💡

Board Exam Tips

  • →Write the New Cartesian sign convention at the start of every numerical: distances from the pole or optical centre, positive along the incident light, negative against it. Put signs in before substituting.
  • →The mirror equation 1/v + 1/u = 1/f and the lens formula 1/v − 1/u = 1/f differ by one sign. So do the magnifications: −v/u for a mirror, v/u for a lens.
  • →Derivations to prepare: mirror equation, refraction at a spherical surface, lens maker's formula, lenses in contact, and the prism formula at minimum deviation.
  • →For optical instruments, draw the labelled ray diagram (final image at infinity unless told otherwise) and then write the magnifying power.
  • →Power in dioptres needs f in metres: P = 1/f(m) = 100/f(cm).

📊 Diagram

📐 Formulas(18)

✏️ Solved Examples

1Solved Exampleeasy4 steps

An object is placed 25 cm in front of a concave mirror of focal length 15 cm. Find the position, nature and magnification of the image.

1

New Cartesian signs: the object and focus are in front of the mirror

2Solved Exampleboard5 steps

A double-convex lens is made of glass of refractive index 1.5 and both its faces have a radius of curvature of 20 cm. (a) Find its focal length and power in air. (b) An object is placed 30 cm from the lens. Find the position and magnification of the image.

1

Signs for a double-convex lens

3Solved Exampleboard3 steps

A prism of angle 60° gives a minimum deviation of 30°. Find (a) the refractive index of the prism material, (b) the angle of incidence at minimum deviation and (c) the critical angle for this material in air.

1

Prism formula at minimum deviation

4Solved ExampleHOTS6 steps

A compound microscope has an objective of focal length 2.0 cm and an eyepiece of focal length 5.0 cm. An object is placed 2.5 cm in front of the objective and the final image is formed at the least distance of distinct vision (25 cm). Find (a) the magnifying power and (b) the separation between the two lenses.

1

Objective: u_o = −2.5 cm, f_o = +2.0 cm

⚠️ Traps & Common Mistakes

⚠️Common Mistakes6
  • 1

    Taking u as positive for a real object, e.g. u = +25 cm

    ✓In the New Cartesian convention distances measured against the incident light are negative. A real object in front of a mirror or lens has u < 0.

  • 2

    Using the mirror magnification −v/u for a lens

    ✓Lens: m = v/u. Mirror: m = −v/u.

  • 3

    Mixing up the mirror and lens equations

    ✓Mirror: 1/v + 1/u = 1/f. Lens: 1/v − 1/u = 1/f.

  • 4

    Using f in centimetres in P = 1/f

    ✓Convert f to metres first: f = 25 cm gives P = 1/0.25 = 4 D. Equivalently P = 100/f with f in cm.

  • 5

    Stating only one condition for total internal reflection

    ✓Both are needed: light must go from the denser to the rarer medium, and the angle of incidence must exceed the critical angle.

  • 6

    Applying D = (n − 1)A to a 60° prism

    ✓That is the thin-prism approximation. For a large prism angle use n = sin((A + D_m)/2)/sin(A/2).

🎯 Practice Yourself

🎯Practice Yourself6 questions
  1. Q1

    A concave mirror has a radius of curvature of 30 cm. What is its focal length, with sign?

  2. Q2

    Find the power of a concave lens of focal length 25 cm.

  3. Q3

    Lenses of power +10 D and −4 D are placed in contact. Find the power and focal length of the combination.

  4. Q4

    Find the critical angle for a glass–air interface if the refractive index of glass is 1.5.

  5. Q5

    An astronomical telescope has an objective of focal length 150 cm and an eyepiece of focal length 5.0 cm. Find its magnifying power and tube length in normal adjustment.

  6. Q6

    A thin prism of angle 5° is made of glass of refractive index 1.6. Find the deviation it produces.

📝 Notes

Ray Optics and Optical Instruments

Almost every numerical in this chapter is one formula plus careful signs. Get the sign convention right and the rest is arithmetic.

Sign convention first

In the New Cartesian convention, measure every distance from the pole (mirror) or optical centre (lens). Distances in the direction of the incident light are positive; distances against it are negative; heights above the axis are positive. So a real object always has u<0u < 0, a concave mirror has f<0f < 0 and a convex lens has f>0f > 0.

Mirrors and lenses side by side

  • Mirror: 1v+1u=1f\dfrac{1}{v} + \dfrac{1}{u} = \dfrac{1}{f} and m=−vum = -\dfrac{v}{u}.
  • Lens: 1v−1u=1f\dfrac{1}{v} - \dfrac{1}{u} = \dfrac{1}{f} and m=vum = \dfrac{v}{u}.

In both cases a negative mm means a real, inverted image.

Refraction, TIR and the prism

Snell's law leads to the critical angle sin⁡ic=1/n\sin i_c = 1/n and, applied to a curved surface, to n2v−n1u=n2−n1R\dfrac{n_2}{v} - \dfrac{n_1}{u} = \dfrac{n_2 - n_1}{R}. Using that relation twice gives the lens maker's formula. For a prism, combine r1+r2=Ar_1 + r_2 = A and A+δ=i+eA + \delta = i + e; at minimum deviation the ray passes symmetrically, which gives n=sin⁡A+Dm2/sin⁡A2n = \sin\frac{A+D_m}{2} / \sin\frac{A}{2}.

Optical instruments

  • Simple microscope: m=1+D/fm = 1 + D/f (image at near point), D/fD/f (image at infinity).
  • Compound microscope: m≈(L/fo)(D/fe)m \approx (L/f_o)(D/f_e) — both focal lengths small.
  • Telescope: m=fo/fem = f_o/f_e, tube length fo+fef_o + f_e — large fof_o, small fef_e.

Reflecting telescopes use a concave mirror as the objective: there is no chromatic aberration, a parabolic mirror removes spherical aberration, and a large mirror is easier to support than a large lens.

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