A lorentz invariant or field theory approach.

洛伦兹不变量和场论步骤。

This relationship can be quantified with something called the Lorentz factor, which is defined by this equation.

这种关系可以用洛伦兹来量化，这是洛伦兹定义公式。

When you have a magnetic field and a current flowing, it creates Lorentz force.

当磁场与电流同时存在时，会产生洛伦兹力。

At 86.6% of the speed of light, the Lorentz factor is 2, meaning time will pass twice as slowly aboard the spaceship.

当速度为光速 86.6％ 时，洛伦兹为 2，意味着飞船上时慢为原来时一半。

This works because of Lorentz force.

这是由于洛伦兹力作用。

Lorentz was the guy who discovered this force.

洛伦兹是发现这种力人。

You've got a Lorentz Attractor with multiple initial conditions varied very slightly, animating prettily with a glitchy trail.

你有一带有始条件Lorenz吸引， 始条件相差很小，动画效果很漂亮， 带有一点故障艺术轨迹。

Of course, Einstein didn't figure out this special principle of relativity in 1905 - it was already done by a guy named Lorentz ten years earlier.

当然，在1905年，爱斯坦并没有想出这种特殊相对性原则洛伦兹早在10年前就发现了它。

And so if it offers some sort of poetic insight to imagine that there's no time from the point of view of a photon, there's no space, it's all been Lorentz contracted infinitely far.

此，若能以某种诗意视角想象， 从光角度来看， 时不复存在，空亦然，一切都被洛伦兹收缩至无限远， 这确实提供了一种深刻理解方式。

In fact, the problem with relativity wasn't that it involved a lot of differential equations, Lorentz transformations, and other complicated mathematics (though it did-even Einstein needed help with some of it), but that it was just so thoroughly nonintuitive.

实际上，相对论问题并不在于它涉及许微分方程、洛伦兹变换和其他复杂数学（虽然它确实涉及——有方面连爱斯坦也需要别人帮忙），而是在于它不是凭直觉所能完全搞懂。

And then we can take the solutions where I'm passing in a given function, which we want to be the Lorentz system and passing in that initial state, which is the initial state we just wrote down.

然后我们可以取解， 其中我传入一给定函数，我们希望这函数是Lorenz系统， 并传入始状态，也就是我们刚刚写下始状态。