Timeline for Second Law of Dynamics and Pulleys
Current License: CC BY-SA 3.0
10 events
| when toggle format | what | by | license | comment | |
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| Jun 11, 2020 at 9:33 | history | edited | CommunityBot |
Commonmark migration
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| Jul 1, 2016 at 0:22 | answer | added | sammy gerbil | timeline score: 0 | |
| Jun 30, 2016 at 14:41 | vote | accept | DumSpiroSpero | ||
| S Jun 30, 2016 at 7:49 | history | suggested | lucas | CC BY-SA 3.0 |
Format correction.
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| Jun 30, 2016 at 6:35 | answer | added | Farcher | timeline score: 1 | |
| Jun 30, 2016 at 6:19 | answer | added | lucas | timeline score: 3 | |
| Jun 30, 2016 at 5:29 | review | Suggested edits | |||
| S Jun 30, 2016 at 7:49 | |||||
| Jun 30, 2016 at 4:56 | comment | added | user118752 | You can treat block A as a giant moving pulley because: the equations you get truly simplify the system as if A is pulley with (tenion=$2T$) and on the other hand B and C are the blocks hanging on the strings coming out with tension $T$ only. Its a just a like a system with a big pulley (A) attached on one side to ground and on other by one more pulley which is turn is connected on one side by B and the other by C having tensions $T$in both strings connecting B and C, thus automatically the big pulley (A) gets a tension $2T$. | |
| Jun 30, 2016 at 4:21 | review | First posts | |||
| Jun 30, 2016 at 5:11 | |||||
| Jun 30, 2016 at 4:17 | history | asked | DumSpiroSpero | CC BY-SA 3.0 |