80ab523006618c79766e2409b2a62d84 (diff)
[915] Fix COS function using same plan as SIN.
The previous COS function failed badly outside of [-pi/2, pi/2].
Diffstat (limited to 'src')
-rw-r--r--src/mesa/drivers/dri/i915/i915_fragprog.c98
1 files changed, 63 insertions, 35 deletions
diff --git a/src/mesa/drivers/dri/i915/i915_fragprog.c b/src/mesa/drivers/dri/i915/i915_fragprog.c
index cbac07cde16..b475fb632f8 100644
--- a/src/mesa/drivers/dri/i915/i915_fragprog.c
+++ b/src/mesa/drivers/dri/i915/i915_fragprog.c
@@ -48,7 +48,7 @@ static const GLfloat sin_quad_constants[2][4] = {
2.0,
-1.0,
.5,
- 0.0
+ .75
},
{
4.0,
@@ -375,52 +375,80 @@ upload_program(struct i915_fragment_program *p)
case OPCODE_COS:
src0 = src_vector(p, &inst->SrcReg[0], program);
tmp = i915_get_utemp(p);
+ consts0 = i915_emit_const4fv(p, sin_quad_constants[0]);
+ consts1 = i915_emit_const4fv(p, sin_quad_constants[1]);
+ /* Reduce range from repeating about [-pi,pi] to [-1,1] */
i915_emit_arith(p,
- A0_MUL,
+ A0_MAD,
tmp, A0_DEST_CHANNEL_X, 0,
- src0, i915_emit_const1f(p, 1.0 / (M_PI)), 0);
+ src0,
+ swizzle(consts1, Z, ZERO, ZERO, ZERO), /* 1/(2pi) */
+ swizzle(consts0, W, ZERO, ZERO, ZERO)); /* .75 */
- i915_emit_arith(p, A0_MOD, tmp, A0_DEST_CHANNEL_X, 0, tmp, 0, 0);
+ i915_emit_arith(p, A0_FRC, tmp, A0_DEST_CHANNEL_X, 0, tmp, 0, 0);
- /* By choosing different taylor constants, could get rid of this mul:
- */
- i915_emit_arith(p,
- A0_MUL,
- tmp, A0_DEST_CHANNEL_X, 0,
- tmp, i915_emit_const1f(p, (M_PI)), 0);
+ i915_emit_arith(p,
+ A0_MAD,
+ tmp, A0_DEST_CHANNEL_X, 0,
+ tmp,
+ swizzle(consts0, X, ZERO, ZERO, ZERO), /* 2 */
+ swizzle(consts0, Y, ZERO, ZERO, ZERO)); /* -1 */
- /*
- * t0.xy = MUL x.xx11, x.x1111 ; x^2, x, 1, 1
- * t0 = MUL t0.xyxy t0.xx11 ; x^4, x^3, x^2, 1
- * t0 = MUL t0.xxz1 t0.z111 ; x^6 x^4 x^2 1
- * result = DP4 t0, cos_constants
- */
- i915_emit_arith(p,
- A0_MUL,
- tmp, A0_DEST_CHANNEL_XY, 0,
- swizzle(tmp, X, X, ONE, ONE),
- swizzle(tmp, X, ONE, ONE, ONE), 0);
+ /* Compute COS with the same calculation used for SIN, but a
+ * different source range has been mapped to [-1,1] this time.
+ */
- i915_emit_arith(p,
- A0_MUL,
- tmp, A0_DEST_CHANNEL_XYZ, 0,
- swizzle(tmp, X, Y, X, ONE),
- swizzle(tmp, X, X, ONE, ONE), 0);
+ /* tmp.y = abs(tmp.x); {x, abs(x), 0, 0} */
+ i915_emit_arith(p,
+ A0_MAX,
+ tmp, A0_DEST_CHANNEL_Y, 0,
+ swizzle(tmp, ZERO, X, ZERO, ZERO),
+ negate(swizzle(tmp, ZERO, X, ZERO, ZERO), 0, 1, 0, 0),
+ 0);
- i915_emit_arith(p,
- A0_MUL,
- tmp, A0_DEST_CHANNEL_XYZ, 0,
- swizzle(tmp, X, X, Z, ONE),
- swizzle(tmp, Z, ONE, ONE, ONE), 0);
+ /* tmp.y = tmp.y * tmp.x; {x, x * abs(x), 0, 0} */
+ i915_emit_arith(p,
+ A0_MUL,
+ tmp, A0_DEST_CHANNEL_Y, 0,
+ swizzle(tmp, ZERO, X, ZERO, ZERO),
+ tmp,
+ 0);
+ /* tmp.x = tmp.xy DP sin_quad_constants[2].xy */
i915_emit_arith(p,
- A0_DP4,
+ A0_DP3,
+ tmp, A0_DEST_CHANNEL_X, 0,
+ tmp,
+ swizzle(consts1, X, Y, ZERO, ZERO),
+ 0);
+
+ /* tmp.x now contains a first approximation (y). Now, weight it
+ * against tmp.y**2 to get closer.
+ */
+ i915_emit_arith(p,
+ A0_MAX,
+ tmp, A0_DEST_CHANNEL_Y, 0,
+ swizzle(tmp, ZERO, X, ZERO, ZERO),
+ negate(swizzle(tmp, ZERO, X, ZERO, ZERO), 0, 1, 0, 0),
+ 0);
+
+ /* tmp.y = tmp.x * tmp.y - tmp.x; {y, y * abs(y) - y, 0, 0} */
+ i915_emit_arith(p,
+ A0_MAD,
+ tmp, A0_DEST_CHANNEL_Y, 0,
+ swizzle(tmp, ZERO, X, ZERO, ZERO),
+ swizzle(tmp, ZERO, Y, ZERO, ZERO),
+ negate(swizzle(tmp, ZERO, X, ZERO, ZERO), 0, 1, 0, 0));
+
+ /* result = .2225 * tmp.y + tmp.x =.2225(y * abs(y) - y) + y= */
+ i915_emit_arith(p,
+ A0_MAD,
get_result_vector(p, inst),
get_result_flags(inst), 0,
- swizzle(tmp, ONE, Z, Y, X),
- i915_emit_const4fv(p, cos_constants), 0);
-
+ swizzle(consts1, W, W, W, W),
+ swizzle(tmp, Y, Y, Y, Y),
+ swizzle(tmp, X, X, X, X));
break;
case OPCODE_DP3: