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The energy passing through area A in time Δ t is

u × volume = u A c Δ t .

The energy per unit area per unit time passing through a plane perpendicular to the wave, called the energy flux and denoted by S , can be calculated by dividing the energy by the area A and the time interval Δ t .

S = Energy passing area A in time Δ t A Δ t = u c = ε 0 c E 2 = 1 μ 0 E B .

More generally, the flux of energy through any surface also depends on the orientation of the surface. To take the direction into account, we introduce a vector S , called the Poynting vector    , with the following definition:

S = 1 μ 0 E × B .

The cross-product of E and B points in the direction perpendicular to both vectors. To confirm that the direction of S is that of wave propagation, and not its negative, return to [link] . Note that Lenz’s and Faraday’s laws imply that when the magnetic field shown is increasing in time, the electric field is greater at x than at x + Δ x . The electric field is decreasing with increasing x at the given time and location. The proportionality between electric and magnetic fields requires the electric field to increase in time along with the magnetic field. This is possible only if the wave is propagating to the right in the diagram, in which case, the relative orientations show that S = 1 μ 0 E × B is specifically in the direction of propagation of the electromagnetic wave.

The energy flux at any place also varies in time, as can be seen by substituting u from [link] into [link] .

S ( x , t ) = c ε 0 E 0 2 cos 2 ( k x ω t )

Because the frequency of visible light is very high, of the order of 10 14 Hz, the energy flux for visible light through any area is an extremely rapidly varying quantity. Most measuring devices, including our eyes, detect only an average over many cycles. The time average of the energy flux is the intensity I of the electromagnetic wave and is the power per unit area. It can be expressed by averaging the cosine function in [link] over one complete cycle, which is the same as time-averaging over many cycles (here, T is one period):

I = S avg = c ε 0 E 0 2 1 T 0 T cos 2 ( 2 π t T ) d t .

We can either evaluate the integral, or else note that because the sine and cosine differ merely in phase, the average over a complete cycle for cos 2 ( ξ ) is the same as for sin 2 ( ξ ) , to obtain

cos 2 ξ = 1 2 [ cos 2 ξ + sin 2 ξ ] = 1 2 1 = 1 2 .

where the angle brackets stand for the time-averaging operation. The intensity of light moving at speed c in vacuum is then found to be

I = S avg = 1 2 c ε 0 E 0 2

in terms of the maximum electric field strength E 0 , which is also the electric field amplitude. Algebraic manipulation produces the relationship

I = c B 0 2 2 μ 0

where B 0 is the magnetic field amplitude, which is the same as the maximum magnetic field strength. One more expression for I avg in terms of both electric and magnetic field strengths is useful. Substituting the fact that c B 0 = E 0 , the previous expression becomes

I = E 0 B 0 2 μ 0 .

We can use whichever of the three preceding equations is most convenient, because the three equations are really just different versions of the same result: The energy in a wave is related to amplitude squared. Furthermore, because these equations are based on the assumption that the electromagnetic waves are sinusoidal, the peak intensity is twice the average intensity; that is, I 0 = 2 I .

Questions & Answers

Why does the lines of force not touch each other 🇲🇲
Gbemisola Reply
what is unit
Rayyanu Reply
Please canu get more questions on electric field and electric flux please
Gbemisola
is electric field directly proportional to the squared of a distance
Benjamin Reply
No electric field is inversely proportional to the squared distance between the charges
Gbemisola
lets treat linear expansivity please
Ujah Reply
The bullet 2.00cm long is fired at 420/s and passes straight through a 10.0 cm thick board existing at 280 m/s.What is the average acceleration of the bullet through the board?
FAUSTINA
an unstretched spring is 12cm long .A load of 5N stretched it to 15cm .how long will it be under a load of 15N?
Morapeli
hi
Africa
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Benjamin
Benjamin how are u are u a freshman in the university
Africa
like 100 level
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Benjamin
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studying what
Africa
Compare the electric flux through the surface of a cube of side length a that has a charge q at its center to the flux through a spherical surface of radius a with a charge q at its center.
Shari Reply
please I want to know how to solve increase in length
Ujah
Why a charged capacitor has potential difference but not emf
Gideon Reply
what is the dimension symbol of temperature?
Keren Reply
what is the dimension symbol of temperature?
Keren
what's the meaning of enthalpy in terms of latent heat, internal energy, phase change
Anthony Reply
Enthalpy is the degree ofdisorderlinessof a substance
Gbemisola
how to convert Kelvin to centigrade
Sangeetha Reply
what is the s, p, d, f in this table
Sangeetha
s, p, d, f in this table
Sangeetha
what kind of table this
Vengata
Periodic table
Gbemisola
what are waves
KENNETH Reply
In physics, mathematics, and related fields, a wave is a propagating dynamic disturbance (change from equilibrium) of one or more quantities
Abdikadir
Discuss how would orient a planar surface of area A in a uniform electric field of magnitude E0 to obtain (a) the maximum flux and (b) the minimum flux through the area.
KARAN Reply
I'm just doing the first 3 with this message. but thankyou for the time your obviously intending to support us with. viva la accumulation
Marcel
Find the net capacitance of the combination of series and parallel capacitors shown belo
jean Reply
what is ohm?
Sharafat Reply
calculate ideal gas pressure of 0.300mol,v=2L T=40°c
Viola Reply
what is principle of superposition
Jyoti Reply
Practice Key Terms 1

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Source:  OpenStax, University physics volume 2. OpenStax CNX. Oct 06, 2016 Download for free at http://cnx.org/content/col12074/1.3
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