How Black Holes Absorb Light Despite Photons Being Massless

In summary, according to classical mechanics, the force acting on an object with mass m in the gravitational field of a central mass M is F = - \frac{{M \cdot G \cdot r}}{{\left| r \right|^3 }} and the resulting acceleration is \ddot r = \frac{F}{m} . However, according to general relativity, the force acting on an object with mass m in the gravitational field of a central mass M is F = - \frac{{M \cdot G \cdot r}}{{\left| r \right|^3 }} and the resulting acceleration is \ddot r = \frac{F}{m} .
  • #1
Muhammad Valent
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We know light made up of photons which is massless, but why it can absorbed by black hole? Is it becuz the Einstein's relativity about every object can curve time space
 
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  • #2
Muhammad Valent said:
We know light made up of photons which is massless, but why it can absorbed by black hole? Is it becuz the Einstein's relativity about every object can curve time space
LIght doesn't have mass but it has momentum and it moves along geodesics just like everything else that is not being acted on by outside forces.
 
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  • #3
phinds said:
LIght doesn't have mass but it has momentum and it moves along geodesics just like everything else that is not being acted on by outside forces.

But Accord to momentum itu also need mass "p =mv which is non
 
  • #4
##p=mv## is a classical formula that is valid only when ##m## is not zero and ##v## is small compared with the speed of light. Neither of these are true of photons, so you have to use the more general formula ##E^2=(mc^2)^2+(pc)^2##.
 
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  • #5
Muhammad Valent said:
But Accord to momentum itu also need mass "p =mv which is non

I can also write the momentum of light as p = ħk. So where is the "mass" requirement there?

Please note that even before 1900, i.e. before Special Relativity and Quantum Mechanics, classical theory of electromagnetism and light already know about the momentum of light, all without even considering the picture that light consist of "photons" or the possibility that it has mass. So even back then, there was zero need to introduce mass to account for the momentum of light that they had observed. This means that just because something has a momentum, it doesn't automatically means that it must also have a mass.

BTW, in solid state physics, we also designate a crystal momentum as p=ħk without invoking any mass. So this isn't specific just to light. It means that there is a more universal definition of momentum than what you already know.

Zz.
 
  • #6
Photons have a rest mass of zero, but they can never be at rest.

Consider that photons have a defined energy and then apply energy mass equivalence. This is a bit of hand waving, but should be adequate to answer your original question.
 
  • #7
Eric Bretschneider said:
Photons have a rest mass of zero, but they can never be at rest.

Consider that photons have a defined energy and then apply energy mass equivalence. This is a bit of hand waving, but should be adequate to answer your original question.

You cannot simply "apply" the mass-energy equivalence, because the "mass" in that is the rest/invariant mass. It will also mess up the full relativistic energy equation, because now, the "m" in E2 = (pc)2 + (mc2)2 is no longer zero.

Zz.
 
  • #8
Muhammad Valent said:
Is it becuz the Einstein's relativity about every object can curve time space

Yes. That was precisely the point that made Einstein famous to the general public. Newton's theory of gravitation predicted light, with no mass, will not be affected by gravity. Einstein predicted that light, because it follows geodesics in distorted space-time, will be affected. Well-respected astronomer Sir Arthur Eddington, through observations of a solar eclipse, verified that Einstein was right and Newton was wrong.

Not merely in the actual fact, but the amount to which it is bent by gravity is precisely predicted by general relativity. A lot of people seem to miss the fact that when physics makes predictions, they have actual numerical values.
 
  • #9
RPinPA said:
Newton's theory of gravitation predicted light, with no mass, will not be affected by gravity.

Can you provide a corresponding calculation? In case of light deflection by a central mass I get half the effect compared to relativity.
 
  • #10
RPinPA said:
... Newton's theory of gravitation predicted light, with no mass, will not be affected by gravity.

DrStupid said:
Can you provide a corresponding calculation? In case of light deflection by a central mass I get half the effect compared to relativity.

I'm puzzled. How could you do a calculation in Newtonian physics that says light, being massless, is affected by gravity at anything other than zero effect? How does Newtonian gravity affect something that has no mass?
 
  • #11
phinds said:
How could you do a calculation in Newtonian physics that says light, being massless, is affected by gravity at anything other than zero effect?

The gravitational force is zero but not the effect. Keep in mind that the force required to accelerate a massless object is zero too in classical mechanics. Calculating the resulting effect is quite easy:

According to Newton's law of gravitaton, the force acting on an object with mass m in the gravitational field of a central mass M is

[itex]F = - \frac{{M \cdot G \cdot r}}{{\left| r \right|^3 }} \cdot m[/itex]

According to the second law of motion the resulting acceleration is

[itex]\ddot r = \frac{F}{m} = - \frac{{M \cdot G \cdot r}}{{\left| r \right|^3 }} \cdot \frac{m}{m}[/itex]

If light is assumed to be massless (that's not obvious in classical mechanics) L'Hôpital's rule results in

[itex]\mathop {\lim }\limits_{m \to 0} \ddot r = - \frac{{M \cdot G \cdot r}}{{\left| r \right|^3 }}[/itex]
 
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1. How can black holes absorb light if photons have no mass?

Despite having no mass, photons still have energy and momentum. When they get too close to a black hole, they can be captured by its strong gravitational pull, just like any other object with mass.

2. Why doesn't the light escape from the black hole?

As the photons get closer to the black hole, the gravitational pull becomes stronger, and they lose more and more energy. Eventually, they reach a point of no return, known as the event horizon, where the gravitational pull is so strong that even light cannot escape.

3. Can black holes absorb all types of light?

Yes, black holes can absorb all types of light, including visible light, infrared light, ultraviolet light, and even X-rays and gamma rays. The strength of the gravitational pull depends on the mass of the black hole, so the type of light does not affect its absorption.

4. How do we know that black holes absorb light?

We can observe the effects of black holes on the light around them. For example, we can see stars and other objects behind a black hole appear distorted or even disappear as the light gets bent and absorbed by the black hole's gravity.

5. Is all light that enters a black hole absorbed?

No, not all light that enters a black hole is absorbed. Some photons may have enough energy to escape the event horizon and be emitted back into space. This is known as Hawking radiation and is a result of the quantum effects near the event horizon.

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