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Optics — Class 11 MCQs with Answers

Class 11 CBSE Physics · Chapter 303

40 practice questions · 20 Easy · 20 Medium · Updated

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Practise the most important Class 11 CBSE Physics questions from Chapter 303, "Optics". You get 4 timed quizzes made from 40 NCERT-based MCQs, with answers and explanations. The questions are split into 20 Easy and 20 Medium. Warm up on the basics, then move on to the exam-level questions that top scorers in CBSE & Maharashtra HSC Board exams, JEE Main, MHT-CET, JEE Advanced and NEET UG get right.

To score well in "Optics", focus on numericals, derivations and applying concepts. Each MCQ here is timed and uses exam-style marking (+4 correct, −1 wrong, 0 skipped). This helps you stay accurate when time is short, just as real papers need. Every question has a short explanation, so a wrong answer becomes a quick lesson. It is the fastest way to fix gaps before a test.

Use this chapter for focused revision. Start with the Easy set to check your basics on Optics, then move to Medium to practise applying them. Your accuracy, streaks and XP save automatically. This chapter also adds to your overall Class 11 Physics mastery score. Try the 4 sample questions below: tap an option to see the answer and a worked explanation. Sign in free to start practising.

Optics — important questions & MCQs with answers (Class 11 Physics)

4 solved questions from this chapter's difficulty levels, each with its answer and explanation. Tap an option to check yourself.

0 of 4 answered

  1. Q1 of 4Easy

    Snell's law:

    Show answer

    Answer: n₁ sinθ₁ = n₂ sinθ₂

    Explanation: Refraction at interface.

  2. Q2 of 4Easy

    Young's experiment demonstrates:

    Show answer

    Answer: Interference of light

    Explanation: Two-slit interference pattern.

  3. Q3 of 4Medium

    Width of central maximum in single-slit diffraction (screen at D, slit a):

    Show answer

    Answer: 2λD/a

    Explanation: From first minima on either side.

  4. Q4 of 4Medium

    Total internal reflection occurs when:

    Show answer

    Answer: Light passes from denser to rarer beyond critical angle

    Explanation: Used in optical fibres.

Optics notes: key concepts (Class 11 Physics)

Light treated as rays: reflection at spherical mirrors with the mirror formula and sign convention, refraction and Snell's law, total internal reflection with its applications, refraction at a spherical surface leading to the lens maker's formula, lens power and combinations, the prism, and the microscope and telescope. Light treated as a wave: Huygens' principle and wavefronts, coherence and interference in Young's double-slit experiment with its fringe width, diffraction at a single slit and the width of the central maximum, how interference differs from diffraction, and polarisation with Malus's and Brewster's laws.

Laws of reflection
The angle of incidence equals the angle of reflection, and the incident ray, reflected ray and normal all lie in one plane.
Spherical mirrors
A concave mirror converges light and can form real or virtual images; a convex mirror always diverges and forms only virtual, diminished images.
A concave mirror with its reflecting surface facing left. The principal axis passes through the centre of curvature C, the principal focus F and the pole P. Two rays travelling parallel to the axis, one above and one below it, strike the mirror and are reflected so that they converge through the focus F, which lies midway between C and P. The focal length f is the distance FP and the radius of curvature R = CP = 2f.
Sign convention
Distances are measured from the pole, positive along the incident light and negative against it. Nearly every optics error traces back to a sign here.
Mirror formula and magnification
One relation links object distance, image distance and focal length, with magnification −v/u telling you the size and orientation of the image.
Refraction
The bending of light as it crosses into a medium of different optical density, caused entirely by the change in the SPEED of light.
Snell's law
The ratio of the sines of the angles of incidence and refraction is constant, equal to the ratio of refractive indices of the two media.
A ray of light passes from a medium of refractive index n₁ (above) into an optically denser medium of refractive index n₂ (below, shaded). At the point of incidence O a dashed normal is drawn perpendicular to the boundary. The incident ray makes the angle of incidence i with the normal; the refracted ray bends towards the normal, making a smaller angle of refraction r. Drawn for n₂/n₁ = 1.5. Snell's law: sin i / sin r = n₂ / n₁.
Refractive index
The ratio of the speed of light in vacuum to that in the medium. It is always greater than one and depends on the wavelength of light.
Total internal reflection
When light travels from a denser to a rarer medium beyond the critical angle, it is completely reflected — no light is refracted at all.
Rays from a point S inside glass, the denser medium, meet the boundary with air at increasing angles of incidence. The first ray, at a small angle, is refracted into the air, bending away from the normal. The second meets the boundary at the critical angle c (about 42° for glass of refractive index 1.5): its refracted ray just grazes along the surface. The third, at an angle greater than c, is not refracted at all but totally reflected back into the glass. Dashed normals are drawn at each point.
Critical angle
The angle of incidence in the denser medium for which the refracted ray just grazes the surface at 90°. Its sine equals the reciprocal of the refractive index.
Applications of TIR
Optical fibres, the sparkle of a diamond, mirages and the totally reflecting prisms in binoculars all rely on total internal reflection.
An optical fibre in section: a glass core of higher refractive index surrounded by a cladding of lower refractive index. Light entering one end strikes the core–cladding boundary at an angle of incidence i greater than the critical angle c, so it is totally reflected. It zig-zags along the core by repeated total internal reflection and emerges at the far end with almost no loss.
Refraction at a spherical surface
Relates object and image distances across a single curved boundary and is the step from which the lens maker's formula is derived.
A convex spherical surface separating a medium of refractive index n₁ on the left from a denser medium n₂ on the right (shaded). Its pole is P and its centre of curvature C lies in the denser medium, at distance R from P. A ray from a point object O on the principal axis meets the surface at M, where the dashed normal passes through C, and bends towards the normal to meet the axis at the real image I. The object distance u is PO, the image distance v is PI. They are related by n₂/v − n₁/u = (n₂ − n₁)/R.
Lens maker's formula
Gives the focal length from the refractive index and the two radii of curvature, showing how a lens's power depends on both shape and material.
Thin lens formula and magnification
Links object distance, image distance and focal length; the magnification v/u gives the image size and whether it is erect or inverted.
A convex lens with optical centre O, foci F₁ and F₂ and the points 2F₁ and 2F₂ on the principal axis. An object stands beyond 2F₁. A ray from its top parallel to the axis is refracted through F₂; a ray through O goes on undeviated. They meet between F₂ and 2F₂, forming a real, inverted, diminished image. The object distance u (negative), the image distance v (positive) and the focal length f are marked from O. They obey 1/v − 1/u = 1/f, and the magnification is m = v/u, negative here because the image is inverted.
Power of a lens
The reciprocal of focal length in metres, measured in dioptre. Converging lenses have positive power, diverging lenses negative.
Combination of lenses
For thin lenses in contact, powers simply add algebraically — the basis of correcting lenses and of achromatic doublets.
Optical instruments
A simple microscope magnifies with a single converging lens; a compound microscope and a telescope each use an objective and an eyepiece, but with very different focal-length choices.
Huygens' principle
Every point on a wavefront acts as a source of secondary wavelets, and the new wavefront is their common tangent. It explains reflection and refraction geometrically.
Huygens' construction. AB is a plane wavefront at one instant. Each point on it, shown as a dot, sends out a secondary wavelet: after a time t each wavelet is a hemisphere of radius vt, drawn as a blue arc ahead of AB. The new wavefront CD, in green, is the common tangent to all these wavelets, a plane parallel to AB at distance vt ahead of it. An arrow shows the direction of propagation, perpendicular to the wavefronts.
Wavefront
The locus of all points vibrating in the same phase. The direction of propagation is always perpendicular to the wavefront.
Types of wavefront
A point source gives spherical wavefronts, a line source cylindrical ones, and a source at effectively infinite distance gives plane wavefronts.
Two kinds of wavefront side by side. Left: a point source with wavefronts that are concentric spheres around it, drawn as green arcs, and rays spreading radially outwards. Right: a source at a very large distance gives plane wavefronts, drawn as parallel green straight lines, with parallel rays perpendicular to them. In both, the rays are perpendicular to the wavefronts.
Coherent sources
Two sources with a constant phase difference and identical frequency. Sustained interference is impossible without them, which is why two bulbs never interfere.
Interference of light
The superposition of coherent waves, producing alternating bright and dark fringes. Energy is redistributed, never created or destroyed.
Young's double slit experiment
The classic demonstration of the wave nature of light, producing equally spaced fringes of uniform brightness on a distant screen.
Young's double-slit arrangement. Light from a narrow slit S falls on two slits S₁ and S₂ a distance d apart, which act as coherent sources. A screen stands at distance D. Waves from S₁ and S₂ reach a point P at height y above the centre O of the screen. The path difference S₂P − S₁P is approximately yd/D. P is bright when it is a whole number of wavelengths nλ, and dark when it is an odd number of half-wavelengths. The strip beside the screen shows the equally spaced bright and dark fringes, with a bright fringe at O.
Conditions for bright and dark fringes
A bright fringe forms where the path difference is a whole number of wavelengths, a dark fringe where it is an odd number of half-wavelengths.
Fringe width
The spacing between consecutive bright fringes, λD/d. Widening the slit separation narrows the fringes; using a longer wavelength widens them.
Effect of immersing in a liquid
The wavelength shortens by a factor n inside the medium, so the whole fringe pattern contracts by the same factor.
Diffraction
The bending of light around obstacles or through narrow apertures, appreciable only when the aperture is comparable to the wavelength.
Single slit diffraction
Produces a broad central maximum flanked by much weaker secondary maxima, with minima where a sin θ equals a whole number of wavelengths.
Intensity I against angle θ for diffraction at a single slit of width a. A broad, bright central maximum is centred on θ = 0. The first minima, where the intensity falls to zero, are at θ = λ/a and θ = −λ/a, and further minima at ±2λ/a. Between the minima lie the secondary maxima, much weaker than the central one and half as wide. The curve is drawn from I = I₀(sin β/β)².
Width of the central maximum
Twice as wide as any secondary maximum and inversely proportional to slit width — narrowing the slit spreads the pattern out.
Interference versus diffraction
Interference fringes are equally spaced and equally bright and come from two sources; diffraction bands are unequal in width and intensity and come from one aperture.
Polarisation
The restriction of the electric field's vibration to a single plane, possible only because light is a TRANSVERSE wave. Sound can never be polarised.
Unpolarised light, whose electric field vibrates in all directions across the beam (shown by double arrows in several directions), falls on a polariser P₁ with a vertical transmission axis. It leaves plane polarised, vibrating in one plane only, with intensity I₀. It then meets an analyser P₂ whose transmission axis makes an angle θ with that of P₁. The light that emerges is polarised along P₂'s axis and its intensity is I₀cos²θ (Malus's law), shown by a shorter double arrow.
Malus's law
The intensity transmitted by an analyser varies as the square of the cosine of the angle between the transmission axes of polariser and analyser.
Brewster's law
At a particular angle of incidence the reflected light is completely plane polarised, and the tangent of that angle equals the refractive index.
Light falls on a glass surface of refractive index n at the Brewster angle i_B, measured from the dashed normal. The reflected ray leaves at the same angle i_B and the refracted ray makes a right angle with it (square mark). The incident light is unpolarised, marked with both dots (vibrations perpendicular to the page) and short ticks (vibrations in the page). The reflected light carries only dots: it is completely plane polarised. The refracted light is partly polarised. At this angle tan i_B = n; drawn for n = 1.5.
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Optics — FAQs

What are the key concepts in Class 11 Physics Optics?+

Light treated as rays: reflection at spherical mirrors with the mirror formula and sign convention, refraction and Snell's law, total internal reflection with its applications, refraction at a spherical surface leading to the lens maker's formula, lens power and combinations, the prism, and the microscope and telescope. Light treated as a wave: Huygens' principle and wavefronts, coherence and interference in Young's double-slit experiment with its fringe width, diffraction at a single slit and the width of the central maximum, how interference differs from diffraction, and polarisation with Malus's and Brewster's laws. Key ideas include Laws of reflection, Spherical mirrors, Sign convention, Mirror formula and magnification, Refraction, Snell's law.

What does Class 11 Physics Chapter 303 (Optics) cover on XamBaaz?+

It has 40 NCERT-based MCQs on "Optics": 20 Easy and 20 Medium. Together they make 4 timed quizzes, and you never get the same set twice. Every question has an instant explanation. They help you prepare for CBSE & Maharashtra HSC Board exams, JEE Main, MHT-CET, JEE Advanced and NEET UG.

Are these "Optics" questions free to practise?+

Yes. Sign in with Google to practise "Optics" free. Full unlimited access is ₹1,999/year. One year from the day you pay. You stay in Class 11 till 31 March; on 1 April your account moves up to Class 12 and the rest of your year carries over. No chapter is charged separately.

How should I revise "Optics" for the exam?+

Start with the Easy quiz to check your basics, then try Medium to practise applying them. There are 4 timed quizzes on this chapter, so you can come back for a fresh set instead of one you have seen. Read each explanation, retry the questions you miss, and track your accuracy until it stays high.

Are these "Optics" MCQs available with answers?+

Yes. 4 sample questions are on this page with answers: tap an option, or "Show answer", to see the correct option and a step-by-step explanation. Sign in free with Google to start practising, with instant scoring.

Is there negative marking in the "Optics" quizzes?+

Yes. The timed quizzes use exam-style marking: +4 for a right answer, −1 for a wrong one and 0 for a skip, the same negative marking as JEE Main, JEE Advanced and NEET UG. MHT-CET and CBSE board papers have no negative marking. Our mocks for those are scored their way.

What are the important questions from Optics (Class 11 Physics)?+

The questions that matter most test Laws of reflection, Spherical mirrors, Sign convention, Mirror formula and magnification, Refraction, Snell's law. This page shows 4 solved important MCQs with answers and explanations. Sign in to practise all 40 questions on the chapter as timed quizzes.

Is there an online quiz for Optics?+

Yes — Class 11 Physics Optics has timed online quizzes at Easy and Medium levels, with instant scoring and a worked explanation on every question. The first quiz on the chapter is free.

Are there question answers and extra questions for Optics (Class 11 Physics)?+

Yes. This page has 4 solved questions on Optics, each with the correct answer and a short explanation. Sign in to practise all 40 questions on the chapter as timed quizzes.

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