Why does an accelerated charge radiate away energy?

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My textbook says:




"Neils Bohr objected to the idea of an electron orbiting a nucleus in a circular orbit. An electron experiences centripetal acceleration and an accelerated charge radiates away energy. So such an orbit would be unstable: the electron would spiral into the nucleus."




But why does a charge radiate away energy when accelerated? From my understanding of circular motion, if the electron is in circular motion, then the centripetal force that is acting on the electron only changes the electron's direction and not its linear velocity. And hence the electron's kinetic energy should remain constant.



Therefore, if the energy that the charge radiates shouldn't come from the kinetic energy then what type of energy would it radiate away when accelerated and why? Thanks.







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  • I think your question begs for a logical correction. Your core argument is that since the centripetal force in a circular motion acts at right angles to the velocity, it cannot change the kinetic energy and thus, the particle shouldn't be able to radiate away any energy because if the kinetic energy is not changing then where can the energy to be radiated away come from? But this argument is valid only for the case in which the particle is in a circular motion and not for a generic accelerated motion. So, that is the logical correction that I think must be pointed out in your question.
    – Dvij Mankad
    Sep 4 at 4:10






  • 1




    See en.wikipedia.org/wiki/Larmor_formula
    – J.G.
    Sep 4 at 5:46










  • Consider you hold a charge and another charge is attracted to it, but is held by a spring. Nothing is moving, no energy is emitted. Now, if you move you charge a bit closer to the other charge, that charge would attract to your charge stronger and stretch the spring a bit more. It takes energy to stretch the spring, where did this energy come from? Clearly from your hands, but how? Through the electromagnetic interaction between the charges. In other words, this energy was emitted by your charge and absorbed by the other charge. This would happen even if you move your charge along a circle.
    – safesphere
    Sep 4 at 6:41










  • A charge in circular motion would be essentially an alternating electric current.
    – Dmitry Grigoryev
    Sep 4 at 8:09






  • 1




    Iti s basic that change in direction also means change in velocity, altough it doesn't change $\vecv|$ (modulus), but direction changes, so there is an acceleration.
    – FGSUZ
    Sep 5 at 10:36















up vote
7
down vote

favorite
3












My textbook says:




"Neils Bohr objected to the idea of an electron orbiting a nucleus in a circular orbit. An electron experiences centripetal acceleration and an accelerated charge radiates away energy. So such an orbit would be unstable: the electron would spiral into the nucleus."




But why does a charge radiate away energy when accelerated? From my understanding of circular motion, if the electron is in circular motion, then the centripetal force that is acting on the electron only changes the electron's direction and not its linear velocity. And hence the electron's kinetic energy should remain constant.



Therefore, if the energy that the charge radiates shouldn't come from the kinetic energy then what type of energy would it radiate away when accelerated and why? Thanks.







share|cite|improve this question






















  • I think your question begs for a logical correction. Your core argument is that since the centripetal force in a circular motion acts at right angles to the velocity, it cannot change the kinetic energy and thus, the particle shouldn't be able to radiate away any energy because if the kinetic energy is not changing then where can the energy to be radiated away come from? But this argument is valid only for the case in which the particle is in a circular motion and not for a generic accelerated motion. So, that is the logical correction that I think must be pointed out in your question.
    – Dvij Mankad
    Sep 4 at 4:10






  • 1




    See en.wikipedia.org/wiki/Larmor_formula
    – J.G.
    Sep 4 at 5:46










  • Consider you hold a charge and another charge is attracted to it, but is held by a spring. Nothing is moving, no energy is emitted. Now, if you move you charge a bit closer to the other charge, that charge would attract to your charge stronger and stretch the spring a bit more. It takes energy to stretch the spring, where did this energy come from? Clearly from your hands, but how? Through the electromagnetic interaction between the charges. In other words, this energy was emitted by your charge and absorbed by the other charge. This would happen even if you move your charge along a circle.
    – safesphere
    Sep 4 at 6:41










  • A charge in circular motion would be essentially an alternating electric current.
    – Dmitry Grigoryev
    Sep 4 at 8:09






  • 1




    Iti s basic that change in direction also means change in velocity, altough it doesn't change $\vecv|$ (modulus), but direction changes, so there is an acceleration.
    – FGSUZ
    Sep 5 at 10:36













up vote
7
down vote

favorite
3









up vote
7
down vote

favorite
3






3





My textbook says:




"Neils Bohr objected to the idea of an electron orbiting a nucleus in a circular orbit. An electron experiences centripetal acceleration and an accelerated charge radiates away energy. So such an orbit would be unstable: the electron would spiral into the nucleus."




But why does a charge radiate away energy when accelerated? From my understanding of circular motion, if the electron is in circular motion, then the centripetal force that is acting on the electron only changes the electron's direction and not its linear velocity. And hence the electron's kinetic energy should remain constant.



Therefore, if the energy that the charge radiates shouldn't come from the kinetic energy then what type of energy would it radiate away when accelerated and why? Thanks.







share|cite|improve this question














My textbook says:




"Neils Bohr objected to the idea of an electron orbiting a nucleus in a circular orbit. An electron experiences centripetal acceleration and an accelerated charge radiates away energy. So such an orbit would be unstable: the electron would spiral into the nucleus."




But why does a charge radiate away energy when accelerated? From my understanding of circular motion, if the electron is in circular motion, then the centripetal force that is acting on the electron only changes the electron's direction and not its linear velocity. And hence the electron's kinetic energy should remain constant.



Therefore, if the energy that the charge radiates shouldn't come from the kinetic energy then what type of energy would it radiate away when accelerated and why? Thanks.









share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








edited Sep 4 at 5:24









Qmechanic♦

96.7k121631021




96.7k121631021










asked Sep 4 at 3:42









Bøbby Leung

1526




1526











  • I think your question begs for a logical correction. Your core argument is that since the centripetal force in a circular motion acts at right angles to the velocity, it cannot change the kinetic energy and thus, the particle shouldn't be able to radiate away any energy because if the kinetic energy is not changing then where can the energy to be radiated away come from? But this argument is valid only for the case in which the particle is in a circular motion and not for a generic accelerated motion. So, that is the logical correction that I think must be pointed out in your question.
    – Dvij Mankad
    Sep 4 at 4:10






  • 1




    See en.wikipedia.org/wiki/Larmor_formula
    – J.G.
    Sep 4 at 5:46










  • Consider you hold a charge and another charge is attracted to it, but is held by a spring. Nothing is moving, no energy is emitted. Now, if you move you charge a bit closer to the other charge, that charge would attract to your charge stronger and stretch the spring a bit more. It takes energy to stretch the spring, where did this energy come from? Clearly from your hands, but how? Through the electromagnetic interaction between the charges. In other words, this energy was emitted by your charge and absorbed by the other charge. This would happen even if you move your charge along a circle.
    – safesphere
    Sep 4 at 6:41










  • A charge in circular motion would be essentially an alternating electric current.
    – Dmitry Grigoryev
    Sep 4 at 8:09






  • 1




    Iti s basic that change in direction also means change in velocity, altough it doesn't change $\vecv|$ (modulus), but direction changes, so there is an acceleration.
    – FGSUZ
    Sep 5 at 10:36

















  • I think your question begs for a logical correction. Your core argument is that since the centripetal force in a circular motion acts at right angles to the velocity, it cannot change the kinetic energy and thus, the particle shouldn't be able to radiate away any energy because if the kinetic energy is not changing then where can the energy to be radiated away come from? But this argument is valid only for the case in which the particle is in a circular motion and not for a generic accelerated motion. So, that is the logical correction that I think must be pointed out in your question.
    – Dvij Mankad
    Sep 4 at 4:10






  • 1




    See en.wikipedia.org/wiki/Larmor_formula
    – J.G.
    Sep 4 at 5:46










  • Consider you hold a charge and another charge is attracted to it, but is held by a spring. Nothing is moving, no energy is emitted. Now, if you move you charge a bit closer to the other charge, that charge would attract to your charge stronger and stretch the spring a bit more. It takes energy to stretch the spring, where did this energy come from? Clearly from your hands, but how? Through the electromagnetic interaction between the charges. In other words, this energy was emitted by your charge and absorbed by the other charge. This would happen even if you move your charge along a circle.
    – safesphere
    Sep 4 at 6:41










  • A charge in circular motion would be essentially an alternating electric current.
    – Dmitry Grigoryev
    Sep 4 at 8:09






  • 1




    Iti s basic that change in direction also means change in velocity, altough it doesn't change $\vecv|$ (modulus), but direction changes, so there is an acceleration.
    – FGSUZ
    Sep 5 at 10:36
















I think your question begs for a logical correction. Your core argument is that since the centripetal force in a circular motion acts at right angles to the velocity, it cannot change the kinetic energy and thus, the particle shouldn't be able to radiate away any energy because if the kinetic energy is not changing then where can the energy to be radiated away come from? But this argument is valid only for the case in which the particle is in a circular motion and not for a generic accelerated motion. So, that is the logical correction that I think must be pointed out in your question.
– Dvij Mankad
Sep 4 at 4:10




I think your question begs for a logical correction. Your core argument is that since the centripetal force in a circular motion acts at right angles to the velocity, it cannot change the kinetic energy and thus, the particle shouldn't be able to radiate away any energy because if the kinetic energy is not changing then where can the energy to be radiated away come from? But this argument is valid only for the case in which the particle is in a circular motion and not for a generic accelerated motion. So, that is the logical correction that I think must be pointed out in your question.
– Dvij Mankad
Sep 4 at 4:10




1




1




See en.wikipedia.org/wiki/Larmor_formula
– J.G.
Sep 4 at 5:46




See en.wikipedia.org/wiki/Larmor_formula
– J.G.
Sep 4 at 5:46












Consider you hold a charge and another charge is attracted to it, but is held by a spring. Nothing is moving, no energy is emitted. Now, if you move you charge a bit closer to the other charge, that charge would attract to your charge stronger and stretch the spring a bit more. It takes energy to stretch the spring, where did this energy come from? Clearly from your hands, but how? Through the electromagnetic interaction between the charges. In other words, this energy was emitted by your charge and absorbed by the other charge. This would happen even if you move your charge along a circle.
– safesphere
Sep 4 at 6:41




Consider you hold a charge and another charge is attracted to it, but is held by a spring. Nothing is moving, no energy is emitted. Now, if you move you charge a bit closer to the other charge, that charge would attract to your charge stronger and stretch the spring a bit more. It takes energy to stretch the spring, where did this energy come from? Clearly from your hands, but how? Through the electromagnetic interaction between the charges. In other words, this energy was emitted by your charge and absorbed by the other charge. This would happen even if you move your charge along a circle.
– safesphere
Sep 4 at 6:41












A charge in circular motion would be essentially an alternating electric current.
– Dmitry Grigoryev
Sep 4 at 8:09




A charge in circular motion would be essentially an alternating electric current.
– Dmitry Grigoryev
Sep 4 at 8:09




1




1




Iti s basic that change in direction also means change in velocity, altough it doesn't change $\vecv|$ (modulus), but direction changes, so there is an acceleration.
– FGSUZ
Sep 5 at 10:36





Iti s basic that change in direction also means change in velocity, altough it doesn't change $\vecv|$ (modulus), but direction changes, so there is an acceleration.
– FGSUZ
Sep 5 at 10:36











4 Answers
4






active

oldest

votes

















up vote
10
down vote



accepted










It emits light, because it "stirs up" the electromagnetic field. To understand this, just dip your finger into a still pond and move it in a circle. Water waves will emanate from your finger. These waves have energy, which means energy is being taken away from you. Same goes for the charges.



enter image description here



In fact, this follows almost automatically from the finite propagation speed of light. The electric field of a stationary charge obeys Coulomb's law. If the charge suddenly starts moving, the field won't obey Coulomb's law anymore, but it can't instantly change everywhere because of the finite propagation speed. Instead a "shockwave" of information goes out from the charge at speed $c$. This shockwave contains electromagnetic energy and travels at the speed of light -- it is light.






share|cite|improve this answer




















  • thanks for this Knzhou, and for the very useful drawing. I have seen it a couple of times before and always wondered what the magnetic field looks like in the vicinity of the kink. Can you sketch it out for me? -Niels
    – niels nielsen
    Sep 4 at 4:25










  • @nielsnielsen For a plane wave $mathbfE = mathbfv times mathbfB$, so similarly here I think the magnetic field is pointing in/out of the page, with magnitude proportional to $|mathbfE|$.
    – knzhou
    Sep 4 at 4:36










  • This Phet simulation might be of interest? phet.colorado.edu/sims/radiating-charge/…
    – Farcher
    Sep 4 at 6:32










  • Thank you very much for the answer. You mentioned "because it 'stirs up' the electromagnetic field," do you mean that an accelerated charge will 'stir up' its own electric and magnetic field? Therefore in the case of an electron in orbital, is it that the electron stirs up its own electric and magnetic field?
    – Bøbby Leung
    Sep 4 at 9:42










  • @BøbbyLeung I wouldn't say that. There is just one electromagnetic field, not one electromagnetic field for every charge. If a flashlight emits some light and it travels millions of miles into space, "whose" field is it?
    – knzhou
    Sep 4 at 19:34

















up vote
3
down vote













An accelerating charge radiates energy because, according to Maxwell's equations, it produces an electromagnetic wave.




what type of energy would it radiate when accelerated and why?




In addition to kinetic energy, the electron-nucleus system also has energy stored in the electric field between the electron and the positively charged nucleus.






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    up vote
    0
    down vote














    From my understanding of circular motion, if the electron is in
    circular motion, then the centripetal force that is acting on the
    electron only changes the electron's direction and not its linear
    velocity. And hence the electron's kinetic energy should remain
    constant.




    We could speculate that the electron's kinetic energy would remain constant, if it did not radiate. But Bohr's whole argument was that the electron would lose its orbit, i.e., would lose its kinetic energy because it would radiate if it was orbiting the atom.




    Therefore, if the energy that the charge radiates shouldn't come from
    the kinetic energy then what type of energy would it radiate away when
    accelerated and why?




    Based on the argument above, Bohr, presumably, was thinking that the radiation energy would come from the electron's kinetic energy. This premise is supported by an observation on a macro level that an electron rotating in a uniform magnetic field is gradually losing its energy and spirals down.



    The electron radiates electromagnetic energy and it radiates it because it accelerates. The type of radiation specifically associated with the circular motion, i.e., due to the centripetal acceleration, is known as a synchrotron radiation, because it occurs in synchrotrons and other circular particle accelerators and is considered a drawback due to the loss of energy associated with radiation.



    The radiation power of a charged particle due to its acceleration is quantified by the Larmor formula:



    $P=frac q^2a^2 6piepsilon_0 c^3,$



    where $a$ is acceleration of a particle. More details related to the radiation due to the circular motion could be found in this Wikipedia article.






    share|cite|improve this answer





























      up vote
      -1
      down vote














      From my understanding of circular motion, if the electron is in circular motion, then the centripetal force that is acting on the electron only changes the electron's direction and not its linear velocity. And hence the electron's kinetic energy should remain constant.




      Being on the place of the moving around a nucleus electron, you will feel a force like in a carousel. The force drags you outwards, however, if the connection to the carousel is cut off, you fly tangentially away from the turning circle. Feeling a force, you are under acceleration and hence a circular motion (except the motion in free space around a massive body) is an acceleration.



      To make it even more visible, if you are sitting in a car blindfolded and the driver accelerates or turns right or left you are able to decide between this acceleration and the turns. But, if during your ride your car seat will be turned by 90°, you will call the turns falsely acceleration and braking; and the accelerations you will feel as the turns. In reality, blindfolded you couldn’t anymore follow your experiences and the circular motion is not decidable from linear acceleration.




      But why does a charge radiate away energy when accelerated?




      What you mention was found out when electrons are moving in a magnetic field. In the case, the trajectory of the electron is perpendicular to the magnetic field, the electron undergoes a turn perpendicular to both the magnetic field and the direction of it’s movement. It was observed that this time the electron emits photons and its kinetic energy decreases. The trajectory of the electron becomes a spiral path until the kinetic energy gets converted fully to radiation and the electron stops in the center of the spiral path.



      No rope nor magnetic field in the case of the nucleus and the electron; the electron simply couldn’t circle around the nucleus and Bohr’s model was discarded.






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        4 Answers
        4






        active

        oldest

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        4 Answers
        4






        active

        oldest

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        active

        oldest

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        active

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        up vote
        10
        down vote



        accepted










        It emits light, because it "stirs up" the electromagnetic field. To understand this, just dip your finger into a still pond and move it in a circle. Water waves will emanate from your finger. These waves have energy, which means energy is being taken away from you. Same goes for the charges.



        enter image description here



        In fact, this follows almost automatically from the finite propagation speed of light. The electric field of a stationary charge obeys Coulomb's law. If the charge suddenly starts moving, the field won't obey Coulomb's law anymore, but it can't instantly change everywhere because of the finite propagation speed. Instead a "shockwave" of information goes out from the charge at speed $c$. This shockwave contains electromagnetic energy and travels at the speed of light -- it is light.






        share|cite|improve this answer




















        • thanks for this Knzhou, and for the very useful drawing. I have seen it a couple of times before and always wondered what the magnetic field looks like in the vicinity of the kink. Can you sketch it out for me? -Niels
          – niels nielsen
          Sep 4 at 4:25










        • @nielsnielsen For a plane wave $mathbfE = mathbfv times mathbfB$, so similarly here I think the magnetic field is pointing in/out of the page, with magnitude proportional to $|mathbfE|$.
          – knzhou
          Sep 4 at 4:36










        • This Phet simulation might be of interest? phet.colorado.edu/sims/radiating-charge/…
          – Farcher
          Sep 4 at 6:32










        • Thank you very much for the answer. You mentioned "because it 'stirs up' the electromagnetic field," do you mean that an accelerated charge will 'stir up' its own electric and magnetic field? Therefore in the case of an electron in orbital, is it that the electron stirs up its own electric and magnetic field?
          – Bøbby Leung
          Sep 4 at 9:42










        • @BøbbyLeung I wouldn't say that. There is just one electromagnetic field, not one electromagnetic field for every charge. If a flashlight emits some light and it travels millions of miles into space, "whose" field is it?
          – knzhou
          Sep 4 at 19:34














        up vote
        10
        down vote



        accepted










        It emits light, because it "stirs up" the electromagnetic field. To understand this, just dip your finger into a still pond and move it in a circle. Water waves will emanate from your finger. These waves have energy, which means energy is being taken away from you. Same goes for the charges.



        enter image description here



        In fact, this follows almost automatically from the finite propagation speed of light. The electric field of a stationary charge obeys Coulomb's law. If the charge suddenly starts moving, the field won't obey Coulomb's law anymore, but it can't instantly change everywhere because of the finite propagation speed. Instead a "shockwave" of information goes out from the charge at speed $c$. This shockwave contains electromagnetic energy and travels at the speed of light -- it is light.






        share|cite|improve this answer




















        • thanks for this Knzhou, and for the very useful drawing. I have seen it a couple of times before and always wondered what the magnetic field looks like in the vicinity of the kink. Can you sketch it out for me? -Niels
          – niels nielsen
          Sep 4 at 4:25










        • @nielsnielsen For a plane wave $mathbfE = mathbfv times mathbfB$, so similarly here I think the magnetic field is pointing in/out of the page, with magnitude proportional to $|mathbfE|$.
          – knzhou
          Sep 4 at 4:36










        • This Phet simulation might be of interest? phet.colorado.edu/sims/radiating-charge/…
          – Farcher
          Sep 4 at 6:32










        • Thank you very much for the answer. You mentioned "because it 'stirs up' the electromagnetic field," do you mean that an accelerated charge will 'stir up' its own electric and magnetic field? Therefore in the case of an electron in orbital, is it that the electron stirs up its own electric and magnetic field?
          – Bøbby Leung
          Sep 4 at 9:42










        • @BøbbyLeung I wouldn't say that. There is just one electromagnetic field, not one electromagnetic field for every charge. If a flashlight emits some light and it travels millions of miles into space, "whose" field is it?
          – knzhou
          Sep 4 at 19:34












        up vote
        10
        down vote



        accepted







        up vote
        10
        down vote



        accepted






        It emits light, because it "stirs up" the electromagnetic field. To understand this, just dip your finger into a still pond and move it in a circle. Water waves will emanate from your finger. These waves have energy, which means energy is being taken away from you. Same goes for the charges.



        enter image description here



        In fact, this follows almost automatically from the finite propagation speed of light. The electric field of a stationary charge obeys Coulomb's law. If the charge suddenly starts moving, the field won't obey Coulomb's law anymore, but it can't instantly change everywhere because of the finite propagation speed. Instead a "shockwave" of information goes out from the charge at speed $c$. This shockwave contains electromagnetic energy and travels at the speed of light -- it is light.






        share|cite|improve this answer












        It emits light, because it "stirs up" the electromagnetic field. To understand this, just dip your finger into a still pond and move it in a circle. Water waves will emanate from your finger. These waves have energy, which means energy is being taken away from you. Same goes for the charges.



        enter image description here



        In fact, this follows almost automatically from the finite propagation speed of light. The electric field of a stationary charge obeys Coulomb's law. If the charge suddenly starts moving, the field won't obey Coulomb's law anymore, but it can't instantly change everywhere because of the finite propagation speed. Instead a "shockwave" of information goes out from the charge at speed $c$. This shockwave contains electromagnetic energy and travels at the speed of light -- it is light.







        share|cite|improve this answer












        share|cite|improve this answer



        share|cite|improve this answer










        answered Sep 4 at 3:54









        knzhou

        33.6k897169




        33.6k897169











        • thanks for this Knzhou, and for the very useful drawing. I have seen it a couple of times before and always wondered what the magnetic field looks like in the vicinity of the kink. Can you sketch it out for me? -Niels
          – niels nielsen
          Sep 4 at 4:25










        • @nielsnielsen For a plane wave $mathbfE = mathbfv times mathbfB$, so similarly here I think the magnetic field is pointing in/out of the page, with magnitude proportional to $|mathbfE|$.
          – knzhou
          Sep 4 at 4:36










        • This Phet simulation might be of interest? phet.colorado.edu/sims/radiating-charge/…
          – Farcher
          Sep 4 at 6:32










        • Thank you very much for the answer. You mentioned "because it 'stirs up' the electromagnetic field," do you mean that an accelerated charge will 'stir up' its own electric and magnetic field? Therefore in the case of an electron in orbital, is it that the electron stirs up its own electric and magnetic field?
          – Bøbby Leung
          Sep 4 at 9:42










        • @BøbbyLeung I wouldn't say that. There is just one electromagnetic field, not one electromagnetic field for every charge. If a flashlight emits some light and it travels millions of miles into space, "whose" field is it?
          – knzhou
          Sep 4 at 19:34
















        • thanks for this Knzhou, and for the very useful drawing. I have seen it a couple of times before and always wondered what the magnetic field looks like in the vicinity of the kink. Can you sketch it out for me? -Niels
          – niels nielsen
          Sep 4 at 4:25










        • @nielsnielsen For a plane wave $mathbfE = mathbfv times mathbfB$, so similarly here I think the magnetic field is pointing in/out of the page, with magnitude proportional to $|mathbfE|$.
          – knzhou
          Sep 4 at 4:36










        • This Phet simulation might be of interest? phet.colorado.edu/sims/radiating-charge/…
          – Farcher
          Sep 4 at 6:32










        • Thank you very much for the answer. You mentioned "because it 'stirs up' the electromagnetic field," do you mean that an accelerated charge will 'stir up' its own electric and magnetic field? Therefore in the case of an electron in orbital, is it that the electron stirs up its own electric and magnetic field?
          – Bøbby Leung
          Sep 4 at 9:42










        • @BøbbyLeung I wouldn't say that. There is just one electromagnetic field, not one electromagnetic field for every charge. If a flashlight emits some light and it travels millions of miles into space, "whose" field is it?
          – knzhou
          Sep 4 at 19:34















        thanks for this Knzhou, and for the very useful drawing. I have seen it a couple of times before and always wondered what the magnetic field looks like in the vicinity of the kink. Can you sketch it out for me? -Niels
        – niels nielsen
        Sep 4 at 4:25




        thanks for this Knzhou, and for the very useful drawing. I have seen it a couple of times before and always wondered what the magnetic field looks like in the vicinity of the kink. Can you sketch it out for me? -Niels
        – niels nielsen
        Sep 4 at 4:25












        @nielsnielsen For a plane wave $mathbfE = mathbfv times mathbfB$, so similarly here I think the magnetic field is pointing in/out of the page, with magnitude proportional to $|mathbfE|$.
        – knzhou
        Sep 4 at 4:36




        @nielsnielsen For a plane wave $mathbfE = mathbfv times mathbfB$, so similarly here I think the magnetic field is pointing in/out of the page, with magnitude proportional to $|mathbfE|$.
        – knzhou
        Sep 4 at 4:36












        This Phet simulation might be of interest? phet.colorado.edu/sims/radiating-charge/…
        – Farcher
        Sep 4 at 6:32




        This Phet simulation might be of interest? phet.colorado.edu/sims/radiating-charge/…
        – Farcher
        Sep 4 at 6:32












        Thank you very much for the answer. You mentioned "because it 'stirs up' the electromagnetic field," do you mean that an accelerated charge will 'stir up' its own electric and magnetic field? Therefore in the case of an electron in orbital, is it that the electron stirs up its own electric and magnetic field?
        – Bøbby Leung
        Sep 4 at 9:42




        Thank you very much for the answer. You mentioned "because it 'stirs up' the electromagnetic field," do you mean that an accelerated charge will 'stir up' its own electric and magnetic field? Therefore in the case of an electron in orbital, is it that the electron stirs up its own electric and magnetic field?
        – Bøbby Leung
        Sep 4 at 9:42












        @BøbbyLeung I wouldn't say that. There is just one electromagnetic field, not one electromagnetic field for every charge. If a flashlight emits some light and it travels millions of miles into space, "whose" field is it?
        – knzhou
        Sep 4 at 19:34




        @BøbbyLeung I wouldn't say that. There is just one electromagnetic field, not one electromagnetic field for every charge. If a flashlight emits some light and it travels millions of miles into space, "whose" field is it?
        – knzhou
        Sep 4 at 19:34










        up vote
        3
        down vote













        An accelerating charge radiates energy because, according to Maxwell's equations, it produces an electromagnetic wave.




        what type of energy would it radiate when accelerated and why?




        In addition to kinetic energy, the electron-nucleus system also has energy stored in the electric field between the electron and the positively charged nucleus.






        share|cite|improve this answer
























          up vote
          3
          down vote













          An accelerating charge radiates energy because, according to Maxwell's equations, it produces an electromagnetic wave.




          what type of energy would it radiate when accelerated and why?




          In addition to kinetic energy, the electron-nucleus system also has energy stored in the electric field between the electron and the positively charged nucleus.






          share|cite|improve this answer






















            up vote
            3
            down vote










            up vote
            3
            down vote









            An accelerating charge radiates energy because, according to Maxwell's equations, it produces an electromagnetic wave.




            what type of energy would it radiate when accelerated and why?




            In addition to kinetic energy, the electron-nucleus system also has energy stored in the electric field between the electron and the positively charged nucleus.






            share|cite|improve this answer












            An accelerating charge radiates energy because, according to Maxwell's equations, it produces an electromagnetic wave.




            what type of energy would it radiate when accelerated and why?




            In addition to kinetic energy, the electron-nucleus system also has energy stored in the electric field between the electron and the positively charged nucleus.







            share|cite|improve this answer












            share|cite|improve this answer



            share|cite|improve this answer










            answered Sep 4 at 3:53









            The Photon

            8,35811830




            8,35811830




















                up vote
                0
                down vote














                From my understanding of circular motion, if the electron is in
                circular motion, then the centripetal force that is acting on the
                electron only changes the electron's direction and not its linear
                velocity. And hence the electron's kinetic energy should remain
                constant.




                We could speculate that the electron's kinetic energy would remain constant, if it did not radiate. But Bohr's whole argument was that the electron would lose its orbit, i.e., would lose its kinetic energy because it would radiate if it was orbiting the atom.




                Therefore, if the energy that the charge radiates shouldn't come from
                the kinetic energy then what type of energy would it radiate away when
                accelerated and why?




                Based on the argument above, Bohr, presumably, was thinking that the radiation energy would come from the electron's kinetic energy. This premise is supported by an observation on a macro level that an electron rotating in a uniform magnetic field is gradually losing its energy and spirals down.



                The electron radiates electromagnetic energy and it radiates it because it accelerates. The type of radiation specifically associated with the circular motion, i.e., due to the centripetal acceleration, is known as a synchrotron radiation, because it occurs in synchrotrons and other circular particle accelerators and is considered a drawback due to the loss of energy associated with radiation.



                The radiation power of a charged particle due to its acceleration is quantified by the Larmor formula:



                $P=frac q^2a^2 6piepsilon_0 c^3,$



                where $a$ is acceleration of a particle. More details related to the radiation due to the circular motion could be found in this Wikipedia article.






                share|cite|improve this answer


























                  up vote
                  0
                  down vote














                  From my understanding of circular motion, if the electron is in
                  circular motion, then the centripetal force that is acting on the
                  electron only changes the electron's direction and not its linear
                  velocity. And hence the electron's kinetic energy should remain
                  constant.




                  We could speculate that the electron's kinetic energy would remain constant, if it did not radiate. But Bohr's whole argument was that the electron would lose its orbit, i.e., would lose its kinetic energy because it would radiate if it was orbiting the atom.




                  Therefore, if the energy that the charge radiates shouldn't come from
                  the kinetic energy then what type of energy would it radiate away when
                  accelerated and why?




                  Based on the argument above, Bohr, presumably, was thinking that the radiation energy would come from the electron's kinetic energy. This premise is supported by an observation on a macro level that an electron rotating in a uniform magnetic field is gradually losing its energy and spirals down.



                  The electron radiates electromagnetic energy and it radiates it because it accelerates. The type of radiation specifically associated with the circular motion, i.e., due to the centripetal acceleration, is known as a synchrotron radiation, because it occurs in synchrotrons and other circular particle accelerators and is considered a drawback due to the loss of energy associated with radiation.



                  The radiation power of a charged particle due to its acceleration is quantified by the Larmor formula:



                  $P=frac q^2a^2 6piepsilon_0 c^3,$



                  where $a$ is acceleration of a particle. More details related to the radiation due to the circular motion could be found in this Wikipedia article.






                  share|cite|improve this answer
























                    up vote
                    0
                    down vote










                    up vote
                    0
                    down vote










                    From my understanding of circular motion, if the electron is in
                    circular motion, then the centripetal force that is acting on the
                    electron only changes the electron's direction and not its linear
                    velocity. And hence the electron's kinetic energy should remain
                    constant.




                    We could speculate that the electron's kinetic energy would remain constant, if it did not radiate. But Bohr's whole argument was that the electron would lose its orbit, i.e., would lose its kinetic energy because it would radiate if it was orbiting the atom.




                    Therefore, if the energy that the charge radiates shouldn't come from
                    the kinetic energy then what type of energy would it radiate away when
                    accelerated and why?




                    Based on the argument above, Bohr, presumably, was thinking that the radiation energy would come from the electron's kinetic energy. This premise is supported by an observation on a macro level that an electron rotating in a uniform magnetic field is gradually losing its energy and spirals down.



                    The electron radiates electromagnetic energy and it radiates it because it accelerates. The type of radiation specifically associated with the circular motion, i.e., due to the centripetal acceleration, is known as a synchrotron radiation, because it occurs in synchrotrons and other circular particle accelerators and is considered a drawback due to the loss of energy associated with radiation.



                    The radiation power of a charged particle due to its acceleration is quantified by the Larmor formula:



                    $P=frac q^2a^2 6piepsilon_0 c^3,$



                    where $a$ is acceleration of a particle. More details related to the radiation due to the circular motion could be found in this Wikipedia article.






                    share|cite|improve this answer















                    From my understanding of circular motion, if the electron is in
                    circular motion, then the centripetal force that is acting on the
                    electron only changes the electron's direction and not its linear
                    velocity. And hence the electron's kinetic energy should remain
                    constant.




                    We could speculate that the electron's kinetic energy would remain constant, if it did not radiate. But Bohr's whole argument was that the electron would lose its orbit, i.e., would lose its kinetic energy because it would radiate if it was orbiting the atom.




                    Therefore, if the energy that the charge radiates shouldn't come from
                    the kinetic energy then what type of energy would it radiate away when
                    accelerated and why?




                    Based on the argument above, Bohr, presumably, was thinking that the radiation energy would come from the electron's kinetic energy. This premise is supported by an observation on a macro level that an electron rotating in a uniform magnetic field is gradually losing its energy and spirals down.



                    The electron radiates electromagnetic energy and it radiates it because it accelerates. The type of radiation specifically associated with the circular motion, i.e., due to the centripetal acceleration, is known as a synchrotron radiation, because it occurs in synchrotrons and other circular particle accelerators and is considered a drawback due to the loss of energy associated with radiation.



                    The radiation power of a charged particle due to its acceleration is quantified by the Larmor formula:



                    $P=frac q^2a^2 6piepsilon_0 c^3,$



                    where $a$ is acceleration of a particle. More details related to the radiation due to the circular motion could be found in this Wikipedia article.







                    share|cite|improve this answer














                    share|cite|improve this answer



                    share|cite|improve this answer








                    edited Sep 5 at 14:25

























                    answered Sep 5 at 10:01









                    V.F.

                    7,3812621




                    7,3812621




















                        up vote
                        -1
                        down vote














                        From my understanding of circular motion, if the electron is in circular motion, then the centripetal force that is acting on the electron only changes the electron's direction and not its linear velocity. And hence the electron's kinetic energy should remain constant.




                        Being on the place of the moving around a nucleus electron, you will feel a force like in a carousel. The force drags you outwards, however, if the connection to the carousel is cut off, you fly tangentially away from the turning circle. Feeling a force, you are under acceleration and hence a circular motion (except the motion in free space around a massive body) is an acceleration.



                        To make it even more visible, if you are sitting in a car blindfolded and the driver accelerates or turns right or left you are able to decide between this acceleration and the turns. But, if during your ride your car seat will be turned by 90°, you will call the turns falsely acceleration and braking; and the accelerations you will feel as the turns. In reality, blindfolded you couldn’t anymore follow your experiences and the circular motion is not decidable from linear acceleration.




                        But why does a charge radiate away energy when accelerated?




                        What you mention was found out when electrons are moving in a magnetic field. In the case, the trajectory of the electron is perpendicular to the magnetic field, the electron undergoes a turn perpendicular to both the magnetic field and the direction of it’s movement. It was observed that this time the electron emits photons and its kinetic energy decreases. The trajectory of the electron becomes a spiral path until the kinetic energy gets converted fully to radiation and the electron stops in the center of the spiral path.



                        No rope nor magnetic field in the case of the nucleus and the electron; the electron simply couldn’t circle around the nucleus and Bohr’s model was discarded.






                        share|cite|improve this answer
























                          up vote
                          -1
                          down vote














                          From my understanding of circular motion, if the electron is in circular motion, then the centripetal force that is acting on the electron only changes the electron's direction and not its linear velocity. And hence the electron's kinetic energy should remain constant.




                          Being on the place of the moving around a nucleus electron, you will feel a force like in a carousel. The force drags you outwards, however, if the connection to the carousel is cut off, you fly tangentially away from the turning circle. Feeling a force, you are under acceleration and hence a circular motion (except the motion in free space around a massive body) is an acceleration.



                          To make it even more visible, if you are sitting in a car blindfolded and the driver accelerates or turns right or left you are able to decide between this acceleration and the turns. But, if during your ride your car seat will be turned by 90°, you will call the turns falsely acceleration and braking; and the accelerations you will feel as the turns. In reality, blindfolded you couldn’t anymore follow your experiences and the circular motion is not decidable from linear acceleration.




                          But why does a charge radiate away energy when accelerated?




                          What you mention was found out when electrons are moving in a magnetic field. In the case, the trajectory of the electron is perpendicular to the magnetic field, the electron undergoes a turn perpendicular to both the magnetic field and the direction of it’s movement. It was observed that this time the electron emits photons and its kinetic energy decreases. The trajectory of the electron becomes a spiral path until the kinetic energy gets converted fully to radiation and the electron stops in the center of the spiral path.



                          No rope nor magnetic field in the case of the nucleus and the electron; the electron simply couldn’t circle around the nucleus and Bohr’s model was discarded.






                          share|cite|improve this answer






















                            up vote
                            -1
                            down vote










                            up vote
                            -1
                            down vote










                            From my understanding of circular motion, if the electron is in circular motion, then the centripetal force that is acting on the electron only changes the electron's direction and not its linear velocity. And hence the electron's kinetic energy should remain constant.




                            Being on the place of the moving around a nucleus electron, you will feel a force like in a carousel. The force drags you outwards, however, if the connection to the carousel is cut off, you fly tangentially away from the turning circle. Feeling a force, you are under acceleration and hence a circular motion (except the motion in free space around a massive body) is an acceleration.



                            To make it even more visible, if you are sitting in a car blindfolded and the driver accelerates or turns right or left you are able to decide between this acceleration and the turns. But, if during your ride your car seat will be turned by 90°, you will call the turns falsely acceleration and braking; and the accelerations you will feel as the turns. In reality, blindfolded you couldn’t anymore follow your experiences and the circular motion is not decidable from linear acceleration.




                            But why does a charge radiate away energy when accelerated?




                            What you mention was found out when electrons are moving in a magnetic field. In the case, the trajectory of the electron is perpendicular to the magnetic field, the electron undergoes a turn perpendicular to both the magnetic field and the direction of it’s movement. It was observed that this time the electron emits photons and its kinetic energy decreases. The trajectory of the electron becomes a spiral path until the kinetic energy gets converted fully to radiation and the electron stops in the center of the spiral path.



                            No rope nor magnetic field in the case of the nucleus and the electron; the electron simply couldn’t circle around the nucleus and Bohr’s model was discarded.






                            share|cite|improve this answer













                            From my understanding of circular motion, if the electron is in circular motion, then the centripetal force that is acting on the electron only changes the electron's direction and not its linear velocity. And hence the electron's kinetic energy should remain constant.




                            Being on the place of the moving around a nucleus electron, you will feel a force like in a carousel. The force drags you outwards, however, if the connection to the carousel is cut off, you fly tangentially away from the turning circle. Feeling a force, you are under acceleration and hence a circular motion (except the motion in free space around a massive body) is an acceleration.



                            To make it even more visible, if you are sitting in a car blindfolded and the driver accelerates or turns right or left you are able to decide between this acceleration and the turns. But, if during your ride your car seat will be turned by 90°, you will call the turns falsely acceleration and braking; and the accelerations you will feel as the turns. In reality, blindfolded you couldn’t anymore follow your experiences and the circular motion is not decidable from linear acceleration.




                            But why does a charge radiate away energy when accelerated?




                            What you mention was found out when electrons are moving in a magnetic field. In the case, the trajectory of the electron is perpendicular to the magnetic field, the electron undergoes a turn perpendicular to both the magnetic field and the direction of it’s movement. It was observed that this time the electron emits photons and its kinetic energy decreases. The trajectory of the electron becomes a spiral path until the kinetic energy gets converted fully to radiation and the electron stops in the center of the spiral path.



                            No rope nor magnetic field in the case of the nucleus and the electron; the electron simply couldn’t circle around the nucleus and Bohr’s model was discarded.







                            share|cite|improve this answer












                            share|cite|improve this answer



                            share|cite|improve this answer










                            answered Sep 4 at 5:55









                            HolgerFiedler

                            3,71531133




                            3,71531133



























                                 

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