VOTING POWER100.00%
DOWNVOTE POWER100.00%
RESOURCE CREDITS100.00%
REPUTATION PROGRESS0.00%
Net Worth
0.080USD
STEEM
0.000STEEM
SBD
0.089SBD
Effective Power
5.001SP
├── Own SP
0.658SP
└── Incoming DelegationsDeleg
+4.343SP
Detailed Balance
| STEEM | ||
| balance | 0.000STEEM | STEEM |
| market_balance | 0.000STEEM | STEEM |
| savings_balance | 0.000STEEM | STEEM |
| reward_steem_balance | 0.000STEEM | STEEM |
| STEEM POWER | ||
| Own SP | 0.658SP | SP |
| Delegated Out | 0.000SP | SP |
| Delegation In | 4.343SP | SP |
| Effective Power | 5.001SP | SP |
| Reward SP (pending) | 0.000SP | SP |
| SBD | ||
| sbd_balance | 0.089SBD | SBD |
| sbd_conversions | 0.000SBD | SBD |
| sbd_market_balance | 0.000SBD | SBD |
| savings_sbd_balance | 0.000SBD | SBD |
| reward_sbd_balance | 0.000SBD | SBD |
{
"balance": "0.000 STEEM",
"savings_balance": "0.000 STEEM",
"reward_steem_balance": "0.000 STEEM",
"vesting_shares": "1072.217883 VESTS",
"delegated_vesting_shares": "0.000000 VESTS",
"received_vesting_shares": "7071.441923 VESTS",
"sbd_balance": "0.089 SBD",
"savings_sbd_balance": "0.000 SBD",
"reward_sbd_balance": "0.000 SBD",
"conversions": []
}Account Info
| name | ulearn |
| id | 683000 |
| rank | 622,989 |
| reputation | 585267593 |
| created | 2018-01-29T16:03:57 |
| recovery_account | steem |
| proxy | None |
| post_count | 8 |
| comment_count | 0 |
| lifetime_vote_count | 0 |
| witnesses_voted_for | 0 |
| last_post | 2018-02-14T18:45:12 |
| last_root_post | 2018-02-14T18:45:12 |
| last_vote_time | 2018-02-15T18:15:42 |
| proxied_vsf_votes | 0, 0, 0, 0 |
| can_vote | 1 |
| voting_power | 0 |
| delayed_votes | 0 |
| balance | 0.000 STEEM |
| savings_balance | 0.000 STEEM |
| sbd_balance | 0.089 SBD |
| savings_sbd_balance | 0.000 SBD |
| vesting_shares | 1072.217883 VESTS |
| delegated_vesting_shares | 0.000000 VESTS |
| received_vesting_shares | 7071.441923 VESTS |
| reward_vesting_balance | 0.000000 VESTS |
| vesting_balance | 0.000 STEEM |
| vesting_withdraw_rate | 0.000000 VESTS |
| next_vesting_withdrawal | 1969-12-31T23:59:59 |
| withdrawn | 0 |
| to_withdraw | 0 |
| withdraw_routes | 0 |
| savings_withdraw_requests | 0 |
| last_account_recovery | 1970-01-01T00:00:00 |
| reset_account | null |
| last_owner_update | 1970-01-01T00:00:00 |
| last_account_update | 2018-01-29T18:23:48 |
| mined | No |
| sbd_seconds | 0 |
| sbd_last_interest_payment | 1970-01-01T00:00:00 |
| savings_sbd_last_interest_payment | 1970-01-01T00:00:00 |
{
"id": 683000,
"name": "ulearn",
"owner": {
"weight_threshold": 1,
"account_auths": [],
"key_auths": [
[
"STM7S2fhhyiBQexq2b6s9S3Tix7eYW482qRsBYGaKMsmFQH2i8pmQ",
1
]
]
},
"active": {
"weight_threshold": 1,
"account_auths": [],
"key_auths": [
[
"STM8FTwbi2fii5f7QrjoibJ4YKrnTr5AcapD8ztQfpQhM445kDbbZ",
1
]
]
},
"posting": {
"weight_threshold": 1,
"account_auths": [],
"key_auths": [
[
"STM7pp6bRQwB1sRPbVkfCQPCVeAfZ4MeRLXF9Zd16JsaYmAeZZEyr",
1
]
]
},
"memo_key": "STM55E3qtTRQha1v1V9B69UGeaKkSVYRssdjeGgfQu7yuK2sK48t2",
"json_metadata": "{\"profile\":{\"cover_image\":\"https://www.nasa.gov/sites/default/files/images/649694main_pia15417-43_full.jpg\",\"about\":\"All things STEM, history, and some other stuff\",\"location\":\"United States\",\"profile_image\":\"https://cdn.pixabay.com/photo/2016/09/16/19/12/atom-1674878_640.png\"}}",
"posting_json_metadata": "{\"profile\":{\"cover_image\":\"https://www.nasa.gov/sites/default/files/images/649694main_pia15417-43_full.jpg\",\"about\":\"All things STEM, history, and some other stuff\",\"location\":\"United States\",\"profile_image\":\"https://cdn.pixabay.com/photo/2016/09/16/19/12/atom-1674878_640.png\"}}",
"proxy": "",
"last_owner_update": "1970-01-01T00:00:00",
"last_account_update": "2018-01-29T18:23:48",
"created": "2018-01-29T16:03:57",
"mined": false,
"recovery_account": "steem",
"last_account_recovery": "1970-01-01T00:00:00",
"reset_account": "null",
"comment_count": 0,
"lifetime_vote_count": 0,
"post_count": 8,
"can_vote": true,
"voting_manabar": {
"current_mana": "8143659806",
"last_update_time": 1779090399
},
"downvote_manabar": {
"current_mana": 2035914951,
"last_update_time": 1779090399
},
"voting_power": 0,
"balance": "0.000 STEEM",
"savings_balance": "0.000 STEEM",
"sbd_balance": "0.089 SBD",
"sbd_seconds": "0",
"sbd_seconds_last_update": "2018-02-14T16:54:54",
"sbd_last_interest_payment": "1970-01-01T00:00:00",
"savings_sbd_balance": "0.000 SBD",
"savings_sbd_seconds": "0",
"savings_sbd_seconds_last_update": "1970-01-01T00:00:00",
"savings_sbd_last_interest_payment": "1970-01-01T00:00:00",
"savings_withdraw_requests": 0,
"reward_sbd_balance": "0.000 SBD",
"reward_steem_balance": "0.000 STEEM",
"reward_vesting_balance": "0.000000 VESTS",
"reward_vesting_steem": "0.000 STEEM",
"vesting_shares": "1072.217883 VESTS",
"delegated_vesting_shares": "0.000000 VESTS",
"received_vesting_shares": "7071.441923 VESTS",
"vesting_withdraw_rate": "0.000000 VESTS",
"next_vesting_withdrawal": "1969-12-31T23:59:59",
"withdrawn": 0,
"to_withdraw": 0,
"withdraw_routes": 0,
"curation_rewards": 0,
"posting_rewards": 48,
"proxied_vsf_votes": [
0,
0,
0,
0
],
"witnesses_voted_for": 0,
"last_post": "2018-02-14T18:45:12",
"last_root_post": "2018-02-14T18:45:12",
"last_vote_time": "2018-02-15T18:15:42",
"post_bandwidth": 0,
"pending_claimed_accounts": 0,
"vesting_balance": "0.000 STEEM",
"reputation": 585267593,
"transfer_history": [],
"market_history": [],
"post_history": [],
"vote_history": [],
"other_history": [],
"witness_votes": [],
"tags_usage": [],
"guest_bloggers": [],
"rank": 622989
}Withdraw Routes
| Incoming | Outgoing |
|---|---|
Empty | Empty |
{
"incoming": [],
"outgoing": []
}From Date
To Date
2026/05/18 07:46:39
2026/05/18 07:46:39
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 7071.441923 VESTS |
| Transaction Info | Block #106152440/Trx 433821cc310e59025a499ee376640502a483ba64 |
View Raw JSON Data
{
"block": 106152440,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "7071.441923 VESTS"
}
],
"op_in_trx": 0,
"timestamp": "2026-05-18T07:46:39",
"trx_id": "433821cc310e59025a499ee376640502a483ba64",
"trx_in_block": 1,
"virtual_op": 0
}2026/05/13 10:21:03
2026/05/13 10:21:03
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 4359.231518 VESTS |
| Transaction Info | Block #106012236/Trx e9e357e0a148cda315ad9991ea1f345476cb14ba |
View Raw JSON Data
{
"block": 106012236,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "4359.231518 VESTS"
}
],
"op_in_trx": 0,
"timestamp": "2026-05-13T10:21:03",
"trx_id": "e9e357e0a148cda315ad9991ea1f345476cb14ba",
"trx_in_block": 3,
"virtual_op": 0
}2026/04/26 06:56:36
2026/04/26 06:56:36
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 7083.957679 VESTS |
| Transaction Info | Block #105519889/Trx c03191739537d5048a038bb073b761b6538d654c |
View Raw JSON Data
{
"block": 105519889,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "7083.957679 VESTS"
}
],
"op_in_trx": 0,
"timestamp": "2026-04-26T06:56:36",
"trx_id": "c03191739537d5048a038bb073b761b6538d654c",
"trx_in_block": 2,
"virtual_op": 0
}2026/01/24 04:00:39
2026/01/24 04:00:39
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 4400.778337 VESTS |
| Transaction Info | Block #102876012/Trx 8ba8cfdb01f9d6247446e1642274458f80ffb9f6 |
View Raw JSON Data
{
"block": 102876012,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "4400.778337 VESTS"
}
],
"op_in_trx": 0,
"timestamp": "2026-01-24T04:00:39",
"trx_id": "8ba8cfdb01f9d6247446e1642274458f80ffb9f6",
"trx_in_block": 1,
"virtual_op": 0
}2024/12/17 23:09:12
2024/12/17 23:09:12
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 4564.997534 VESTS |
| Transaction Info | Block #91322203/Trx e83c694b800dfdc146b801aaba10baf0c17e1997 |
View Raw JSON Data
{
"block": 91322203,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "4564.997534 VESTS"
}
],
"op_in_trx": 0,
"timestamp": "2024-12-17T23:09:12",
"trx_id": "e83c694b800dfdc146b801aaba10baf0c17e1997",
"trx_in_block": 2,
"virtual_op": 0
}2023/11/14 14:47:51
2023/11/14 14:47:51
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 4734.131066 VESTS |
| Transaction Info | Block #79876291/Trx 04f8892128f08d0df3d1655c342344559c161fe3 |
View Raw JSON Data
{
"block": 79876291,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "4734.131066 VESTS"
}
],
"op_in_trx": 0,
"timestamp": "2023-11-14T14:47:51",
"trx_id": "04f8892128f08d0df3d1655c342344559c161fe3",
"trx_in_block": 2,
"virtual_op": 0
}2023/09/22 12:08:15
2023/09/22 12:08:15
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 7671.039852 VESTS |
| Transaction Info | Block #78364952/Trx 5878862a5cc7ff162522ceac491ce8b618db959c |
View Raw JSON Data
{
"block": 78364952,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "7671.039852 VESTS"
}
],
"op_in_trx": 0,
"timestamp": "2023-09-22T12:08:15",
"trx_id": "5878862a5cc7ff162522ceac491ce8b618db959c",
"trx_in_block": 3,
"virtual_op": 0
}2022/11/03 19:24:12
2022/11/03 19:24:12
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 7893.091290 VESTS |
| Transaction Info | Block #69122458/Trx 7d723a31517b388f3960e955898d44b69af3615e |
View Raw JSON Data
{
"block": 69122458,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "7893.091290 VESTS"
}
],
"op_in_trx": 0,
"timestamp": "2022-11-03T19:24:12",
"trx_id": "7d723a31517b388f3960e955898d44b69af3615e",
"trx_in_block": 0,
"virtual_op": 0
}2022/01/18 00:27:21
2022/01/18 00:27:21
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 8113.198891 VESTS |
| Transaction Info | Block #60825533/Trx e94981cbc67b34f74567f30af6b36bc350d99183 |
View Raw JSON Data
{
"block": 60825533,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "8113.198891 VESTS"
}
],
"op_in_trx": 0,
"timestamp": "2022-01-18T00:27:21",
"trx_id": "e94981cbc67b34f74567f30af6b36bc350d99183",
"trx_in_block": 5,
"virtual_op": 0
}2021/06/14 07:34:36
2021/06/14 07:34:36
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 8297.393179 VESTS |
| Transaction Info | Block #54615778/Trx 3ec0980945b6d53bc3306fb0ccdfec46f3d45d15 |
View Raw JSON Data
{
"block": 54615778,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "8297.393179 VESTS"
}
],
"op_in_trx": 0,
"timestamp": "2021-06-14T07:34:36",
"trx_id": "3ec0980945b6d53bc3306fb0ccdfec46f3d45d15",
"trx_in_block": 0,
"virtual_op": 0
}2020/12/11 17:45:27
2020/12/11 17:45:27
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 8484.815153 VESTS |
| Transaction Info | Block #49362995/Trx 75d5f57e98d33ae1811f6bffb0cabd9bf8679648 |
View Raw JSON Data
{
"block": 49362995,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "8484.815153 VESTS"
}
],
"op_in_trx": 0,
"timestamp": "2020-12-11T17:45:27",
"trx_id": "75d5f57e98d33ae1811f6bffb0cabd9bf8679648",
"trx_in_block": 1,
"virtual_op": 0
}2020/12/06 11:20:42
2020/12/06 11:20:42
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 1912.543513 VESTS |
| Transaction Info | Block #49214510/Trx 466aa606e6bace1996f05b112cbb24a975d2884b |
View Raw JSON Data
{
"block": 49214510,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "1912.543513 VESTS"
}
],
"op_in_trx": 0,
"timestamp": "2020-12-06T11:20:42",
"trx_id": "466aa606e6bace1996f05b112cbb24a975d2884b",
"trx_in_block": 3,
"virtual_op": 0
}2020/12/05 21:23:21
2020/12/05 21:23:21
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 8491.023007 VESTS |
| Transaction Info | Block #49198079/Trx 25d7efb13b85947581e581132812d547d7e2cae8 |
View Raw JSON Data
{
"block": 49198079,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "8491.023007 VESTS"
}
],
"op_in_trx": 0,
"timestamp": "2020-12-05T21:23:21",
"trx_id": "25d7efb13b85947581e581132812d547d7e2cae8",
"trx_in_block": 1,
"virtual_op": 0
}2020/11/03 05:21:45
2020/11/03 05:21:45
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 1920.017158 VESTS |
| Transaction Info | Block #48273960/Trx f5cfc1593fdcd01213c2d5df62cd99640cc7521d |
View Raw JSON Data
{
"block": 48273960,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "1920.017158 VESTS"
}
],
"op_in_trx": 0,
"timestamp": "2020-11-03T05:21:45",
"trx_id": "f5cfc1593fdcd01213c2d5df62cd99640cc7521d",
"trx_in_block": 1,
"virtual_op": 0
}2020/05/09 12:25:09
2020/05/09 12:25:09
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 8693.828366 VESTS |
| Transaction Info | Block #43224861/Trx 0b78f5eb8bc6331139ce4a72ebdfa1984f1c992e |
View Raw JSON Data
{
"block": 43224861,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "8693.828366 VESTS"
}
],
"op_in_trx": 0,
"timestamp": "2020-05-09T12:25:09",
"trx_id": "0b78f5eb8bc6331139ce4a72ebdfa1984f1c992e",
"trx_in_block": 10,
"virtual_op": 0
}2020/05/08 17:01:06
2020/05/08 17:01:06
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 1953.311140 VESTS |
| Transaction Info | Block #43202128/Trx 988feb5d5fe34475227cc6cbfb0f84eb0464dc77 |
View Raw JSON Data
{
"block": 43202128,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "1953.311140 VESTS"
}
],
"op_in_trx": 0,
"timestamp": "2020-05-08T17:01:06",
"trx_id": "988feb5d5fe34475227cc6cbfb0f84eb0464dc77",
"trx_in_block": 65,
"virtual_op": 0
}2020/04/17 15:53:09
2020/04/17 15:53:09
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 8705.856540 VESTS |
| Transaction Info | Block #42611669/Trx 70d28983929b55a4c79d9c4f86d05a00d135aebd |
View Raw JSON Data
{
"block": 42611669,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "8705.856540 VESTS"
}
],
"op_in_trx": 0,
"timestamp": "2020-04-17T15:53:09",
"trx_id": "70d28983929b55a4c79d9c4f86d05a00d135aebd",
"trx_in_block": 31,
"virtual_op": 0
}2020/01/29 21:07:36
2020/01/29 21:07:36
| author | steemitboard |
| body | Congratulations @ulearn! You received a personal award! <table><tr><td>https://steemitimages.com/70x70/http://steemitboard.com/@ulearn/birthday2.png</td><td>Happy Birthday! - You are on the Steem blockchain for 2 years!</td></tr></table> <sub>_You can view [your badges on your Steem Board](https://steemitboard.com/@ulearn) and compare to others on the [Steem Ranking](https://steemitboard.com/ranking/index.php?name=ulearn)_</sub> ###### [Vote for @Steemitboard as a witness](https://v2.steemconnect.com/sign/account-witness-vote?witness=steemitboard&approve=1) to get one more award and increased upvotes! |
| json metadata | {"image":["https://steemitboard.com/img/notify.png"]} |
| parent author | ulearn |
| parent permlink | making-the-perfect-valentine-with-calculus |
| permlink | steemitboard-notify-ulearn-20200129t210735000z |
| title | |
| Transaction Info | Block #40362460/Trx 1aae90dd58031df182cb0068a82183c5f18680b3 |
View Raw JSON Data
{
"block": 40362460,
"op": [
"comment",
{
"author": "steemitboard",
"body": "Congratulations @ulearn! You received a personal award!\n\n<table><tr><td>https://steemitimages.com/70x70/http://steemitboard.com/@ulearn/birthday2.png</td><td>Happy Birthday! - You are on the Steem blockchain for 2 years!</td></tr></table>\n\n<sub>_You can view [your badges on your Steem Board](https://steemitboard.com/@ulearn) and compare to others on the [Steem Ranking](https://steemitboard.com/ranking/index.php?name=ulearn)_</sub>\n\n\n###### [Vote for @Steemitboard as a witness](https://v2.steemconnect.com/sign/account-witness-vote?witness=steemitboard&approve=1) to get one more award and increased upvotes!",
"json_metadata": "{\"image\":[\"https://steemitboard.com/img/notify.png\"]}",
"parent_author": "ulearn",
"parent_permlink": "making-the-perfect-valentine-with-calculus",
"permlink": "steemitboard-notify-ulearn-20200129t210735000z",
"title": ""
}
],
"op_in_trx": 0,
"timestamp": "2020-01-29T21:07:36",
"trx_id": "1aae90dd58031df182cb0068a82183c5f18680b3",
"trx_in_block": 2,
"virtual_op": 0
}2019/05/14 06:32:15
2019/05/14 06:32:15
| delegatee | ulearn |
| delegator | steem |
| vesting shares | 8901.438287 VESTS |
| Transaction Info | Block #32893023/Trx 95a61a24aed792622111a0316781283191b8db68 |
View Raw JSON Data
{
"block": 32893023,
"op": [
"delegate_vesting_shares",
{
"delegatee": "ulearn",
"delegator": "steem",
"vesting_shares": "8901.438287 VESTS"
}
],
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}ulearnupvoted (100.00%) @melanie2 / lets-take-a-walk2018/02/15 18:15:42
ulearnupvoted (100.00%) @melanie2 / lets-take-a-walk
2018/02/15 18:15:42
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}ulearnupvoted (100.00%) @paulyaces76 / should-we-move-to-venezuela-to-mine2018/02/15 18:14:21
ulearnupvoted (100.00%) @paulyaces76 / should-we-move-to-venezuela-to-mine
2018/02/15 18:14:21
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}ulearnupvoted (100.00%) @mindtrap / smiley-people-are-happy-people2018/02/15 18:12:33
ulearnupvoted (100.00%) @mindtrap / smiley-people-are-happy-people
2018/02/15 18:12:33
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}ulearnupvoted (100.00%) @ulearn / making-the-perfect-valentine-with-calculus2018/02/15 08:27:42
ulearnupvoted (100.00%) @ulearn / making-the-perfect-valentine-with-calculus
2018/02/15 08:27:42
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}ulearnpublished a new post: making-the-perfect-valentine-with-calculus2018/02/14 18:45:12
ulearnpublished a new post: making-the-perfect-valentine-with-calculus
2018/02/14 18:45:12
| author | ulearn |
| body |  [Source](https://pixabay.com/en/heart-card-pastels-figure-762564/) Valentine's Day is a time for happiness and a time for being with loved ones. Or maybe not. From New Year's Day to Valentine's Day, people think about breaking up more than any other time of the year [[1]](http://abcnews.go.com/US/story?id=2863607&page=1). So, although it's Valentine’s Day, there may be a little bit of sadness brewing. However, fear not! The Valentines that we will be making are useful to both those with and without love in their life. If you have a special someone in your life, then you will be able to give them a PERFECT Valentine made with MATH. If you are without a special someone, come with me. We will numb our brains on something better than alcohol. You know I’m talking about Calculus. And who knows? Maybe this will help you hook up with a math minded individual. Alright, so what is the most important aspect of the Valentine? Is it the message? Is it the card itself? Is it the chocolate and/or flowers that goes with it? Absolutely not! It is the heart drawing. Every Valentine needs a heart and if you can draw the PERFECT heart then you will have the PERFECT Valentine. How can we draw the perfect heart? With online graphing tools. Duh. I recommend using [Desmos](https://www.desmos.com/calculator/ksjcpazwa9). If you have taken any algebra courses, you may be wondering how graphing a heart is even possible. After all, if you were to put a heart on graph paper you would notice that it does not pass the vertical line test. However, failing the vertical line test ONLY proves that the tested equation does not have y as a function of x. This means we can graph just about anything using the correct perimeters. For example, y^2 = x does not pass the vertical line test, but it is easily graphed by plugging in points.  ## Alright, let us begin! Equation 1:   Alright, let’s start this off with something relatively easy. This equation is a good start. At its core, it is just a variation of an equation for a circle (x^2+y^2=1). This equation is also in simple y/x (Cartesian) coordinates so there isn’t too much going on. However, this graph proves less is more. The easy format makes it easy to plot, and you could graph it at home right now if you really wanted to. I would rate this equation as 8 hearts out of 10. Equation 2:   This equation is for a cardioid named after, you guessed it, its heart-like shape. The cardioid appears in calculus quite often and any mathematician is sure to recognize it. However, the cardioid is in polar coordinates making it more difficult to graph. Polar coordinates are in terms of “theta” and “r.” If you are unfamiliar with polar coordinates, you may be wondering what “r” and “theta” represent. r^2 = x^2 + y^2 and theta is the angle of a right triangle if x and y were sides.  [Source](https://en.wikipedia.org/wiki/Polar_coordinate_system#/media/File:Polar_to_cartesian.svg) I know it’s confusing, but that’s why its calculus. (Is your mind going numb yet?) Unfortunately, the cardioid is a little ugly compared to its competitor. It could barely pass as a heart. With all this in mind, I give the cardioid 5 hearts out of 10. Equation 3:  x=16(sin(t))^3, y=13cos(t)-5cos(2t)-2cos(3t)-cos(4t)  So, this last one is a little bit more complex for sure. You may have noticed that this equation is in terms of “t.” That is because it is in parametric coordinates. Graphing this is probably easier than what you may be thinking. Pick any value for “t” and plug it in. Solve for the y/x values. Then, use the solved values to graph. The equation just looks worse than it actually is. In reality, the equation given is really just another manipulation of a circle. The parametric equation for a circle is sin(t) = x, cos(t) = y. This is obviously a lot messier, but look at that perfect heart. It is voluptuous and curvy. Indeed, this heart is something special. I give it 10 hearts out of 10 and I think it is the perfect heart for which we are all looking. Now that we have several candidates, its time to make a Valentine. Get out any kind of paper (preferable graphing paper) and write your favorite equation and graph it. Your done! You just created the perfect Valentine. Anything else, like a meaningful message, would just get in the way. Trust in the heart and let it do its magic. I guarantee that you will become instantly more attractive and you will feel much more accomplished! Obviously, I have not listed every equation that yields a heart when graphed. There might be some easier ones and I am sure that there are harder ones. Also, by using the z-axis it is possible to make a 3-Dimensional heart… but let’s not do that today (maybe next year). Also, all of the graphs are pretty fun to play around with. Sometimes little changes can dramatically change the shape. There are some interesting links below. Thanks for reading and Happy Valentine’s Day. ___________________________________________________________________________________________________ *I made most of the photos with Desmos, an awesome online graphing tool. Also, any comments or feedback is always appreciated.* ___________________________________________________________________________________________________ Sources: http://www.mathematische-basteleien.de/heart.htm http://mathworld.wolfram.com/HeartCurve.html https://www.desmos.com/calculator/ksjcpazwa9 http://abcnews.go.com/US/story?id=2863607&page=1 |
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"body": "\n[Source](https://pixabay.com/en/heart-card-pastels-figure-762564/)\n\nValentine's Day is a time for happiness and a time for being with loved ones. Or maybe not. From New Year's Day to Valentine's Day, people think about breaking up more than any other time of the year [[1]](http://abcnews.go.com/US/story?id=2863607&page=1). So, although it's Valentine’s Day, there may be a little bit of sadness brewing. However, fear not! The Valentines that we will be making are useful to both those with and without love in their life. If you have a special someone in your life, then you will be able to give them a PERFECT Valentine made with MATH. If you are without a special someone, come with me. We will numb our brains on something better than alcohol. You know I’m talking about Calculus. And who knows? Maybe this will help you hook up with a math minded individual.\n\nAlright, so what is the most important aspect of the Valentine? Is it the message? Is it the card itself? Is it the chocolate and/or flowers that goes with it? Absolutely not! It is the heart drawing. Every Valentine needs a heart and if you can draw the PERFECT heart then you will have the PERFECT Valentine.\n\nHow can we draw the perfect heart? With online graphing tools. Duh. I recommend using [Desmos](https://www.desmos.com/calculator/ksjcpazwa9).\n\nIf you have taken any algebra courses, you may be wondering how graphing a heart is even possible. After all, if you were to put a heart on graph paper you would notice that it does not pass the vertical line test. However, failing the vertical line test ONLY proves that the tested equation does not have y as a function of x. This means we can graph just about anything using the correct perimeters. For example, y^2 = x does not pass the vertical line test, but it is easily graphed by plugging in points.\n\n\n## Alright, let us begin!\n\nEquation 1:\n\n\n\nAlright, let’s start this off with something relatively easy. This equation is a good start. At its core, it is just a variation of an equation for a circle (x^2+y^2=1). This equation is also in simple y/x (Cartesian) coordinates so there isn’t too much going on. However, this graph proves less is more. The easy format makes it easy to plot, and you could graph it at home right now if you really wanted to. I would rate this equation as 8 hearts out of 10.\n\nEquation 2:\n\n\n\nThis equation is for a cardioid named after, you guessed it, its heart-like shape. The cardioid appears in calculus quite often and any mathematician is sure to recognize it. However, the cardioid is in polar coordinates making it more difficult to graph. Polar coordinates are in terms of “theta” and “r.” If you are unfamiliar with polar coordinates, you may be wondering what “r” and “theta” represent. r^2 = x^2 + y^2 and theta is the angle of a right triangle if x and y were sides.\n\n[Source](https://en.wikipedia.org/wiki/Polar_coordinate_system#/media/File:Polar_to_cartesian.svg)\n I know it’s confusing, but that’s why its calculus. (Is your mind going numb yet?) Unfortunately, the cardioid is a little ugly compared to its competitor. It could barely pass as a heart. With all this in mind, I give the cardioid 5 hearts out of 10.\n\nEquation 3: \n\nx=16(sin(t))^3, y=13cos(t)-5cos(2t)-2cos(3t)-cos(4t)\n\n\nSo, this last one is a little bit more complex for sure. You may have noticed that this equation is in terms of “t.” That is because it is in parametric coordinates. Graphing this is probably easier than what you may be thinking. Pick any value for “t” and plug it in. Solve for the y/x values. Then, use the solved values to graph. \nThe equation just looks worse than it actually is. In reality, the equation given is really just another manipulation of a circle. The parametric equation for a circle is sin(t) = x, cos(t) = y. This is obviously a lot messier, but look at that perfect heart. It is voluptuous and curvy. Indeed, this heart is something special. I give it 10 hearts out of 10 and I think it is the perfect heart for which we are all looking.\n\t\nNow that we have several candidates, its time to make a Valentine. Get out any kind of paper (preferable graphing paper) and write your favorite equation and graph it. Your done! You just created the perfect Valentine. Anything else, like a meaningful message, would just get in the way. Trust in the heart and let it do its magic. I guarantee that you will become instantly more attractive and you will feel much more accomplished!\n\nObviously, I have not listed every equation that yields a heart when graphed. 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}ulearnupvoted (100.00%) @marjinaal / 20180214t165537520z-post2018/02/14 16:57:15
ulearnupvoted (100.00%) @marjinaal / 20180214t165537520z-post
2018/02/14 16:57:15
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}ulearnfollowed @cryptoriddler2018/02/14 16:56:36
ulearnfollowed @cryptoriddler
2018/02/14 16:56:36
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}ulearnclaimed reward balance: 0.089 SBD, 0.030 SP2018/02/14 16:54:54
ulearnclaimed reward balance: 0.089 SBD, 0.030 SP
2018/02/14 16:54:54
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}ulearnupvoted (100.00%) @adsactly / adsactly-awareness-why-there-are-hidden-chemicals-in-our-food2018/02/14 03:59:54
ulearnupvoted (100.00%) @adsactly / adsactly-awareness-why-there-are-hidden-chemicals-in-our-food
2018/02/14 03:59:54
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2018/02/14 03:59:27
| author | ulearn |
| body | Most people don't really know everything they are eating. A lot of table salt producers add small amounts of potassium iodide in with the regular salt. It's always fun to look at what you are really eating. |
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}ulearnupvoted (100.00%) @janusface / all-that-glitters-is-not-gold-it-could-be-a-ripe-fruit-too2018/02/14 03:52:09
ulearnupvoted (100.00%) @janusface / all-that-glitters-is-not-gold-it-could-be-a-ripe-fruit-too
2018/02/14 03:52:09
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}ulearnreceived 0.077 SBD, 0.026 SP author reward for @ulearn / the-thinnest-material-ever2018/02/09 20:38:36
ulearnreceived 0.077 SBD, 0.026 SP author reward for @ulearn / the-thinnest-material-ever
2018/02/09 20:38:36
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}ulearnupvoted (100.00%) @ulearn / the-thinnest-material-ever2018/02/07 08:45:33
ulearnupvoted (100.00%) @ulearn / the-thinnest-material-ever
2018/02/07 08:45:33
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}ulearnreceived 0.012 SBD, 0.004 SP author reward for @ulearn / re-sustainablyyours-does-eating-carrots-really-help-your-eyes-20180129t233130371z2018/02/05 23:31:36
ulearnreceived 0.012 SBD, 0.004 SP author reward for @ulearn / re-sustainablyyours-does-eating-carrots-really-help-your-eyes-20180129t233130371z
2018/02/05 23:31:36
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}sustainablyyoursupvoted (100.00%) @ulearn / the-thinnest-material-ever2018/02/03 00:33:57
sustainablyyoursupvoted (100.00%) @ulearn / the-thinnest-material-ever
2018/02/03 00:33:57
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2018/02/02 20:55:33
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}ulearnpublished a new post: the-thinnest-material-ever2018/02/02 20:38:36
ulearnpublished a new post: the-thinnest-material-ever
2018/02/02 20:38:36
| author | ulearn |
| body | # **The Miracle Material** Andre Geim, a physicist, was a brilliant researcher working for the University of Manchester. Besides working on just one research project, Geim took on many temporary projects. He called them “Friday night experiments.” Our story begins in 2002, when Geim assigned a graduate student one of these “Friday night experiments” to help him get acquainted with the lab. The experiment was simple. Try to get graphite as thin as possible. Geim also worked on the experiment with his colleagues, and in a sudden moment of brilliance, a colleague brought Geim a simple piece of scotch tape that was recently taken from a graphite surface [[1]](http://www.mypearsonstore.com/bookstore/chemistry-structure-and-properties-0134293932). By 2004, two men, Andre Geim and his closest colleague, Konstantin Novoselov had isolated the flakes on the scotch tape and studied them. They had discovered something truly amazing. They had discovered a material that was only one atom thick (Yes, the thinnest material). This material was also as strong as it was thin. Upon further examination, this material was 200 times the strength of steel and only one-sixteenth as dense. It could bend, stretch, flip, or be folded[[2]](http://www.graphene.manchester.ac.uk/explore/what-can-graphene-do/). Yes, I am talking about **graphene**. ## **What is graphene?** ###### **Structure** Graphene’s exceptionality is best understood through its crystalline lattices. A crystalline lattice is the natural way the atoms of a crystalline solid aggregate to minimize their energy[[1]](http://www.mypearsonstore.com/bookstore/chemistry-structure-and-properties-0134293932). You can think of a lattice as a crystal structure. Different lattice structures change the properties of the materials they make up. A few examples of materials with crystalline lattices are quartz, ice, salt, and diamonds. Here is a picture of graphene’s lattice.  [Image Source](https://en.wikipedia.org/wiki/Graphene#/media/File:Graphen.jpg) Graphene has a simple 2-dimensional hexagonal lattice structure. Usually, lattice structures are pretty difficult to understand because most are 3-dimensional, but graphene’s is 2-dimensional. Graphene’s 2-dimensional structure is one of the two reasons why graphene is so strong. All the bonds in graphene are on a singular plane. This means that if you were to somehow pull on a graphene nanoribbon, all (or most) the bonds would be working against you[[3]](https://www.chemguide.co.uk/atoms/structures/giantcov.html). For reference, steel is typically a body centered lattice and diamonds have a special kind of lattice structure called diamond cubic. Here are some pictures. https://upload.wikimedia.org/wikipedia/commons/2/22/Diamond_Cubic-F_lattice_animation.gif [Diamond Cubic](https://en.wikipedia.org/wiki/Diamond_cubic#/media/File:Diamond_Cubic-F_lattice_animation.gif)  [Body centered](https://en.wikipedia.org/wiki/Cubic_crystal_system#/media/File:CsCl_crystal.png) Steel has a greater packing efficiency than graphene (as seen above). An important thing to note is compactness doesn’t necessarily mean strength. However, compactness is directly correlated with density. This is why the open lattice of graphene is one-sixteenth the density of steel. ###### **Bonds** In case you haven’t realized it yet, graphene is completely made up of carbon. These carbon atoms are held together in their lattice by powerful covalent bonds, the same bonds used in diamonds. Because of these powerful bonds, graphene has a high melting point[[3]](https://www.chemguide.co.uk/atoms/structures/giantcov.html). A key difference between the carbon atoms of diamond and the carbon atoms of graphene is their hybridization. Graphene has an sp^2 hybridization while diamond has an sp^3 hybridization. For our purposes, hybridization determines how many bonds carbon will have. Sp^2 means carbon will bond with 3 atoms and sp^3 means carbon will bond with four [[4]](http://chemed.chem.purdue.edu/genchem/topicreview/bp/ch10/carbon.php). Carbon typically likes to have four bonds because it has four valence electrons. Graphene’s carbon atoms only use three out of their four valence electrons on bonds. What, you may be wondering, is this one, lone electron doing? Well, this electron is a free-floating electron and it grants graphene the ability to conduct electricity. This is a very important property. Sometimes, the free-floating electrons will bond with another, making the bonds within graphene even stronger. [[3]](https://www.chemguide.co.uk/atoms/structures/giantcov.html)(Because even electrons want friends too…) https://upload.wikimedia.org/wikipedia/commons/thumb/1/17/Covalent.svg/334px-Covalent.svg.png [Covalent Bonds in Methane](https://en.wikipedia.org/wiki/Covalent_bond#/media/File:Covalent.svg) Well, if graphene is so strong, why does graphite seem so weak? After all, graphite is just stacked graphene. Well, graphene doesn’t bond well when stacked. Instead of strong covalent bonds, graphene uses a weak and pitiful intermolecular force known as London dispersion forces [[5]](https://en.wikipedia.org/wiki/Graphite). Just about every molecule experiences these forces, and they are the reason why pencils can write. A good analogy is think of graphite as a stack of cards. The individual card is strong, but this does not translate to a durable stack of cards. Instead, they will slide off one another with just a gentle push.  [Image Source](https://www.pexels.com/photo/playing-game-card-58562/) ###### **Is graphene useful?** Hopefully by now, you have a good idea of why graphene can be so strong but also so light and flexible. But, like my high school English teacher would say about my papers, “so what?” (I got a C in English that year). Is graphene useful? The answer is obviously yes. Graphene has many qualities which makes it useful in a broad range of subjects. Remember when I told you it was a good conductor. Graphene has a strong future in electronics. Studies show that it could be used for one of the most energy efficient transistors ever [[6]](http://www.thegraphenecouncil.org/?page=ElectronicsJAN15). Others foresee graphene being used in flexible/foldable touchscreens [[2]](http://www.graphene.manchester.ac.uk/explore/the-applications/electronics/). It doesn’t stop at electronics. Because of graphene’s high melting point, there is talk of using graphene in the automotive industry which could save as much as 30% to 50% in automotive structural weight while also adding more safety to the operator.[[7]](http://articles.sae.org/13441/). In biomedical engineering, there is talk of using graphene for tissue regeneration[[8]](http://pubs.rsc.org/en/content/articlelanding/2013/tb/c3tb20405g#!divAbstract). Honestly, the uses for graphene are limited only by our imagination. Are we already using it? What are we using graphene for right now? Well, graphene is being used in censors. Think about it. Every atom of graphene is exposed to its environment [[3]](htp://www.graphene.manchester.ac.uk/explore/the-applications/sensors/0). When applied, graphene can make for incredibly accurate censors that can distinguish materials down to the molecule. If you want to get a glimpse of the future, googling “potential uses for graphene,” is probably a good way to do it. Graphene is still a relatively new discovery, but I would classify it as a major discovery. I am excited to see what becomes of graphene and I hope you are too. ___________________________________________________________________________________________________ *(Hey! Thank you for reading! I had a lot of fun researching and writing this post. If you have any feedback for me, you can comment below. That is always helpful and appreciated. My next post will be sometime this weekend. Thanks again for reading and I hope to see you again soon! -ulearn)* ___________________________________________________________________________________________________ Sources http://www.mypearsonstore.com/bookstore/chemistry-structure-and-properties-0134293932 http://www.graphene.manchester.ac.uk/explore/the-applications/electronics/ https://www.chemguide.co.uk/atoms/structures/giantcov.html http://chemed.chem.purdue.edu/genchem/topicreview/bp/ch10/carbon.php https://en.wikipedia.org/wiki/Graphite http://www.thegraphenecouncil.org/?page=ElectronicsJAN15 http://articles.sae.org/13441/ http://pubs.rsc.org/en/content/articlelanding/2013/tb/c3tb20405g#!divAbstract |
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| permlink | the-thinnest-material-ever |
| title | The THINNEST material ever! |
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"body": "# **The Miracle Material**\n\nAndre Geim, a physicist, was a brilliant researcher working for the University of Manchester. Besides working on just one research project, Geim took on many temporary projects. He called them “Friday night experiments.” Our story begins in 2002, when Geim assigned a graduate student one of these “Friday night experiments” to help him get acquainted with the lab. The experiment was simple. Try to get graphite as thin as possible. Geim also worked on the experiment with his colleagues, and in a sudden moment of brilliance, a colleague brought Geim a simple piece of scotch tape that was recently taken from a graphite surface [[1]](http://www.mypearsonstore.com/bookstore/chemistry-structure-and-properties-0134293932). By 2004, two men, Andre Geim and his closest colleague, Konstantin Novoselov had isolated the flakes on the scotch tape and studied them. They had discovered something truly amazing. They had discovered a material that was only one atom thick (Yes, the thinnest material). This material was also as strong as it was thin. Upon further examination, this material was 200 times the strength of steel and only one-sixteenth as dense. It could bend, stretch, flip, or be folded[[2]](http://www.graphene.manchester.ac.uk/explore/what-can-graphene-do/). Yes, I am talking about **graphene**.\n\n## **What is graphene?**\n\n###### **Structure**\nGraphene’s exceptionality is best understood through its crystalline lattices. A crystalline lattice is the natural way the atoms of a crystalline solid aggregate to minimize their energy[[1]](http://www.mypearsonstore.com/bookstore/chemistry-structure-and-properties-0134293932). You can think of a lattice as a crystal structure. Different lattice structures change the properties of the materials they make up. A few examples of materials with crystalline lattices are quartz, ice, salt, and diamonds. Here is a picture of graphene’s lattice.\n\n\n[Image Source](https://en.wikipedia.org/wiki/Graphene#/media/File:Graphen.jpg)\n\nGraphene has a simple 2-dimensional hexagonal lattice structure. Usually, lattice structures are pretty difficult to understand because most are 3-dimensional, but graphene’s is 2-dimensional. Graphene’s 2-dimensional structure is one of the two reasons why graphene is so strong. All the bonds in graphene are on a singular plane. This means that if you were to somehow pull on a graphene nanoribbon, all (or most) the bonds would be working against you[[3]](https://www.chemguide.co.uk/atoms/structures/giantcov.html). For reference, steel is typically a body centered lattice and diamonds have a special kind of lattice structure called diamond cubic. Here are some pictures. \nhttps://upload.wikimedia.org/wikipedia/commons/2/22/Diamond_Cubic-F_lattice_animation.gif\n[Diamond Cubic](https://en.wikipedia.org/wiki/Diamond_cubic#/media/File:Diamond_Cubic-F_lattice_animation.gif)\n\n\n[Body centered](https://en.wikipedia.org/wiki/Cubic_crystal_system#/media/File:CsCl_crystal.png)\n\nSteel has a greater packing efficiency than graphene (as seen above). An important thing to note is compactness doesn’t necessarily mean strength. However, compactness is directly correlated with density. This is why the open lattice of graphene is one-sixteenth the density of steel.\n\n###### **Bonds**\n\nIn case you haven’t realized it yet, graphene is completely made up of carbon. These carbon atoms are held together in their lattice by powerful covalent bonds, the same bonds used in diamonds. Because of these powerful bonds, graphene has a high melting point[[3]](https://www.chemguide.co.uk/atoms/structures/giantcov.html). A key difference between the carbon atoms of diamond and the carbon atoms of graphene is their hybridization. Graphene has an sp^2 hybridization while diamond has an sp^3 hybridization. For our purposes, hybridization determines how many bonds carbon will have. Sp^2 means carbon will bond with 3 atoms and sp^3 means carbon will bond with four [[4]](http://chemed.chem.purdue.edu/genchem/topicreview/bp/ch10/carbon.php). Carbon typically likes to have four bonds because it has four valence electrons. Graphene’s carbon atoms only use three out of their four valence electrons on bonds. What, you may be wondering, is this one, lone electron doing? Well, this electron is a free-floating electron and it grants graphene the ability to conduct electricity. This is a very important property. Sometimes, the free-floating electrons will bond with another, making the bonds within graphene even stronger. [[3]](https://www.chemguide.co.uk/atoms/structures/giantcov.html)(Because even electrons want friends too…)\nhttps://upload.wikimedia.org/wikipedia/commons/thumb/1/17/Covalent.svg/334px-Covalent.svg.png\n[Covalent Bonds in Methane](https://en.wikipedia.org/wiki/Covalent_bond#/media/File:Covalent.svg)\n\nWell, if graphene is so strong, why does graphite seem so weak? After all, graphite is just stacked graphene. Well, graphene doesn’t bond well when stacked. Instead of strong covalent bonds, graphene uses a weak and pitiful intermolecular force known as London dispersion forces [[5]](https://en.wikipedia.org/wiki/Graphite). Just about every molecule experiences these forces, and they are the reason why pencils can write. A good analogy is think of graphite as a stack of cards. The individual card is strong, but this does not translate to a durable stack of cards. Instead, they will slide off one another with just a gentle push.\n\n[Image Source](https://www.pexels.com/photo/playing-game-card-58562/)\n\n###### **Is graphene useful?**\n\nHopefully by now, you have a good idea of why graphene can be so strong but also so light and flexible. But, like my high school English teacher would say about my papers, “so what?” (I got a C in English that year). Is graphene useful? The answer is obviously yes. Graphene has many qualities which makes it useful in a broad range of subjects. Remember when I told you it was a good conductor. Graphene has a strong future in electronics. Studies show that it could be used for one of the most energy efficient transistors ever [[6]](http://www.thegraphenecouncil.org/?page=ElectronicsJAN15). Others foresee graphene being used in flexible/foldable touchscreens [[2]](http://www.graphene.manchester.ac.uk/explore/the-applications/electronics/). It doesn’t stop at electronics. Because of graphene’s high melting point, there is talk of using graphene in the automotive industry which could save as much as 30% to 50% in automotive structural weight while also adding more safety to the operator.[[7]](http://articles.sae.org/13441/). In biomedical engineering, there is talk of using graphene for tissue regeneration[[8]](http://pubs.rsc.org/en/content/articlelanding/2013/tb/c3tb20405g#!divAbstract). Honestly, the uses for graphene are limited only by our imagination. \n\nAre we already using it? What are we using graphene for right now? Well, graphene is being used in censors. Think about it. Every atom of graphene is exposed to its environment [[3]](htp://www.graphene.manchester.ac.uk/explore/the-applications/sensors/0). When applied, graphene can make for incredibly accurate censors that can distinguish materials down to the molecule. \nIf you want to get a glimpse of the future, googling “potential uses for graphene,” is probably a good way to do it. Graphene is still a relatively new discovery, but I would classify it as a major discovery. I am excited to see what becomes of graphene and I hope you are too.\n\n\n\n___________________________________________________________________________________________________\n\n*(Hey! Thank you for reading! I had a lot of fun researching and writing this post. If you have any feedback for me, you can comment below. That is always helpful and appreciated. My next post will be sometime this weekend. Thanks again for reading and I hope to see you again soon!\n-ulearn)*\n\n___________________________________________________________________________________________________\nSources\nhttp://www.mypearsonstore.com/bookstore/chemistry-structure-and-properties-0134293932\nhttp://www.graphene.manchester.ac.uk/explore/the-applications/electronics/\nhttps://www.chemguide.co.uk/atoms/structures/giantcov.html\nhttp://chemed.chem.purdue.edu/genchem/topicreview/bp/ch10/carbon.php\nhttps://en.wikipedia.org/wiki/Graphite\nhttp://www.thegraphenecouncil.org/?page=ElectronicsJAN15\nhttp://articles.sae.org/13441/\nhttp://pubs.rsc.org/en/content/articlelanding/2013/tb/c3tb20405g#!divAbstract",
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}ulearnupvoted (100.00%) @muphy / let-quarks-be-free-particle-physics-series-episode-3c2018/02/02 00:07:09
ulearnupvoted (100.00%) @muphy / let-quarks-be-free-particle-physics-series-episode-3c
2018/02/02 00:07:09
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2018/02/01 00:36:39
| author | matheusggr |
| body | They must! The bibliography is very important. And with good references! But we still need to produce a lot and get to know a lot to evolve in these areas. And that's just a hit and miss. They should and are not always, well-supervised so as not to be unethical and to endanger human lives. |
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2018/01/31 12:29:39
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2018/01/30 20:48:45
| author | ulearn |
| body | Carbon plays a fundamental role in all life and everybody uses it everyday. Carbon is a tramp! |
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}ulearnupvoted (100.00%) @pangoli / and-that-s-why-carbon-is-a-tramp-wait-there-s-more2018/01/30 20:47:42
ulearnupvoted (100.00%) @pangoli / and-that-s-why-carbon-is-a-tramp-wait-there-s-more
2018/01/30 20:47:42
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2018/01/30 20:25:27
| author | ulearn |
| body | I completely agree. Many news networks make their money through advertisements. Scary headlines are just better at bringing in a larger audience. Many studies, not just one, are needed to determine the dangers involved in anything. I think any article making such a large claim should cite multiple studies to back up their point. |
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2018/01/30 20:18:15
| author | ulearn |
| body | Pretty much anything in moderation is fine. Good article! |
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2018/01/30 20:18:03
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}ulearnupvoted (100.00%) @gavvet / the-taung-child-the-australopithecenes-rocky-start2018/01/30 20:10:45
ulearnupvoted (100.00%) @gavvet / the-taung-child-the-australopithecenes-rocky-start
2018/01/30 20:10:45
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2018/01/29 23:31:36
| author | ulearn |
| body | Now I feel like eating a carrot. Good article! |
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}ulearnupvoted (100.00%) @sustainablyyours / does-eating-carrots-really-help-your-eyes2018/01/29 23:29:15
ulearnupvoted (100.00%) @sustainablyyours / does-eating-carrots-really-help-your-eyes
2018/01/29 23:29:15
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}ulearnfollowed @thehermitmonk2018/01/29 23:17:12
ulearnfollowed @thehermitmonk
2018/01/29 23:17:12
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2018/01/29 23:10:30
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2018/01/29 23:07:12
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}ulearnupvoted (100.00%) @ulearn / hello-an-introduction-to-ulearn2018/01/29 23:03:30
ulearnupvoted (100.00%) @ulearn / hello-an-introduction-to-ulearn
2018/01/29 23:03:30
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}swaggerupvoted (10.00%) @ulearn / hello-an-introduction-to-ulearn2018/01/29 22:57:12
swaggerupvoted (10.00%) @ulearn / hello-an-introduction-to-ulearn
2018/01/29 22:57:12
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}ulearnpublished a new post: hello-an-introduction-to-ulearn2018/01/29 22:53:00
ulearnpublished a new post: hello-an-introduction-to-ulearn
2018/01/29 22:53:00
| author | ulearn |
| body | @@ -1180,8 +1180,94 @@ nebula. + Read more about it here:%0Ahttps://www.jpl.nasa.gov/spaceimages/details.php?id=pia14417 |
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}bottymcbotfaceupvoted (1.00%) @ulearn / hello-an-introduction-to-ulearn2018/01/29 22:52:51
bottymcbotfaceupvoted (1.00%) @ulearn / hello-an-introduction-to-ulearn
2018/01/29 22:52:51
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ulearnpublished a new post: hello-an-introduction-to-ulearn
2018/01/29 22:51:54
| author | ulearn |
| body | @@ -1071,8 +1071,117 @@ Thanks. +%0A%0Ahttps://photojournal.jpl.nasa.gov/jpeg/PIA14417.jpg%0A%0AP.S. I really like space. This is the Dumbbell nebula. |
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ulearnpublished a new post: hello-an-introduction-to-ulearn
2018/01/29 22:33:39
| author | ulearn |
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ulearnupdated their account properties
2018/01/29 18:23:48
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ulearnupdated their account properties
2018/01/29 18:22:54
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2018/01/29 17:59:12
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ulearnfollowed @steemstem
2018/01/29 17:58:57
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ulearnupdated their account properties
2018/01/29 17:54:42
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