Fresnel Equations: What are they? (Derivation & Explanation)

Contents

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Key learnings:

Fresnel Equations Definition: Fresnel Equations describe the ratios of electric fields of reflected and transmitted waves to the incident wave.
Light Reflection and Transmission: These equations explain how light reflects and transmits at the boundary between two different mediums.
Historical Insight: Augustin-Jean Fresnel developed these equations, understanding light as a transverse wave.
Polarizations: Light polarization can be S (perpendicular) or P (parallel) to the plane of incidence.
Fresnel Equations Derivation: The detailed derivation shows how to calculate reflection and transmission coefficients for both S-polarization and P-polarization.

What are the Fresnel Equations?

The Fresnel Equations (also known as Fresnel coefficients) are defined as the ratios of the electric field of reflected and transmitted waves to the incident wave. These complex ratios describe both the relative amplitude and the phase shifts between the waves.

The Fresnel Equations describe the reflection and transmission of light at the interface between two different mediums. Introduced by Augustin-Jean Fresnel, they explain how light behaves as a transverse wave.

When light hits the surface of a dielectric, it reflects and refracts depending on the angle of incidence. The direction of the reflected wave follows the “Law of Reflection”.

We see the Fresnel effect in everyday life, on both shiny and rough surfaces. It’s especially clear on the water surface. When light hits water from the air, it reflects based on the angle of incidence.

The Fresnel effect is everywhere. Look around and you’ll see many examples. This effect greatly depends on the angle of incidence.

The angle of incidence is the angle between the line of sight and surface of the object you are looking for. The below figure shows the effect of the angle of an incident in Fresnel reflection.

S and P Polarizations

The plane which has the surface normal and the propagation vector of the incoming radiation is known as the plane of incidence or incidence plane.

The plane of incidence plays an important role in the strength of reflection of incident light polarization. The polarization is defined as a property of a transverse wave that specifies the geometrical orientation of the oscillation.

There are two types of polarization;

S-Polarization
P-Polarization

When the polarization of light is perpendicular to the plane of the incident, the polarization is known as S-polarization. The ‘S’ word comes from the German word senkrecht that means perpendicular. S-polarization is also known as Transverse Electric (TE).

When the polarization of light is parallel to the plane of an incident or it lying in the plane of an incident. The plane is known as P-Polarization. S-polarization is also known as Transverse Magnetic (TM).

The below figure shows that the incident light is reflected and transmitted in S-polarization and P-Polarization.

Fresnel Equations Complex Index of Refraction

The Fresnel Equations are a complex equation that means it considers the magnitude and phase both. The Fresnel Equations represents in terms of the electromagnetic field complex amplitude that consider the phase besides power.

These equations are the ratios of an electromagnetic field and it makes in various forms. The complex amplitude coefficients are represented by r and t.

The reflection coefficient ‘r’ is a ratio of electric field complex amplitude of the reflected wave to the incident wave. And the reflection coefficient ‘t’ is a ratio of electric field complex amplitude of the transmitted wave to the incident wave.

As shown in the above figure, we have assumed that the angle of incidence is θ_i, reflected at an angle of θ_r, and transmitted at an angle of θ_t.

N_i is the refractive indices of a medium of incident light and N_t is the refractive indices of a medium of transmitted light.

Hence, there are four Fresnel Equations; two equations for reflection coefficient ‘r’ that is (r_p and r_s) and two equations for reflection coefficient ‘t’ that is (t_p and t_s).

Fresnel Equations Derivation

Let’s assume that incident light reflects as shown in the above figure. In the first case, we will derive a Fresnel Equation for S-Polarization.

For S-Polarization, parallel component E and perpendicular component B is continuous across the boundary between two media.

Hence from the boundary condition, we can write equations for E-field and B-field,

(1) $\begin{equation*}E_i + E_r = E_t\end{equation*}$

(2) $\begin{equation*}B_i \cos(\theta_i) - B_r \cos(\theta_r) = B_t \cos(\theta_t)\end{equation*}$

We use the below relation between B and E to eliminate B.

$B = \frac{nE}{c_0}$

And from the law of reflection,

$\theta_i = \theta_r$

Put this value in eq-2,

(3) $\begin{equation*} \frac{n_i E_i}{c_0} \cos(\theta_i) - \frac{n_i E_r}{c_0} \cos(\theta_i) = \frac{n_t E_t}{c_0} \cos(\theta_t) \end{equation*}$

(4) $\begin{equation*}n_i \cos(\theta_i) [ E_i - E_r ] = n_t E_t \cos(\theta_t) \end{equation*}$

(5) $\begin{equation*}n_i \cos(\theta_i) [ E_i - E_r ] = n_t [ E_i + E_r ] \cos(\theta_t) \end{equation*}$

(6) $\begin{equation*}n_i E_i \cos(\theta_i) - n_i E_r \cos(\theta_i) = n_t E_i \cos(\theta_t) + n_t E_r \cos(\theta_t)\end{equation*}$

(7) $\begin{equation*}n_i E_i \cos(\theta_i) - n_t E_i \cos(\theta_t) = n_t E_r \cos(\theta_t) + n_i E_r \cos(\theta_i) \end{equation*}$

(8) $\begin{equation*}E_i [ n_i \cos(\theta_i) - n_t \cos(\theta_t) ] = E_r [n_t \cos(\theta_t) + n_i \cos(\theta_i)]\end{equation*}$

(9) $\begin{equation*}r_s = \frac{E_r}{E_i} = \frac{n_i \cos(\theta_i) - n_t \cos(\theta_t)}{n_t \cos(\theta_t) + n_i \cos(\theta_i)}\end{equation*}$

Now, for reflection coefficient t, from eq-1 and eq-4,

(10) $\begin{equation*}n_i \cos(\theta_i) [ E_i - (E_t - E_i) ] = n_t E_t \cos(\theta_t) \end{equation*}$

(11) $\begin{equation*}n_i \cos(\theta_i) [ 2E_i - E_t ] = n_t E_t \cos(\theta_t) \end{equation*}$

(12) $\begin{equation*} 2E_i n_i \cos(\theta_i) - E_t n_i \cos(\theta_i) = n_t E_t \cos(\theta_t) \end{equation*}$

(13) $\begin{equation*} 2E_i n_i \cos(\theta_i) = E_t n_i \cos(\theta_i) + n_t E_t \cos(\theta_t) \end{equation*}$

(14) $\begin{equation*}t_s = \frac{E_t}{E_i} = \frac{2 n_i \cos(\theta_i)}{ n_i \cos(\theta_i) + n_t \cos(\theta_t)} \end{equation*}$

These are the Fresnel Equations for perpendicularly polarized light (S-Polarization).

Now, let’s derive equations for parallel polarized light (P-Polarization).

For S-Polarization, equations for E-field and B-field is;

(15) $\begin{equation*}E_i \cos(\theta_i) + E_r \cos(\theta_i) = E_t \cos(\theta_t)\end{equation*}$

(16) $\begin{equation*}B_i - B_r = B_t\end{equation*}$

We use the below relation between B and E to eliminate B.

$B = \frac{nE}{c_0}$

(17) $\begin{equation*}n_i E_i - n_i E_r = n_t E_t\end{equation*}$

$n_i [E_i - E_r] = n_t E_t$

$\frac{n_i}{n_t} [E_i - E_r] = E_t$

Put this value in eq-15,

(18) $\begin{equation*}E_i \cos(\theta_i) + E_r \cos(\theta_i) = \frac{n_i}{n_t} [E_i - E_r] \cos(\theta_t)\end{equation*}$

(19) $\begin{equation*}n_t [E_i \cos(\theta_i) + E_r \cos(\theta_i)] = {n_i} [E_i - E_r] \cos(\theta_t)\end{equation*}$

(20) $\begin{equation*}n_t E_i \cos(\theta_i) + n_t E_r \cos(\theta_i) = n_i E_i \cos(\theta_t) - n_i E_r \cos(\theta_t)\end{equation*}$

(21) $\begin{equation*} n_t E_i \cos(\theta_i) - n_i E_i \cos(\theta_t) = -n_t E_r \cos(\theta_i) - n_i E_r \cos(\theta_t) \end{equation*}$

(22) $\begin{equation*}E_i [n_t \cos(\theta_i) - n_i \cos(\theta_t)] = -E_r [n_t \cos(\theta_i) + n_i \cos(\theta_t)] \end{equation*}$

(23) $\begin{equation*}E_i [ n_i \cos(\theta_t) - n_t \cos(\theta_i)] = E_r [n_t \cos(\theta_i) + n_i \cos(\theta_t)] \end{equation*}$

(24) $\begin{equation*}r_p = \frac{E_r}{E_i} = \frac{ n_i \cos(\theta_t) - n_t \cos(\theta_i)}{n_t \cos(\theta_i) + n_i \cos(\theta_t)}\end{equation*}$

Now, for reflection coefficient t, from eq-17

$n_i E_i - n_t E_t = n_i E_r$

$E_i -\frac{n_t}{n_i} E_t = E_r$

Put this value in eq-15

(25) $\begin{equation*}E_i \cos(\theta_i) + [ E_i -\frac{n_t}{n_i} E_t] \cos(\theta_i) = E_t \cos(\theta_t)\end{equation*}$

(26) $\begin{equation*}E_i \cos(\theta_i) + E_i \cos(\theta_i) - \frac{n_t}{n_i} E_t \cos(\theta_i) = E_t \cos(\theta_t) \end{equation*}$

(27) $\begin{equation*}2 E_i \cos(\theta_i) = \frac{n_t}{n_i} E_t \cos(\theta_i) + E_t \cos(\theta_t) \end{equation*}$

(28) $\begin{equation*}2 E_i n_i \cos(\theta_i) = n_t E_t \cos(\theta_i) + {n_i} E_t \cos(\theta_t) \end{equation*}$

(29) $\begin{equation*}2 E_i n_i \cos(\theta_i) = E_t [n_t \cos(\theta_i) + {n_i} \cos(\theta_t)] \end{equation*}$

(30) $\begin{equation*} t_p = \frac{E_t}{E_i} = \frac{2 n_i \cos(\theta_i)}{ n_t \cos(\theta_i) + {n_i} \cos(\theta_t)} \end{equation*}$

Let’s summarized all four Fresnel’s equations,

$r_s = \frac{n_i \cos(\theta_i) - n_t \cos(\theta_t)}{n_t \cos(\theta_t) + n_i \cos(\theta_i)}$

$t_s = \frac{2 n_i \cos(\theta_i)}{ n_i \cos(\theta_i) + n_t \cos(\theta_t)}$

$r_p = \frac{ n_i \cos(\theta_t) - n_t \cos(\theta_i)}{n_t \cos(\theta_i) + n_i \cos(\theta_t)}$

$t_p = \frac{2 n_i \cos(\theta_i)}{ n_t \cos(\theta_i) + {n_i} \cos(\theta_t)}$