ljvmiranda921 commited on
Commit
ebfa1fc
·
verified ·
1 Parent(s): 439d963

Scheduled Commit

Browse files
Czech/71e14e5579474d14be224181330c2d50.jsonl CHANGED
@@ -1,2 +1,3 @@
1
  {"comparison_id": "allenai/OpenThoughts3-full-filtered-science-no-cot-decontam-v2_tmp_ids_92277::smith_vs_teacher", "source_id": "allenai/OpenThoughts3-full-filtered-science-no-cot-decontam-v2_tmp_ids_92277", "language": "Czech", "seed_prompt": "What is the equilibrium constant of the reaction \\n2HI(g) ⇌ H₂(g) + I₂(g) \\nat 444°C? \\n(a) 50 \\n(b) 0.02 \\n(c) 0.143 \\n(d) 3.14", "pair": "smith_vs_teacher", "system_left": "teacher", "system_right": "smith", "overall": "a", "aspects": {"naturalness": "tie_both_good", "cultural_appropriateness": "tie_both_good", "instruction_following": "tie_both_good", "coherence": "strong_a"}, "comment": "", "instance_feedback": "", "winner_system": "teacher", "annotator_id": "dreamy_hypatia", "session_id": "71e14e5579474d14be224181330c2d50", "annotated_at": "2026-09-24T20:45:02", "duration_ms": 521422}
2
  {"comparison_id": "allenai/OpenThoughts3-full-filtered-science-no-cot-decontam-v2_tmp_ids_92557::smith_vs_teacher", "source_id": "allenai/OpenThoughts3-full-filtered-science-no-cot-decontam-v2_tmp_ids_92557", "language": "Czech", "seed_prompt": "In let's say, $SU(3)_L\\times SU(3)_R$ approximate symmetry in QCD, what are the operators that can appear in operator product expansion of current of like and unlike chirality?\nFor reference, you could look at Section 20.5, Weinberg QFT 2. I am not completely understanding how to decide based on symmetry and symmetry breaking pattern which operators can appear. Let me know if you have clearer idea.\n", "pair": "smith_vs_teacher", "system_left": "teacher", "system_right": "smith", "overall": "b", "aspects": {"naturalness": "tie_both_good", "cultural_appropriateness": "tie_both_good", "instruction_following": "strong_b", "coherence": "b"}, "comment": "", "instance_feedback": "", "winner_system": "smith", "annotator_id": "dreamy_hypatia", "session_id": "71e14e5579474d14be224181330c2d50", "annotated_at": "2026-09-24T20:52:53", "duration_ms": 470536}
 
 
1
  {"comparison_id": "allenai/OpenThoughts3-full-filtered-science-no-cot-decontam-v2_tmp_ids_92277::smith_vs_teacher", "source_id": "allenai/OpenThoughts3-full-filtered-science-no-cot-decontam-v2_tmp_ids_92277", "language": "Czech", "seed_prompt": "What is the equilibrium constant of the reaction \\n2HI(g) ⇌ H₂(g) + I₂(g) \\nat 444°C? \\n(a) 50 \\n(b) 0.02 \\n(c) 0.143 \\n(d) 3.14", "pair": "smith_vs_teacher", "system_left": "teacher", "system_right": "smith", "overall": "a", "aspects": {"naturalness": "tie_both_good", "cultural_appropriateness": "tie_both_good", "instruction_following": "tie_both_good", "coherence": "strong_a"}, "comment": "", "instance_feedback": "", "winner_system": "teacher", "annotator_id": "dreamy_hypatia", "session_id": "71e14e5579474d14be224181330c2d50", "annotated_at": "2026-09-24T20:45:02", "duration_ms": 521422}
2
  {"comparison_id": "allenai/OpenThoughts3-full-filtered-science-no-cot-decontam-v2_tmp_ids_92557::smith_vs_teacher", "source_id": "allenai/OpenThoughts3-full-filtered-science-no-cot-decontam-v2_tmp_ids_92557", "language": "Czech", "seed_prompt": "In let's say, $SU(3)_L\\times SU(3)_R$ approximate symmetry in QCD, what are the operators that can appear in operator product expansion of current of like and unlike chirality?\nFor reference, you could look at Section 20.5, Weinberg QFT 2. I am not completely understanding how to decide based on symmetry and symmetry breaking pattern which operators can appear. Let me know if you have clearer idea.\n", "pair": "smith_vs_teacher", "system_left": "teacher", "system_right": "smith", "overall": "b", "aspects": {"naturalness": "tie_both_good", "cultural_appropriateness": "tie_both_good", "instruction_following": "strong_b", "coherence": "b"}, "comment": "", "instance_feedback": "", "winner_system": "smith", "annotator_id": "dreamy_hypatia", "session_id": "71e14e5579474d14be224181330c2d50", "annotated_at": "2026-09-24T20:52:53", "duration_ms": 470536}
3
+ {"comparison_id": "allenai/OpenThoughts3-full-filtered-science-no-cot-decontam-v2_tmp_ids_92709::smith_vs_teacher", "source_id": "allenai/OpenThoughts3-full-filtered-science-no-cot-decontam-v2_tmp_ids_92709", "language": "Czech", "seed_prompt": "Consider a closed container of fixed size in contact with its surroundings maintained at a temperature of 298 K. The inside of this container is partitioned by a frictionless, movable wall into two compartments labeled 1 and 2, with initial volumes of V₁ = 5L and V₂ = 1L, respectively. In compartment 1, there is a gaseous equilibrium mixture of molecules A and B with a total pressure of 1 atm. In compartment 2, there is a gas of only compound C also with a pressure of 1 atm. A piece of metal catalyst of negligible volume is then introduced into compartment 2 which causes gas C to decompose into gaseous product D in an equilibrium reaction. This pushes the wall against compartment 1, which increases V₂ and decreases V₁, also shifting the A = B equilibrium as according to Le Chatelier's principle. The wall is pushed until the reactions in both compartments reach a new state of equilibrium. The standard changes in Gibbs free energies for the two equilibria are: A(g) = 2B(g) AG₁ = -5.183 kJ/mol C(g) = 3D(g) AG2 = -5.636 kJ/mol Assume all gases are ideal.\n\ne) Calculate the initial number of moles for A and B.", "pair": "smith_vs_teacher", "system_left": "teacher", "system_right": "smith", "overall": "tie_both_good", "aspects": {"naturalness": "tie_both_good", "cultural_appropriateness": "tie_both_good", "instruction_following": "tie_both_good", "coherence": "tie_both_good"}, "comment": "", "instance_feedback": "", "winner_system": null, "annotator_id": "dreamy_hypatia", "session_id": "71e14e5579474d14be224181330c2d50", "annotated_at": "2026-09-24T20:57:52", "duration_ms": 298594}