Why do electromagnetic waves have it's magnetic and electric field intensities in the same phase?












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My question is exactly about that in the elctromagnetic waves if we consider the electric field as a sine function, the magnetic field will be also a sine function, but i am confused why is that this way, if i look at the maxwells equation, the changing magnetic field generates the electric field and the changing electric field generates the magnetic field, so according to my opinion if the accelerating electron generates a sine electric field change, then its magnetic field should be cosine function because d(sinx)/dx=cosx










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    $begingroup$


    My question is exactly about that in the elctromagnetic waves if we consider the electric field as a sine function, the magnetic field will be also a sine function, but i am confused why is that this way, if i look at the maxwells equation, the changing magnetic field generates the electric field and the changing electric field generates the magnetic field, so according to my opinion if the accelerating electron generates a sine electric field change, then its magnetic field should be cosine function because d(sinx)/dx=cosx










    share|cite|improve this question







    New contributor




    Bálint Tatai is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
    Check out our Code of Conduct.







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      3












      3








      3





      $begingroup$


      My question is exactly about that in the elctromagnetic waves if we consider the electric field as a sine function, the magnetic field will be also a sine function, but i am confused why is that this way, if i look at the maxwells equation, the changing magnetic field generates the electric field and the changing electric field generates the magnetic field, so according to my opinion if the accelerating electron generates a sine electric field change, then its magnetic field should be cosine function because d(sinx)/dx=cosx










      share|cite|improve this question







      New contributor




      Bálint Tatai is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
      Check out our Code of Conduct.







      $endgroup$




      My question is exactly about that in the elctromagnetic waves if we consider the electric field as a sine function, the magnetic field will be also a sine function, but i am confused why is that this way, if i look at the maxwells equation, the changing magnetic field generates the electric field and the changing electric field generates the magnetic field, so according to my opinion if the accelerating electron generates a sine electric field change, then its magnetic field should be cosine function because d(sinx)/dx=cosx







      electromagnetic-radiation






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      share|cite|improve this question







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      asked 5 hours ago









      Bálint TataiBálint Tatai

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          The Maxwell equations that relate electric and magnetic fields to each other read (in vacuum, in SI units) as
          begin{align}
          nabla times mathbf E & = -frac{partialmathbf B}{partial t} \
          nabla times mathbf B & = frac{1}{c^2} frac{partialmathbf E}{partial t},
          end{align}

          where the notation $nabla times{cdot}$ is a spatial derivative (the curl). This means that both sides have derivatives, and if you're applying them to a function like $cos(kx-omega t)$, then they will both change the cosine into a sine. This is what locks the phase of both waves to equal values.






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            $begingroup$

            The Maxwell equations that relate electric and magnetic fields to each other read (in vacuum, in SI units) as
            begin{align}
            nabla times mathbf E & = -frac{partialmathbf B}{partial t} \
            nabla times mathbf B & = frac{1}{c^2} frac{partialmathbf E}{partial t},
            end{align}

            where the notation $nabla times{cdot}$ is a spatial derivative (the curl). This means that both sides have derivatives, and if you're applying them to a function like $cos(kx-omega t)$, then they will both change the cosine into a sine. This is what locks the phase of both waves to equal values.






            share|cite|improve this answer









            $endgroup$


















              3












              $begingroup$

              The Maxwell equations that relate electric and magnetic fields to each other read (in vacuum, in SI units) as
              begin{align}
              nabla times mathbf E & = -frac{partialmathbf B}{partial t} \
              nabla times mathbf B & = frac{1}{c^2} frac{partialmathbf E}{partial t},
              end{align}

              where the notation $nabla times{cdot}$ is a spatial derivative (the curl). This means that both sides have derivatives, and if you're applying them to a function like $cos(kx-omega t)$, then they will both change the cosine into a sine. This is what locks the phase of both waves to equal values.






              share|cite|improve this answer









              $endgroup$
















                3












                3








                3





                $begingroup$

                The Maxwell equations that relate electric and magnetic fields to each other read (in vacuum, in SI units) as
                begin{align}
                nabla times mathbf E & = -frac{partialmathbf B}{partial t} \
                nabla times mathbf B & = frac{1}{c^2} frac{partialmathbf E}{partial t},
                end{align}

                where the notation $nabla times{cdot}$ is a spatial derivative (the curl). This means that both sides have derivatives, and if you're applying them to a function like $cos(kx-omega t)$, then they will both change the cosine into a sine. This is what locks the phase of both waves to equal values.






                share|cite|improve this answer









                $endgroup$



                The Maxwell equations that relate electric and magnetic fields to each other read (in vacuum, in SI units) as
                begin{align}
                nabla times mathbf E & = -frac{partialmathbf B}{partial t} \
                nabla times mathbf B & = frac{1}{c^2} frac{partialmathbf E}{partial t},
                end{align}

                where the notation $nabla times{cdot}$ is a spatial derivative (the curl). This means that both sides have derivatives, and if you're applying them to a function like $cos(kx-omega t)$, then they will both change the cosine into a sine. This is what locks the phase of both waves to equal values.







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered 4 hours ago









                Emilio PisantyEmilio Pisanty

                83.4k22203417




                83.4k22203417






















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