Are pending runs now not visible on the leaderboard for others?
I'm playing Polytrack on Google Chrome, and the engine seems to have deterministic issues with things like respawns. Sometimes, when I respawn, the physics will behave differently than other times. An example is my run on a track that I am working on:
PolyTrack14pdjamtmjirkAerE2AG8lsvvvzdsIBYWtZzwTfROzsqu7TXnZmviyJWgEhCFKifRgTMKNt34bDK6Xqk3Yucacx4pQrnWHGuSn3tcM05itMp4lXKj3gAK8wL2MCL96eFmdrclxX2wz3yxyFWYlEyrYzFEeuhVKRh3ot2QiPFdyOzPffEjdHpH1GtvTMk8nPjIJhevKdf2tCQJQz2fJcACvBv4CPlTyB2Q4JEHAphAUrkQ7VS4LIucr2F77bgPfHkayr7WMAiDvAvMAfA1Fqead4XKjkGOaryNAM5cH5AwQniPnnnubUTBcrjMQfFmod7as3Ct7aOaEQjugmDor2UJr9OzaQjurF2qv3Roi3eORkA0BmsK1yd4eiZq5NEiBTfMBYq5dUt5q9GirYSsZHCy2BTHvYhZEP3Dr0fyhPmdVjeFt56XvXmhhNw332gYvJek2cH2eQrVYkFfLViZ6jmU4OOD0f0oAxr6Xc6QXde8XlXlovsHWfFTc0ecA0jWuHvBeekiBwm4DWaGdihdb3DoQHtPG6MKttetb9eAZZEXwWPs9PQzR6T018p4ADqx9i0M8EP3KXCtucsxeclWcaWe8JkVte9K9fI27XquXvxCGEM0ax4n1o7lJ89gZ8INfe0Sf8cZ3iysrhChghxtYet0PhkEbRbbSrX3Um3qsVvPJciBvEMkRmXZqeWIHP0QlcfgXbla9gzxgjK3KFcb4mZ0xlKUX1KEZl705pYp4oYy51rI3xgchcUqEPLSJ02DvMCN2Yf1NQfc2Wsn86OXilhPUKclpnfZ1kGMvVoH15FxiwrsXFvyvOLd3nWamf8d73BVi7FJSGhkXez9VXWVCziEmHc2xptFe31eluyjGB3cI0aRX45vauXL8rLweqUEzZdKUsBNsX3t4q1QyGbs0KXRYmCrkJe09Q4J9FufMWfVX2DIeK9jOVyn9fo5kmDbXvanuUkcyObiEb97oFqi0uYfeSwj953tQPLON3ULDe9cPqeeuALsFbQRngVaXsATas8nTDSwWrYnrkJMa9qY2lRnmwMwGoSwHtzbUpTg63ODAZRxzW5vBDnYfrvqSr5BCDOeasOe7dgm01XJJZHxeQHUbtXheyg6T3j943alAcZEit0iBH6obfeAAXfPnN4zbPIBKyIIx2PnOG8hBADPQawxJ6quU2PqvbIt0TPFc4PVP4RpZXLBCycc9ByT3hKLwven7T0JeekGtKoiNYJaSeh6XHpuaH7cU39IE3PrHYP6Eb39rk5zQjkUrXTSirRnSmtG5iMvH84IPlcZmOqHAirjZ3EAcEk7nVDceomIXwojyAfc036ClVnEW46m56EOy4p45rq3VSMMY75OR2ncJ5JyJx1M7xp2s6ET75Sieu90xbQAoR0Fo60mzt10uDq0hhzbxcCTqbztYcAfNAtGmb6M0T3ZUCSj7i52YA0JNXJRzEVSkEppqqppemawkzVBQiH4tgbHF9jjgrkyt5s0ebwwDAJXHO8JIgf18IT1jnFbAW2VTuNwpO5BxGs9feQ6tTpZV6Ci0df1DMI1jbOZe91XV4ron9XtzOVyLPGzdEQfKlMhp6xobhgkFHvcd9j9iUw1OInnGx6rjP6bbRgAx7qZF5s9U7uBkKuYl2X1jUdfDSTxeHgg2XWFDxdaha5tHfees89aCPNYl4fApSZGtxe4KaNsGUzu7kIYEp86QIRDdbe70ezu0pjSAX9S937glkY5rZdgObx7vhkF07MJEnT2oOL1PuH0fpDURLrnL8pxgXQEylCFtBajq9DbjvEAOfotOKJKGM34vjNOckfrHtUPjf6fs7DD6nk8TrKteT1MeAf3eaAgJ9qGCSsPEPmej9Qw0xHLiBoi7PzxfjHhgHO1mGmsEDfa39kEODxesn1icpBXlQuAelPpfljAuf9p45wxLCfsfqrcvGfjQieAftTizXE5MX7apeUF6Bqv7lx8HGG7xXH6KqfLJoxRqbaHpNmZejEQe3Sg9wmNaB43rQb7aa3rW1sfo1Bi01KGcSw0Zlfe04jDwv0txdDe8Q6h3enKfXaBkeLL3XyBaDe2foTpFkMfT3tr5FelQIeqfHgEQfD7PjiaaW3PusTE7URCtASrzcvGMeOoVsb12gR6bngfyc5LXfpXphZGRRvkT8q8Yy9wsbvFonihr6eRtKSr0XNd5hX5tO3KR647CER7LPee8t3e6QNwiLYxuKWkTYhBocgr83dxiVDzslLAOKFssb6KefWXwyuwi4FxRimUfm6pkEte6jblc6e21RQTju01iFC8UCEJEKrezGaj8utUsM1oTunMXRRah2Z12CUnQBNv0OAV9Ur85k5lZ96YpjYU5VmgOe6Z2EPyjJEquA4mvqvz6xbpuDcpQcL6LUeoWR8Lc0XANf03WaP5B0MGFkFz9Nhr3mCyjZ97k1xKKxLKkmndBW9tGzvQgONbdva1ke4oredB6eQqGbutvWP3X1gg3JXvv50WxTsSZzk1GNdg7eY7hkwhDfUveH4IGRcc147Aw93CM1tGFp8c0SuIoL27LbPUkkEQzadVKLNPeuq03bDqlCGLxvsmbItzTzel0CgS19T4p4dbq7deYehMTLnmRVlgdNHU75tzPXZTseCuW33xoWJBKTCfu5eDf0FOALOXAHBb0e4JF1vw706UUfdDGfphwfqBtf0wlfqBrvboivl1DvSZntglf3XR9nrALgRkm7IiSR6TfqVsFXGRTWiXBCasd1aOhjSBDXVnk7Ic5Bjl2S9u1tSl9dQnIB0dxQWXsHxFhcCjTP6Zf25jJi3GmCpEm8hZj28efOsud9WmONjFni8s4s6cdFqtIt3e4BBKoBPB9ZtXRq7amwG5TdNI1pLTObOXeCYhAj6SQTn0sITfG5NS3Owo9DOVzPsur5jF21zcfEsayx7Fn6CCbmwidxG1wGalQL8Z79VDjq2VngNojRtDzvRGYSrwUVhxj3hiZxKjvcUEYBoHMEc0wwrWyKrY2qWvNgDuHgsrrR6xDmJ28hNfXBCttsoeYCLSTVgjBqtIMfDs5vGaNsYJkeewMPPFetScVOKoADicIgEFyjevZtkfl3cl2Fk9IUn7eKUYjMPtpfBfCCTwehk043uycw3G05v9HCl3t9o9LPNi9MPQeP6kwgJfGbZtF3LMotyfjBH98jSz9ecuq14EbuG7G4C12erfJC2vCjUj9d8rAw9WhvxFBGGf7esajxfGH66ltC3Yvffs70bPOFf1slhSjIgKX8JXY1hj6oSgDZd7XmcPtrmY6q9ccHrkKhCsfye1eea4IfqtMvtiofy2KGFTimJsvesI3j7Ff0wVR16LBW1tORJ8dPmEqZiCYewq6Kfx7VXmavcRBIlbXRZogsRSdZTnsvGzQpn4LeZBfRScNMkUwdpOz2ZULgV7VBkrrqxhVZ74uwBLyc8ZR8qPLsLpXMMhqDJ8ijPBHCHBeXvZEi2KG2PN3YcaMXbIGuarg71z5A0OU7UHOKFuydNY3NlXRf2y7FxjnF6ECo4DvfW4KtbVxlazqba2CtUGzSBhur3QJ5lKSeJveJl4yEXRyDO9Pb60OKlW7aKWrRbSYoNFWtmlm1mF9T9T4rrESo0QXhlsi2hF9VicnpRHGhL0u74c2Bj1H8VU6ByPZDr10MmRLEipUuihtb1jca4Rop9ynpdZzee7SI9aZiZSYtjonknaNmDhkmMCjvMJUhbttBzZPzLgpTwRlNwbXsWnpeOZ9pa7KQWNgHtYDW25F147CAMEARNORksZ1Rpi8JMJVG3EsyjiTFhmPphWsEFxxK8uWO9Xs4GbFs4sCAXfM44pXwNBrqW03b43Id8Qh4Ea9MQOcZhqblKf5Q9jooqaX5ZVJhsEYXz0hSFqHuwJGAyfJh1CspGU0rmr3d9EEYAsfJZjKDNKHv95TctFeg6qSgTKCBzQdClfDOLHpsd1aZH0YbSzczfeVzOmeLpJOZK8Et09BToUJ0M8VY4qHFAOIQmgmKoAWe6rxOUosJERJSFtDboc96o86w7wTSqgi4DeWt7KsdaaU00muTxgLtKeeSuCDeeJFceE7hI5byMPC297VUeURbM4DIBqk3n8qNo7PLYxJtFAMee0hPoROxvKtP44epyyE8uW8aNR6aGlWPuJErPKIed9a0DpHXop3FbmyT40AB8CUUzraBs8mJIFl6dP0Gn0eZd4N4YXOiD4wlsqxtqBl6WNerydPyPHvgEVzxHA19lEYLyfcerFpWFrrVnzU8fIUgeN09UFJ5IeyTCDiaBHcSleaBmpYpo5EyRhUR0eulKqg01GaTCjYNVfc41taZq4NSBWqS8EWUJqcfU6AbqxEOFtieIrvAPL3dYSj0LXP1rIPbIr9351aeR0tO83k6f0twDFijdod8BhJ7n4DuFDXFIMfVUS56z2cRfSmIQb1hycnHt4HGh7wx83x67B0DgI6pd8BJTf6kKXtkhqyHdqfY2kzJrsZGtnXVBrxbX8Pe2rVkekneEMwkDv0yWtxMoDIiNIeCfbHB3eEJl1lKP5dRKrMHKngyp29sWB6Xl81P5q7ma9mvzhFzKhMfZl8iHBSoL4wjWCRZKiABEYTvoE9ykd1oTDzSonJMqjaGRUU7EYC6BnzWozvQeV3oiZKPruAWbr6OeYdgLu3jxjrBcCsXtOueeb75l1gpWh2J0eW1sAfEMeOw33fQQytTVZT0NATQc6Ycij1PlX7cUYPf1Li9aJM4T4OJNVs0BSoZeDU2ZtCkGNXlX3wihcRg7pU6yjIEWHQf0qqTnr4M9esjCsJNxBEt3Ob8c8u5wvmRVIseRqmW2R9NWtE5dcGCGEfBUMD87OqPfgLuU2ayCzRvP1Hxx8EDJuS7Rx1TBQ2dTUecTfChAJZ24RnV4fq8Dp5qJxzZxN32wJzFeS7LLBT8EXr2qvxZVpP8K38qTI4SUXbFKggghqjqWXIxiHHQf7uwWdeGikEs5AOwp6G5m4WHjJzqq7siSpVDiWmetRyzZGZb8Gex9xkIXdsi2t80M1ccS7hq2fQdxBCPcR0fMULUiR5jjYvkRYBPN0Y969d9k6jVyXy1CkzYMrjcyH5xEfVsUO3HpQkxNOz66vTELY0eVHBK9mHKNe1a4Naey6pWgb99QxnsXqlc8HFxkuxgWcrAiHY5w3E75WYx3ikVwEyUanWLQ0aHeifAfzj8ihpXOeswx6CHbPk1cFRmh0RqqZimpsNBHe96KaNYzgRCLXMZbu2KVZUxjYdFz2drdp2BdqQesNYefcceYg4WtjadIhfUx7ertvFS8AoFGokKmNepztntzotbqallW4PZ8feuh5si9Hj6pS94eLVIHGxc03db5hBFj3RPq896NEJ7zxugcZVt6XKBx7qskLYvU515JYmiHareQqrDP4aFerEOkLIDfcrapXqfujtflta6L97sttSEKGVwLoNaqKLUutsFqT8CzPxiT488gvecjNIVQ4593lZsDZHjlPPHfiNEpI5y4LR5QiBYRKJetjGo84IWAJJYV8LU77IovSm9cN0edVe5RWUaXCbfAfjN2XeCFnE2EGPeMeAuAijxUgLI7pipAm3ehzLDb17Hok0eBM6pRhOpuWBKoePBgrruY5JFxJzdLXTGFjRm3jn91r980OfaasRCCzsDUSHsSLvNZeswHctfRAnX1V8mtxlxahx6CBEhU7DJFNGuzzcnrtKPF4QJnRjX1e7jjcUgBWSTfAkIeqrXEKfDokQ8nU2YB6LbChu3Ojk0KFbEofUTIYQKTT4azIQg727Q8BTsYvbmtosGuM6Ofu7hx9QpzdpTUctEj7o0QKpNZShFSuYKqHljVp7ogI82BIQWXSikDDSGHfAlmq3cTp8TpQvzmDjbMNf4WOoJqWc5Qp6eusrqcIwyUWX1CBEwVWHiRmF5SKadencf2NfqQLunfgMzMJ3Tls1jyKKOcer20MEfmGaNzb94PQyWd1RfoKGzTeXqeUrwT7CYJgDt38zavj94fDK9X0Oe48rf3TtHdbyjmYNmo9aMLEL9O8jWfiGqi0uiX4fsuKf5u5y4QcgOmfiDFxLtarenkxev8K8XE2oZdH17ckoYYwJxxjykA8nHvvgatb9JXRQ3MiIa70RugfBfLePA41QBhfHH8rIs2DEoOHCaXIQ6JTYdmT5ILmQfycLwffXg4fBPmMqFRdKiaSd0Ig9J3F0NyjWEYv9d2RflItgWcA3Gtrfri48raUxO4KfU194zjS8n1OEouRA3PInJIofJ8iWNHOwKwBS0woEefc1G1jfVCuIC4byqtiXZefeJbG7StlT8oMmsUhiLy6QHjNjfS18uEqfjcsUsDY04edaDaIbAemV9cTZIa4ecmBIC1PDlDMSeoOy6RpFBdqNJjsiejS7Jf57YF6vaZeYVELaHDc5xb9603J5Qt3EOeGi4epCE5l8OSL25ogNMogc0IDxLBXdqQeUANv6mtteTtJwfsQoappIFB8egxqSWgpOUc2xx07ZAyBqdCKcVQ8L6btt2dScWmIfLfps7e5lkg7cVoF2F1udAbfeae6eTd35DvheUhI2rrBrdVRFpLtvuyb4kQdn9pAKQs558dTF1PRhNneBMFcHt1dfynK4cGQ8cSQnwfBTnlxNrAVhruwezlwKRaGfH50IydGo6yr9MKDeEReI0MMmsl7n4dXdUaFb88Q5TBuc3Zqcf2Ls1cceV5e8WN27rimaaNqUgYDLvWrRtfAlzB7e48YQKXdJuMis8tLD4m6dRsHIehdjqpUVmsWgsu7dmohnxHSbiNYPjS9H4RcLQlfDQKLaCvJa44emeCUWcXZlVWsJcSdFIPyXDmqBkDMwAvsYkXVL1nYc1fgU1Vh5g5UvXf4KvEQZyGxFwTyM5hAkc4QkFVtsGGwPCQs2b7JEo3nkvYVLYCBIfLkUFMaAdMvepoKbYAUSg7XlfeCD4DoFL9IrdGecsQBJ9E2zuWbDfYsVGinP3zM83h3K8UVULjgvfuVteDlpK8bZw2HKKsT33R5U1EBZFKVGX0Rx3B96hZekubm2rJ7cgC0aXJtqqQd2GuzzxATtraxciSdtQC4uEzXLa8E97mVvOzjHATF8Zxk3MEBXl4YzdoQUWVp8R6bpedyH2U0euPQFhSnO6hjSJIXz9q5WDmMx78eCJYOMq3V0Ea8IkaDI7xQGQliW4CYpc5ueUS0jeVe3WFH0Tw9yHeI2vfDQnfHoobpOWp8fkg37cgfnBKC0Xq7irbrmYijYT1WfRTEopRE1K51MiyOIqZ0jSJIafLDzfU5NXeR7bYGVtGZbIkCk55ecwFPNFhx94X2Jedg9OJAKZfCbiP3lLZIO35S5ddccBSwxlOMFgkAipczeO5HGfHHZqOigIRzGwk7nXZ1m0LR6noArY4BE85fOQyfhfmVWnPZkTEgAxwfdf0e7czjV8VbTlQeslC5SpqL0rLSrLGqLuUTbKcIHpAfz7ASLWtv6TZsC8YQ8HiJJsLsXdYo0rWk3XE27E3LR0rIOcHGYDHB6CbXfXeiqoPfrCPIoS43avRi2eIVDk2DQK7U05UAyIayi7k57o1XI9dyz4XwroZjO2nSX9V9y8Ujy29oik67czTdjieq7xeIeEHzfqARVPwPGa6sN0hGL0u54CXZO4eifL2Xafscevq749EegEIdCFgIim4gmw6Oxz7E57P2UsB3JfOerYdke4vil8pshZjCoscHL5Px2lMmt5zxR5vScYUMItmxDlMoFTJoORLwqfu8lfUAKeRdnh1tgoBcGEpzTXsVdendnX62YjB1kHy955V2GxARyj4WdYTBpejuNlf3aAlfzHSuwixNj7rqF8flTfZMXQhFCRBol0YfVJRZSrvUfSVYYbu6yRGKyCwTdKFbS37AhFiWZ8TKRrL1WGRooKp9TjVeXfS3R1qoyylReIfhXo5VBhejUfLlVp3CYwcPDped8svC3OEwdo2NxGIf3VprVWbUhXfC3QQ2aHKQ0EZkXMPRr3paXfc1yfSzigxOem7ho3GhLXuOB4FUvlOvzLyp7r3kTdgvdjyvfe5wNJPbLzefm46PE1W5lDaNrv27AFxoGFDAPVa90ooKlg5cntvG5BVORyaffUT5TFdJFfKTTVLEnOfzP5r0UksYVIYV49RfpY1iWkcHviHtChcwGeGTdD3rZAfu8UMTxvAZCXZLKrX5s0uro2aVnz4RhCLT9azpf75rokffkIfBrGhFynvEwhQp2VzzDHlzfVsVKhskGs1UNVfOe1EWOfoR9l3fET33v7ulD8jAkHgv1vf6Oe3L3bpmdrJz3wHfXlNGzDwAkmNnZ659rfHIN1E62vLmVCDebEr0vQ2e1AN99LGe1BO1HjtKlYnoEuoc9ep0yZfBN7PwLOe1915ofzXY3P0QfbAwIrqOKHvffB7JSNUfYRV1wXBHJbqyoRN6L8RONehfBQ8v65tlCdLAiXXtQfqffb8zGzxP44fbbsErfpMtDIhR57h8Ja0twYy0a9neHFqPlABb8xfVB2Rs5iY0JATmfiwtWK4fkxV4qDpi3vKO7fznI3Hw2fy94vrsfnFKq1ffViCfNYPjH3fABN3fZaLYXhKRY3JiWLNczBK1mVzc15KQJuTtEor7kVoRqIdlt1wus2GZZkfne3aPZsACAroa8LxELdK8dJWPCaInregrbM0jqHP0tv5tIAEwJAAhciA2KWAVYjAoeu8ECXwXFNk6EQ8WLgcPEbfGqNk70RBqtT1wnduDvFVutUZsnfp6UrBXfTPsJP9isERiYW4FOQICYqjAayc7Mewx0xe9KcmIWwrKYGBOzUNMiAndbqaj7zviHIWl9CyNOdKGI1FkuAIVoJbnHOcJw2zZeiBGiCeFkX9l0oHeWwA4omt3ItdEHzVhnOi7K9pwhKSu76tNIMrNQiBoPTYgKHl2R0L4Jn1e0WcD6e1f8xrHoUz534LkeYPlVmYpGnFsWpTDuj0MMxElf0w1KeFREG3yjeU47rWhLfLdWNQEQxyTzuTxvJTwBQKU3dZO4d0FfVjDReUMZgK78g37DjbioUAl5hCEeZ1pTTFByM60T7I8zkuiWBwUFqpKbeAZW4e4APiT0fCVoT3hVShPwZg7D8QOC9aGiiFBQoDDd3eYGYxeYfXfwrih4V1J7gM3FPJE3OZ1Jf6dxKdO3ThVhCXCOHlCwOJWLlj6n3DAr7Oi3cfNnIWqnHBf6Hv1s0nih9c2S9Tlca7aRZkEeaVbFbR412vftmWN0GEMHWnHf8yEf53iCOtGlDP1egr1vAhE5Mo4wiNV6sxCrMCaJ24Afl3645NqufllTDzW7YuHm5Ubu3RuD6wr7lfjXeRyNxyp6dSYxhxdbbBNCAXl07Pw6UfSmLSFQY9Yr2h3GmHzZiHu7e40fnDHElF6D0aRJbzqibcAUyENx9calc7QzWNsYhC1ETiCqzFmv1OxcNCFkIEhPMBfiPQHufTDmB1t0p3Acattb246Pf5tFQC8Qf6rrmeQX0l6YYCxepEd3llsDX6e6aqZSYltoM6W3Hme6QsyB4KD04iZWVKUV4iehRJue1TucFVeBRQrAuZ25Jn9oPzT20pWheoofy2f0p1ZvbcLcqeFGTNuRB4XqTuh46UpfMgmZCbsf6F6wC1UYAITiRsHtIjjwvNByOiQ72ZgeI0rslprtfqHZWRwDRYGVbCcYtdjC7yA56P2eexmsK2q2WCouPwFRYzANIs5AXaTnE25gBEerslQe9wBqdFYBVf1damq0xAeV77byG7UyK0fy7StNarR1QP2gHzfaDz2jQiS2Yi7feOKXf3cVRbwW3pY2MJYGQo3S1noftoCXCYtTxtm5FrxWUdyNwCickYxNSFAR7pCzwlXtaXQJYuvpHaAgUtK27Xi8Seos6lysqLyWLSr1YopFbEhLpQ43Bm8gk1cIve7VV15yCAfL05ci50WUGtgoJRLeFXxC4c8gBNp35FPQgey1Iapgggpo336gQe1mCzv7mbMLp4b0VLfviS8BIQ2Tw4PHV6PEy7vhxvuOeRyy3xgle5HgIiC4vXFruHqqfeTb6nS6o1iwwcUTHbNC8kWEkikkWewqjdYPo6XfZBp2OdyytgCX7PyenX3oT6oQQwe60bfPJeIWQ2WkDcenrxlYDxpRj9NlrxCyQFLgbB9f8xpA3rvj7hSjBldNKJo5rOR5KvMbvIdkxnu8dDEBluynNVfvBf4UoJx1deoSUgguWjo47mfXaYcqad7pMrsWAKS2lQlUeNZOBeF9u2MGJcpf4VPUanXqbLVUFuE6JdN8RFYsFQYae53hkHbdFM7HfWwkl4lZxTByYCEezvCkfDykAXw4GzN9KgoDkbsmJzGplkyYNR0TlXrePD0RxhW6EmJb3iQq0fvBaonQoYUgIp95jXep66wGD67pEvu8dQZ7s9HX9HuP2VcDDZXeXsLmkvReqoOX7I1713OVInxcwfL0jaDhua8jxwIwykA6ZjuAZ1iA3VCn6ZNZXvKfaV2zMgaxd5IUYHO9ygn4JqfnGmvcCmeQ8vyB48RKPTnAKN3APlOiAiI9t5NM1fGt6hVNeqCHAXagSqkmKvpwC9CacJF4w5QBXeAeZwgWnZWTVct88M7rYgDJaZjND6yVice7oEOZd37aaaue04OoP5ydhCb496XCP2OI7FxHoIxdfcmgvdqdoeyl7t4XJW1J1LP1IWuV2q9CU7peV5QytYdL8LnzFTTG6kIIGSwtp6QrL5taoEG9Ffg6C0OG8oIVFKfNeBcPryCIwO6akGUHe6RLbsNAu1Ga11acfU0T49YXw9Zi4G8epbETJLtY3EXm5fCnKrjftl7teAvRBfXXzBrYYvvcmJU0J5FTP2RhkhTIRyxsob32DhQPlyucZf7HaQpJryk06xDZdXRxCNQkePzJEKtRa1eihZ6lNjnVVIGPTJoOZwk1iKkPe6dfUhk7EKQEQ4gmsSgjifaePkXgIK80bQx3qlUw03qL6Pi8cg2qgOSM4jH6qFpHdJ2wctcCaclV2TSc7VBKvG4V5BEdVcL9VKKdUejV7X7ijGxhLGD3wmmvupWaAYeQqcJkxrvqFr4SwReqwHr0w0nEK7wVIyfwPFFC90Lf9LNmf6JU3TtSkelxKXPIDfEo4dE0B7MIXFBkkATv81Xv655tzc1WdoVwIrNOq22wbXQLkDAA8tK7nXibCQowsy21nJCHEahIRV8o0umDHFgkXICW2MFuEgW1hZQKdIMSPBb8FIuVpTHO84Nf5qNpyp7dqc9tjpI5BFNXSt4DhY4SbKnkZDuRlsZSAo7jcFSeUHJmPOgJWqqJhA5Dtvk6JXk4OSf9nf8yek2l9rvRdv7TX4nf13A0faAKNRaJ5E41VPBk0cemyGbPu2jWhb0viAw7b32UmiOQHXA4PeeKOsXYBfLEcVwVTQ07Lm3304zu9q5dZK2BnheHNvyPO7a9BNJ0D0HEtAZ06NhB4sTTGke9jj1WclewqCL9Uy8cgZkEh59OjnxCxVwuSUe5H0A6PA865lkwnKXMvR9Amv9eeMZ5T6wGZcxtS6NzY6WijFk13bXcwBb3NfgXdxrh0bLohWHgdDkfQAvz0PLFkIRplf2LLDAPKXkBlYAOmaf7N4t4kouof6JU79EiK1QDomDpiclekmCmleIWFoUGTNimDxQ4jkC8godQn9BMdIpBizDeq5BF9IBuxQeeF8I7un33TAwSaLjXaQQaUndfwuT8VjMSMA0euysHJ7fHpj2iOA
I love the beta, but I have just one suggestion that could take a while to implement, but would be a game changer.
Would it be possible to add something in the editor to make levels able to swap between the beta physics and the current physics? And if not, maybe there could be a block that changes the gravity?
No, sorry it would be too complicated.
You'll still be able to play the old version at https://www.kodub.com/apps/polytrack/0.4.2 though!
The gravity changing thing might come at some point, but not anytime soon!
Could you add a single block? It's just a 1x1 block. If you want, you can thing about 1x1 triangle but it's not necessary. This would make maps way better to create because you don't have to cover the block with multiple blocks. Adding this would revolutionise mapping. You could do the same thing with a tile.
I also found a bug
If you watch a replay and go to another tab and after the replay is over you switch back to the polytrack-tab you won't see the finishline as you would see it if you finish a track but your camera is locked on the place your replay-car was on the moment you re-entered the polytrack-tab. It's not a problem but I just wanted to say this :)
Cool track that I made
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