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accidentprone
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c^2 occurs frequently in special relativity: in the Lorentz transformations, in forumlas for the interval, relativistic energy, and others too. Is there an intuitive reason for the high occurence of c^2?
accidentprone said:c^2 occurs frequently in special relativity: in the Lorentz transformations, in forumlas for the interval, relativistic energy, and others too. Is there an intuitive reason for the high occurence of c^2?
GrayGhost said:Good question. As JesseM pointed out already, it's due to the Pythagorean theorem. ...
...snip...
That said, the c2 that pops up often in SR is the direct result of Pythagoras' theorem relating lengths of the 2 systems using a right traingle as seen in EQN 1 above. We often see (v/c)2 as well, mainly because we like to reduce equations to their simplest form, or a form that presents the most inherent meaning at a glance ... eg Tau = t(1-(v/c)2)1/2
GrayGhost
robphy said:c^2 already pops up in (1+1)-Minowski spacetime... due the different choice of units (as mentioned earlier) and the square-interval posted by JesseM. Since the [Euclidean Space] Pythagorean Theorem doesn't play any role in (1+1)-Minkowski spacetime, it can't be the ultimate source of the c^2 in Special Relativity.
If there's a constant that arises from the [Euclidean] Pythagorean Theorem, it's pi.
accidentprone said:c^2 occurs frequently in special relativity: in the Lorentz transformations, in forumlas for the interval, relativistic energy, and others too. Is there an intuitive reason for the high occurence of c^2?
accidentprone said:c^2 occurs frequently in special relativity: in the Lorentz transformations, in forumlas for the interval, relativistic energy, and others too. Is there an intuitive reason for the high occurence of c^2?
The speed of light, denoted by c, is a fundamental constant in physics. It plays a crucial role in the theory of special relativity, which describes how the laws of physics behave in different reference frames moving at constant velocities. The square of the speed of light (c^2) appears in the famous equation E=mc^2, which relates energy (E) and mass (m). It is also a factor in the Lorentz transformation equations, which describe how measurements of time and space differ between observers in different frames of reference.
According to the theory of special relativity, the speed of light is an absolute speed limit in the universe. This means that no object or information can travel faster than c. This is due to the fact that as an object approaches the speed of light, its mass increases infinitely and the energy required to accelerate it further also approaches infinity. Therefore, it is physically impossible for anything to reach or exceed the speed of light.
One of the consequences of special relativity is time dilation, which states that time passes slower for a moving object relative to a stationary observer. The amount of time dilation is directly proportional to the velocity of the object, but also inversely proportional to the square root of 1-c^2/v^2, where v is the velocity of the object. This means that as an object approaches the speed of light, time dilation becomes more significant and time appears to slow down dramatically for the moving object.
Yes, the famous equation E=mc^2 can be rearranged to calculate the mass (m) of an object in terms of its energy (E) and the speed of light (c). This is known as the mass-energy equivalence formula and it shows that mass and energy are interchangeable. As an object's velocity approaches the speed of light, its mass increases significantly due to the presence of the c^2 term in the equation.
Another consequence of special relativity is length contraction, which states that a moving object appears shorter in the direction of motion when measured by a stationary observer. The amount of length contraction is also directly proportional to the velocity of the object, but inversely proportional to the square root of 1-c^2/v^2. This means that as an object approaches the speed of light, length contraction becomes more significant and the object appears to be compressed in the direction of motion.