Mirror Formula
Mirror formula
v1+u1=f1
Tip: Write u, v, f WITH signs before substituting.
Lens Formula
Lens formula
v1−u1=f1
Tip: The only change from the mirror formula is the minus sign; magnification differs too (mirror m = −v/u, lens m = v/u).
Magnification of Mirrors and Lenses
Magnification
mirror m=−uv · lens m=uv
Tip: Negative m means real and inverted, positive m virtual and erect.
Refractive index
n=vc=sinrsini
Tip: Absolute refractive index n ≥ 1; higher n means slower light.
Power of a Lens (Dioptre)
Power of lens
P=f(m)1 (dioptre, D) · lenses in contact: P=P1+P2+…
Tip: f in METRES; +D convex, −D concave.
Mirror relation
R=2f
Tip: For a spherical mirror of small aperture only.
New Cartesian Sign Convention
Rules and signs at a glance
(i) The object is always placed to the left of the mirror or lens, so light falls on it from the left.
(ii) All distances parallel to the principal axis are measured from the pole of the mirror (or the optical centre of the lens).
(iii) Distances to the right of the origin (along +x) are positive; distances to the left (along −x) are negative.
(iv) Distances above the principal axis (along +y) are positive.
(v) Distances below the principal axis (along −y) are negative.
Signs at a glance. Object distance u is always negative.
Mirror: f is negative for a concave mirror and positive for a convex mirror; v is negative for a real image and positive for a virtual image; m is negative for a real image and positive for a virtual image.
Lens: f is positive for a convex lens and negative for a concave lens; v is positive for a real image and negative for a virtual image; m is negative for a real (inverted) image and positive for a virtual (erect) image.
Image Formation by a Concave Mirror (Table)
Position of object → position, size and nature of image
At infinity → at the focus F; highly diminished, point-sized; real and inverted
Beyond C → between F and C; diminished; real and inverted
At C → at C; same size; real and inverted
Between C and F → beyond C; enlarged; real and inverted
At F → at infinity; image would not be formed
Between P and F → behind the mirror; enlarged; virtual and erect
Image Formation by a Convex Mirror (Table)
Position of object → position, size and nature of image
At infinity → at the focus F, behind the mirror; highly diminished, point-sized; virtual and erect
Between infinity and the pole P → between P and F, behind the mirror; diminished; virtual and erect
Image Formation by a Convex Lens (Table)
Position of object → position, size and nature of image
At infinity → at focus F₂; highly diminished, point-sized; real and inverted
Beyond 2F₁ → between F₂ and 2F₂; diminished; real and inverted
At 2F₁ → at 2F₂; same size; real and inverted
Between F₁ and 2F₁ → beyond 2F₂; enlarged; real and inverted
At focus F₁ → at infinity; image would not be formed
Between focus F₁ and optical centre O → on the same side of the lens as the object; enlarged; virtual and erect
Image Formation by a Concave Lens (Table)
Position of object → position, size and nature of image
At infinity → at focus F₁; highly diminished, point-sized; virtual and erect
Between infinity and optical centre O → between F₁ and O; diminished; virtual and erect
A concave lens always gives a virtual, erect and diminished image, whatever the position of the object.
Laws of Refraction (Snell's Law)
(i) The incident ray, the refracted ray and the normal to the interface at the point of incidence all lie in the same plane. (ii) For light of a given colour and a given pair of media, sinrsini=constant (Snell's law). Going from an optically rarer to an optically denser medium, light slows down and bends towards the normal; going from denser to rarer, it speeds up and bends away from the normal.
Laws of Reflection
(i) The angle of incidence equals the angle of reflection. (ii) The incident ray, the reflected ray and the normal at the point of incidence all lie in the same plane. The image formed by a plane mirror is virtual, erect and the same size as the object.
Refraction through a Rectangular Glass Slab
For a rectangular glass slab the emergent ray is parallel to the incident ray, but it is displaced sideways (lateral displacement).