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author(no author) <(no author)@138bc75d-0d04-0410-961f-82ee72b054a4>2004-05-10 23:56:25 +0000
committer(no author) <(no author)@138bc75d-0d04-0410-961f-82ee72b054a4>2004-05-10 23:56:25 +0000
commit2bffd6f3bba6e1746f5b7cd524d76b5b2e2eb48e (patch)
tree0d98bcea72447280d7282a59a38a7b203eabc2ef /gcc/testsuite/gcc.dg/tree-ssa-chrec/ssa-chrec-45.c
parent59bc598e01e292d67c32b6ae240b4544d4c234ab (diff)
This commit was manufactured by cvs2svn to create tagapple/gcc-1749
'apple-gcc-1749'. git-svn-id: svn+ssh://gcc.gnu.org/svn/gcc/tags/apple-gcc-1749@81686 138bc75d-0d04-0410-961f-82ee72b054a4
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+/* { dg-do compile } */
+/* { dg-options "-O1 -fscalar-evolutions -fdump-tree-scev-details" } */
+
+/* That's a reduced testcase of one of my favourite simulation programs.
+ This is also known under the name: "Newton's falling apple".
+ The general version is known under the name: "the N-body simulation problem".
+
+ The physics terminology is the best to describe the scalar evolution algorithm:
+ - first determine the initial conditions of the system,
+ - then analyze its evolution.
+*/
+
+double Newton_s_apple ()
+{
+ /* Initial conditions. */
+ double g = 10.0;
+ double speed_z = 0;
+ double altitude = 3000;
+ double delta_t = 0.1;
+ double total_time = 0;
+
+ /* Laws of evolution. */
+ while (altitude > 0.0)
+ {
+ speed_z += g * delta_t;
+ altitude -= speed_z * delta_t;
+ total_time += delta_t;
+ }
+
+ return total_time;
+}
+
+/*
+ speed_z -> {0.0, +, 1.0e+0}_1
+ altitude -> {3.0e+3, +, {(0.0 + 1.0e+0) * 1.00000000000000005551115123125782702118158340454e-1 * -1, +, 1.0e+0 * 1.00000000000000005551115123125782702118158340454e-1 * -1}_1}_1
+
+ When computing evolutions in the "symbolic as long as possible" strategy,
+ the analyzer extracts only the following:
+
+ altitude -> {3.0e+3, +, T.2_11 * -1}_1
+
+*/
+
+/* FIXME. */