![[;\Delta t'= \Delta t \cdot \gamma;]](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_ua3Te8DVR5z6SQHE_DYMxV-byPqjaqoz6E-C5GuJZUjrWt_ETZLyncPiyoyislqolGslgWqNvbKC9vR_z2wUz6LNoybKd1ZN0I-ikfKMc2aCe4dX0-Y3ja4Cr6oR6gMMr1WlZhEaUhWbmedHI=s0-d "\Delta t'= \Delta t \cdot \gamma")
e que ![[;\Delta s = c\cdot \Delta t;]](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_vKjs3rztOXk70j06XpU9ewZmIbyjl6E3FVQAnwqjVhI1uaiuy96bjSBzuEVim3O176sRmfWgOcRu0HOUnSDBo1gSMTBuRYV8SQI-SDBxUOmEaHXEhIdepZEGhYj9IHqsESdg=s0-d "\Delta s = c\cdot \Delta t")
, ou seja, ![[;\Delta s=c\cdot \Delta t' \cdot \frac{1}{\gamma};]](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_s96m4bQm3kNrDKp2Im-E9yJCD9AwOr7m-E__sDn9jrWxZOlik7r3MjGlY7ufd2dujT3PN-FAoVsqmv69vNs9UTi1YCiK0_4MmAQLdqcB_fJ5pH1S-UO-KG1x-I5xMk2qEBjoRngfv2gXvK-5SYwKfOZnqqznAOp1Z4F1viSt2PbEK4h81vYTQ=s0-d "\Delta s=c\cdot \Delta t' \cdot \frac{1}{\gamma}")
![[;\Rightarrow;]](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_uCspp54vWqwHC7myqapU6pVDHEhhryvCMezA4iap_7jHLkcioH_lmDVPPDFiVHa3FNWoAGEAwyNeksEme2o7LjJb3PtA=s0-d "\Rightarrow")
![[;\Delta s'\cdot \gamma = \Delta s;]](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_t22_zTJ9fNExL-9DYdM77Lq3CZr3A5yrVzJK12pvUx5hGaIvz0btvTRzDzIed1vVwYunkGhalXeLnHG20OAewFjgJa8n60XWZpC76yi7ouyALeR4YdRH4gspMGvCu6OYSHvp6LnKq_sXoUFP8=s0-d "\Delta s'\cdot \gamma = \Delta s")
. Observação: Note que
![[;(1);]](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_vM9Km7ohIyY-8yFHIxYmCmcZB5eHAWfZG54BULwSiSmKd8FXmMpB1xf3Qr5T2Ojg8_0yXvVntQgEX4cA19vg=s0-d "(1)")
![[;\Delta t' = \Delta t \cdot \frac{1}{\sqrt{1-\frac{v^2}{c^2}};]](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_sfJpsTk_nwo_thaZvslyW8vS-bavoy64y7mFEn-z26nj8OkEs4vxru087t-2DWzEgZlPwwAowJdB8P6jidXDiSF5RqHIiITp6fdLRb_tJgnrY5YddUHwLzIBRE1kxuNA8DV_bV9UTQBAHB0QhCJz2RRoUxs-y54K37kCo4WOHCqH3HIQZOlD-VtDhMnSeOZ9wpxA0rYwVXCwqhUipI85AsI9w1HQM=s0-d "\Delta t' = \Delta t \cdot \frac{1}{\sqrt{1-\frac{v^2}{c^2}}")
e ![[;(2);]](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_uYNEUdhfUUy8OibKUJS4Dv04YFpmy1fBy9ajfb5YsAzO5dO_lKeLC3ZKYMqbNt4E2npOe4qMys5mQIB-is9w=s0-d "(2)")
![[;\Delta s' =\Delta s\cdot \sqrt{1-\frac{v^2}{c^2}};]](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_usHKfXvxQB-hMb8sENJYlWWuV3ZsfW4w989hVj4X55Y3r6Jib7hCOLZ7f0zp9dAXj8liAf14JKSdYMFY5VAo0FSr2521pM7tOrzflrhvM9tuywXWF31B4fG9rJM42Zf9LE3FBtdNg4KOBomJa4yYQJggDxO3jPLpEtqfOq1TXtOJXB7DkfbB1a9f6_KsA=s0-d "\Delta s' =\Delta s\cdot \sqrt{1-\frac{v^2}{c^2}}")
Assim, quando a velocidade
![[;v;]](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_vWg8YaBh6PPUE4tuuh_XDxap9g-COirKOixEDoVgpSUUXxspAlhWKcxij9N4_q9oVRfWaQbs8yigA=s0-d "v")
tende a ![[;0;]](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_t_azAJDP4yaWdl_3euth9_p-WB8fRDvpfFGDyoM5zTQtsz1JjvkYqKs2r7XB5u67uy1ns_eOJ66Fk=s0-d "0")
temos que, tanto o tempo relativistico quanto o espaço relativistico se aproximam do tempo e espaço clássicos. Porém, como nem tudo são flores, quando a velocidade tende a velocidade da luz ![[;c;]](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_vPBMoyETAi_A_ZXoVTM_nLh66EFubUJk_cBcf0_dinDktDitaz3XHmbCGdJXJQnQv2YqZ3fh021Kk=s0-d "c")
temos que o tempo relativistivo tente à ![[;\infty;]](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_vxR7xuFl9yiMyxyaFy8j8aEkI1uOYGYGhL3o-OtqV4bqR-d_d3K0S5l-Q7PrWltTecs_JCkxRywpZcoTUV-bd3=s0-d "\infty")
e o espaço relativístico tende à . (Loucura não?)
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