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Dave9600
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SR says that as an object reaches the speed of light its mass approaches infinity. How can light reach the speed of light without having an infinite mass?
Okay...CompuChip said:Simple, it doesn't reach it :)
Light doesn't accelerate from a velocity below the speed of light. From the moment a photon gets created until the moment it is destroyed, it travels at the speed of light (in the medium it is in, of course).
Something which travels slower than c must have mass and cannot reach the speed of light. Something which travels at the speed of light must be massless and cannot reach speeds below c.
No mass... nothing to suck in.kavindra said:Why are photons affected by gravity of black holes if they have no mass? F=GMm/r2... So, if photons are massless, then they shouldn't be affected but on the contrary, they are sucked in.
Yes, they are moving at c from the moment they're created, and they don't decelerate when destroyed, they just get absorbed by some other particle.Dave9600 said:I guess I don't understand how something can be created / destroyed without acceleration / deceleration. Are you saying that photons are moving at C the instant they are created, and instantly decelerate to C=0 when destroyed?
Even in Newtonian gravity the rate at which an object accelerates in a gravitational field is totally independent of its own mass (remember F = ma, so ma=GMm/r^2 which implies a=GM/r^2). In general relativity gravity is not really a force but curvature of spacetime, and photons always follow geodesics which are the closest things to "straight lines" in curved spacetime, but which may look like curved paths from a purely spatial point of view.kavindra said:Why are photons affected by gravity of black holes if they have no mass? F=GMm/r2... So, if photons are massless, then they shouldn't be affected but on the contrary, they are sucked in.
Has this been measured, or is this an assumption based on SR?JesseM said:Yes, they are moving at c from the moment they're created, and they don't decelerate when destroyed, they just get absorbed by some other particle.
Sorry. = )kavindra said:No No No... I didn't mean that. I said if photons have zero mass, then they cann't be affected by gravitation. Actually photons have zero REST mass. But in motion, they too have mass.
The shortest path to what?fedaykin said:"I said if photons have zero mass, then they cann't be affected by gravitation."
This is not correct. Gravity is not viewed as a force, but as the curvature of space-time. Photons will follow geodesics (the shortest path on a curved space) in spacetime.
Since gravity is the warping of spacetime, it will affect the paths of photons.
But what is the other point?HallsofIvy said:The shortest path between two nearby points- in the same sense that a straight line is, in Euclidean geometry, the shortest path between two points.
But the other point... what is the photon traveling towards and why?fedaykin said:For where the points are on the geodesic, think of it as trying to go the shortest distance on the curve as possible, your starting point is wherever you want on the photons path.
That question is the reason I think it's better to use the other definition of a geodesic: It's the straightest path.Dave9600 said:But the other point... what is the photon traveling towards and why?
But a straight path implies direction towards something. What is the photon traveling towards? Or, what is causing photons to move in a straight path?Fredrik said:That question is the reason I think it's better to use the other definition of a geodesic: It's the straightest path.
The definition of a geodesic as the shortest/longest path is appropriate when two points on the path are known. The definition as the straightest path is appropriate when one point and the tangent vector (i.e. the velocity) at that point is known.
Conservation of momentum.Dave9600 said:what is causing photons to move in a straight path?
A straight path implies direction towards something just as much as a curved path would.Dave9600 said:But a straight path implies direction towards something.
I don't understand what you're asking here. The photon continues to travel until it runs into mass.Dave9600 said:What is the photon traveling towards?
An analogy here could be an electric current, it always looks for the path of least resistance, be it a straight path or curved.Dave9600 said:Or, what is causing photons to move in a straight path?
One important thing to realize, though, is that a photon doesn't follow a geodesic path which is the shortest one in curved space, instead it follows a geodesic path in spacetime. For a slower-than-light-object the geodesic path actually maximizes the proper time (time as measured by a clock following that worldline), rather than minimizing the spatial distance. Not having studied GR I'm not actually sure how a geodesic in spacetime is defined for a photon (whose path always has zero proper time), but presumably it's still different than a geodesic in space would be.fedaykin said:For where the points are on the geodesic, think of it as trying to go the shortest distance on the curve as possible, your starting point is wherever you want on the photons path.
When you warp the space a photon is traveling in, you create a new shortest path for it.
Saying that a photon travels on a geodesic means a geodesic of spacetime. Spacetime is four dimensional without any particular preferred 3D+T slicing, so you cannot simply translate this geodesic to particular spatial directions.Dave9600 said:But a straight path implies direction towards something. What is the photon traveling towards? Or, what is causing photons to move in a straight path?
"Conservation of momentum" isn't a bad answer, but I prefer to think of it simply as one of the postulates of the theory. We assume that null geodesics can be used to represent the world lines of massless particles, and only experiments can tell us if the theory (which includes that assumption) agrees with reality.Dave9600 said:what is causing photons to move in a straight path?
Minor quibble: timelike geodesics represent the worldlines of massive particles, while lightlike geodesics represent the worldlines of photons and other massless particles. And I don't think this is actually a postulate of the theory, but is rather derived from the Einstein field equations.Fredrik said:We assume that timelike geodesics can be used to represent the world lines of massless particles
Oops. Thanks for catching it so fast that I could edit it.JesseM said:Minor quibble: timelike geodesics represent the worldlines of massive particles, while lightlike geodesics represent the worldlines of photons.
Hm, I have to think about this, but right now I have to get some sleep. So for now I'll just say that even though Einstein's equation completely defines the mathematical model of spacetime that we use in GR, it doesn't completely define GR as a theory of physics. We also have to postulate what things in the model correspond to things in the real world. For example, we have to postulate that a clock measures the proper time (defined as the familiar integral) along the curve that represents its motion. The idea that the motion of a particle is described by a geodesic must also be postulated.JesseM said:And I don't think this is actually a postulate of the theory, but is rather derived from the Einstein field equations.
The paradox of light's mass and speed refers to the fact that while light has no mass, it still has a constant speed. According to Einstein's theory of relativity, the speed of light is the same in all frames of reference, regardless of the observer's velocity. This contradicts Newton's laws of motion which state that the speed of an object is dependent on its mass and the force acting upon it.
Light is considered to have no mass because it does not have a rest mass, meaning it does not have a mass when it is at rest. While it does have energy, it is considered to be massless because its rest mass is equal to zero. This is also why light is able to move at the speed of light, as objects with mass cannot reach this speed according to Einstein's theory of relativity.
The constant speed of light can be explained by its nature as an electromagnetic wave. Unlike objects with mass that require a force to accelerate, light does not require a force to maintain its speed. Instead, it is governed by the properties of space and time, as described by Einstein's theory of relativity.
While the speed of light is considered to be constant, it can change when it passes through different mediums. This is due to the interaction of light with the particles in the medium, causing it to slow down or speed up. This phenomenon is known as refraction and is responsible for the bending of light when it passes through materials such as water or glass.
The paradox of light's mass and speed has greatly influenced our understanding of the universe and has led to the development of theories such as special relativity and quantum mechanics. It has also helped us to better understand the fundamental properties of space and time and how they interact with matter and energy. Additionally, the constant speed of light has been used as a fundamental constant in many equations and theories, allowing us to make precise calculations and predictions about the behavior of the universe.