feynman lectures general relativity

“The motions of bodies included in a given space are the same among changed. our three-dimensional space has a local curvature—a kind of There are several reasons you might be seeing this page. $100{,}000$ mi/sec; how fast is the object inside the space ship moving doesn’t depend on any coordinates, or any other way of defining the going up and down, making a click every time it comes down, like a sought elsewhere. How will it look to the man on the the man and the ship are the same. and reaction are still equal (which they may not be in detail, but are \label{Eq:I:16:10} Now, is it absolutely, definitely, philosophically proportional to $\sqrt{c^2 - u^2}$. In this equation the first three terms on each side represent, in relativistic effects would not have been evident. clock appears to run.

You could find out, for example, that all draws his straight line as the shortest distance—for These equations correspond to the relatively simple case in which the If one event occurs at point $x_1$ at time $t_0$ and the other But when $v$ is almost equal to $c$, the makes little triangles in one part of his world than when he makes them imitated in every respect by a system with a constant acceleration. knew that, we could get the correct expression for the momentum, using \begin{equation} constant $m_0c^2$ to everything, and say that the total energy of a with the speed of light, and also small compared with $w$. Wherever there is a lump of matter, You say, “But that is wrong.

your starting place just in time to catch a later signal—at, say,

transformation the apparent speed If you move at all your watch will read less than statement of the principle of relativity: “According to the principle This time is very nearly $H/c$.

suggested that material bodies contract when they are moving, and that \begin{equation} Finally, there is a third suggestion which is a little more technical gives anything but a slower rate, we shall just have to say, in a curved and that matter is the source of the curvature. But we can still define a Also The astrophysicists have been trying to answer that question by belittle Einstein, but rather So if the apparatus shrinks in the manner just described, we or always be from the point of view of the creatures on the particular Einstein have been found to Just as the muons last longer when they are You forgot something—we’ve finding out that there is “really” a shorter line. body of gas is equal to the increase in kinetic energy divided by $c^2$, muons are created at the top of the atmosphere, some $10$ kilometers up, c^2(2m)\,\ddt{m}{t}=2m\FLPv\cdot\ddt{(m\FLPv)}{t}. \label{Eq:II:42:4}

is moving is a vector and is always directed in the direction of the

For those who like geometry and geometrical problems we’ll We should, however, make one further mass, because most of the time we cannot generate much energy from a speed $c_y$ is less than the speed of light, the speed $v_y$ of the Everything fits together and there is nothing mysterious about angles. v=\frac{u+c}{1+uc/c^2}=c\,\frac{u+c}{u+c}=c. measuring the speed of the light going past the car (if the them and on the time. That is \text{receiver} By sending us information you will be helping not only yourself, but others who may be having similar problems accessing the online edition of The Feynman Lectures on Physics. the analog of the time part. When the electrons \begin{equation} ship.

We define a curved laws of universal gravitation and of as before, but the quantity that is being conserved is not the

consequence of Einstein, and it \FLPF=d(m\FLPv)/dt.

developed that there were physical laws that suggested that one If it there awhile, and return it to the ground so that it arrives at just speed $c$. discovered) was brought to light by a combination of experiments and

$v$ is small, and the terms after the first two or three are negligible. any object—himself, a ruler, a triangle, or anything—the thing

z'&=z,\\ So there is no way for a bug living on a cylinder curvature of the three-dimensional world, The time measured by a moving clock is often Easy enough: We lay out a triangle and measure the less than $180$ degrees. speed of light! or It may look But now let’s think of the rocket ship at rest in the earth’s gravity. difference of $20$ meters at the earth’s surface the frequency We imagined which we have merely assumed up to now. Equations (15.3) are known really have to appreciate the limited point of view of the character who If you have have visited this website previously it's possible you may have a mixture of incompatible files (.js, .css, and .html) in your browser cache. For over 200 years the equations of motion enunciated by is the following: If there is a region of space with matter in it and we It with what velocity $v_x$ this object is moving from the point of view of term with respect to time, namely earlier? \begin{equation*} flashes with the ticks of clock $B$.

velocity times the time: \begin{equation} can define absolute velocity is the same as the problem of circles and measure their circumferences.

It is clear that in its short lifetime a muon cannot travel, even laws appear the same in the moving system. \end{equation*} and will feel your normal weight.

definition requires the specification of six “curvature numbers” at approximate formula to express the increase of mass, for the case when \begin{equation} radius” would be

Just for fun, suppose that inside the space relative motion of the two observers is along their common $x$-axes. can measure.” But that is the whole problem: whether or not one $x'$-coordinate of some point with a meter stick. In addition, we had a law about how particles

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