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Unconventional Explorations into Uninhabited Areas of Physics
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Talk:Proper Time Adjusted Special Relativity with Gravitation: Difference between revisions
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`x= upsilon T` | `x= upsilon T` | ||
`t' = | `t' = T sqrt (1-upsilon^2/c^2)` | ||
</td> | </td> | ||
<td> | <td> | ||
`x=G*(m_1*T)/x^2 T` | `x=G*(m_1*T)/x^2 T` | ||
`t' = T sqrt(1-(G*(m_1*T)/x^2)^2/c^2)` | `t' = T sqrt (1-(G*(m_1*T)/x^2)^2/c^2)` | ||
</td> | </td> | ||
| Line 36: | Line 36: | ||
`x=root3(G*m_1*T^2)` | `x=root3(G*m_1*T^2)` | ||
`t' = T sqrt(1-(root3(G*m_1*T^2))^2/c^2)` | `t' = T sqrt (1-(root3(G*m_1*T^2))^2/c^2)` | ||
</td></tr> | </td></tr> | ||
| Line 67: | Line 67: | ||
`x= upsilon T` | `x= upsilon T` | ||
`t' = | `t' = T sqrt (1- upsilon^2/c^2)` | ||
</td> | </td> | ||
<td> | <td> | ||
`x=G*(m_1*T)/r^2 T` | `x=G*(m_1*T)/r^2 T` | ||
`t' = T sqrt(1-(G*(m_1*T)/r^2)^2/c^2)` | `t' = T sqrt (1-(G*(m_1*T)/r^2)^2/c^2)` | ||
</td> | </td> | ||
</tr> | </tr> | ||
</table> | </table> | ||
Latest revision as of 23:24, 29 October 2021
|
`F=m_2*a` `F=G*(m_1*m_2)/x^2` |
`m_2*a=G*(m_1*m_2)/x^2` |
`a=G*m_1/x^2` |
`upsilon =a*T` `upsilon =G*m_1/x^2*T=G*(m_1*T)/x^2` |
|
`x= upsilon T` `t' = T sqrt (1-upsilon^2/c^2)` |
`x=G*(m_1*T)/x^2 T` `t' = T sqrt (1-(G*(m_1*T)/x^2)^2/c^2)` |
`x=root3(G*m_1*T^2)` `t' = T sqrt (1-(root3(G*m_1*T^2))^2/c^2)` |
|
`F=m_2*a` `F=G*(m_1*m_2)/r^2` |
`m_2*a=G*(m_1*m_2)/r^2` |
`a=G*m_1/r^2` |
|
`upsilon =a*T` `upsilon =G*m_1/r^2*T=G*(m_1*T)/r^2` |
`x= upsilon T` `t' = T sqrt (1- upsilon^2/c^2)` |
`x=G*(m_1*T)/r^2 T` `t' = T sqrt (1-(G*(m_1*T)/r^2)^2/c^2)` |