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Principles of Electromagnetism and Optics

Geometric Optics: Reflection and Refraction

Physics I 251 words Free to read

A straw in a glass of water looks broken because your brain insists light travels in straight lines — it traces the bent rays backwards and hallucinates the straw where they seem to come from. All of geometric optics is this one game: follow rays that bend at surfaces, then ask where the brain would put the image.

When light encounters a boundary between media, it can be reflected and refracted.

Law of reflection:

θi=θr\theta_i = \theta_r

Snell's law of refraction:

n1sinθ1=n2sinθ2n_1\sin\theta_1 = n_2\sin\theta_2

where n=c/vn = c/v is the refractive index of the medium.

Total internal reflection occurs when light travels from a denser medium (n1>n2n_1 > n_2) and:

θ1>θc=arcsin(n2n1)\theta_1 > \theta_c = \arcsin\left(\frac{n_2}{n_1}\right)

Thin lens equation:

1f=1do+1di\frac{1}{f} = \frac{1}{d_o} + \frac{1}{d_i}

Magnification:

m=didom = -\frac{d_i}{d_o}

Signdi>0d_i > 0di<0d_i < 0
ImageReal (opposite side)Virtual (same side)
m>0m > 0Upright
m<0m < 0Inverted

Mirror equation has the same form, with f=R/2f = R/2 for a spherical mirror of radius RR.

Tip: Always draw a ray diagram with at least two principal rays. The diagram catches sign errors and gives physical intuition about image location.
Common pitfall: Total internal reflection happens only when light tries to leave a slower (denser) medium for a faster one, beyond the critical angle. Going the other way — air into glass — light always enters, no matter the angle.

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Principles of Electromagnetism and Optics