Exhaustive Guide to Light: Reflection and Refraction

The Nature and Propagation of Light

  • Visibility of Objects: We perceive objects through the interaction of light. Dark rooms render things invisible; however, lighting a room reveals its contents.
  • Sunlight and Perception: During daylight hours, sunlight illuminates objects. An object reflects the light falling upon it, and when this reflected light is received by our eyes, it enables us to see.
  • Transparent Media: Visibility through transparent media occurs because light is successfully transmitted through them.
  • Optical Phenomena: Light is responsible for a variety of phenomena including:
    • Image formation by mirrors.
    • The twinkling of stars.
    • The beautiful colors of a rainbow.
    • The bending of light (refraction) by different media.
  • Straight-Line Propagation: Observations of common optical phenomena suggest that light travels in straight lines. A small source of light casting a sharp shadow of an opaque object is evidence of this straight-line path, referred to as a ray of light.
  • The Wave Nature and Diffraction: If an opaque object on the path of light becomes very small, light tends to bend around it rather than traveling in a straight line. This effect is known as diffraction. In these cases, the ray-optics treatment fails, and light is instead modeled as a wave.
  • Modern Quantum Theory: By the early 20th century, the wave theory was found inadequate for describing light interacting with matter, where light behaves like a stream of particles. The modern quantum theory of light reconciles these views, stating light is neither exclusively a 'wave' nor a 'particle', but possesses properties of both.

Reflection of Light and Plane Mirrors

  • Definition: Reflection occurs when a highly polished surface, such as a mirror, reflects most of the light falling upon it.
  • Laws of Reflection: These laws apply to all reflecting surfaces, including spherical ones:
    • (i) The angle of incidence (ii) is always equal to the angle of reflection (rr).
    • (ii) The incident ray, the normal to the mirror at the point of incidence, and the reflected ray all lie in the same plane.
  • Properties of Images Formed by Plane Mirrors:
    1. The image is always virtual and erect.
    2. The size of the image is equal to the size of the object.
    3. The image is located at the same distance behind the mirror as the object is in front of it.
    4. The image is laterally inverted (left appears as right and vice versa).

Geometry and Terminology of Spherical Mirrors

  • Spherical Mirror: A mirror whose reflecting surface is a part of a hollow sphere.
    • Concave Mirror: The reflecting surface is curved inwards (towards the centre of the sphere).
    • Convex Mirror: The reflecting surface is curved outwards.
  • Key Geometric Terms:
    • Pole (PP): The centre of the reflecting surface of a spherical mirror. It lies on the surface of the mirror.
    • Centre of Curvature (CC): The centre of the sphere of which the mirror's reflecting surface forms a part. It lies outside the reflecting surface.
      • For a concave mirror, CC lies in front of the mirror.
      • For a convex mirror, CC lies behind the mirror.
    • Radius of Curvature (RR): The radius of the sphere of which the reflecting surface forms a part. The distance PCPC is equal to the radius of curvature.
    • Principal Axis: An imaginary straight line passing through the pole and the centre of curvature. It is normal to the mirror at its pole.
    • Principal Focus (FF):
      • In a concave mirror, rays parallel to the principal axis meet/intersect at this point after reflection.
      • In a convex mirror, rays parallel to the principal axis appear to diverge from this point behind the mirror.
    • Focal Length (ff): The distance between the pole (PP) and the principal focus (FF).
    • Aperture: The diameter of the circular outline of the reflecting surface (indicated as distance MNMN).
  • Relationship between RR and ff: For mirrors with small apertures, the radius of curvature is twice the focal length:
    • R=2fR = 2f

Principles of Image Formation in Spherical Mirrors

  • Locating Images Using Rays: For clarity in ray diagrams, we choose any two of the following four rays:
    1. Parallel Ray: A ray parallel to the principal axis passes through the focus (FF) for a concave mirror or appears to diverge from FF for a convex mirror after reflection.
    2. Focus Ray: A ray passing through FF (concave) or directed toward FF (convex) emerges parallel to the principal axis after reflection.
    3. Centre of Curvature Ray: A ray passing through CC (concave) or directed toward CC (convex) is reflected back along the same path because it hits the surface normally (90 degrees).
    4. Oblique Ray: A ray incident obliquely to the pole (PP) is reflected obliquely such that the angle of incidence equals the angle of reflection with respect to the principal axis.

Image Formation by Concave Mirrors

Position of ObjectPosition of ImageSize of ImageNature of Image
At infinityAt the focus FFHighly diminished, point-sizedReal and inverted
Beyond CCBetween FF and CCDiminishedReal and inverted
At CCAt CCSame sizeReal and inverted
Between CC and FFBeyond CCEnlargedReal and inverted
At FFAt infinityHighly enlargedReal and inverted
Between PP and FFBehind the mirrorEnlargedVirtual and erect

Image Formation by Convex Mirrors

Position of ObjectPosition of ImageSize of ImageNature of Image
At infinityAt focus FF behind the mirrorHighly diminished, point-sizedVirtual and erect
Between infinity and pole PPBetween PP and FF behind mirrorDiminishedVirtual and erect

Practical Applications of Spherical Mirrors

  • Concave Mirror Uses:
    • Used in torches, search-lights, and vehicle headlights to produce powerful parallel beams of light.
    • Used as shaving mirrors to provide a magnified view of the face.
    • Dentists use them to see larger images of patients' teeth.
    • Used in solar furnaces to concentrate sunlight and generate intense heat.
  • Convex Mirror Uses:
    • Commonly used as rear-view (wing) mirrors in vehicles.
    • Advantage 1: They always produce an erect image.
    • Advantage 2: They have a wider field of view because they are curved outwards, allowing drivers to see more traffic than a plane mirror would.

New Cartesian Sign Convention for Reflection

  • The Pole (PP) is taken as the origin (0,0)(0,0).
  • The Principal Axis is taken as the xx-axis (X′XX'X).
  • Rules:
    1. The object is always placed to the left of the mirror.
    2. Distances measured in the direction of incident light (to the right of the pole) are positive.
    3. Distances measured opposite to the direction of incident light (to the left of the pole) are negative.
    4. Distances measured upward and perpendicular to the principal axis (+y-axis) are positive.
    5. Distances measured downward and perpendicular to the principal axis (-y-axis) are negative.

The Mirror Formula and Magnification

  • Mirror Formula: Defines the relationship between object distance (uu), image distance (vv), and focal length (ff):
    • 1v+1u=1f\frac{1}{v} + \frac{1}{u} = \frac{1}{f}
  • Magnification (mm): The ratio of the height of the image (h′h') to the height of the object (hh):
    • m=h′hm = \frac{h'}{h}
  • Relation to Distances: Magnification is also defined as the negative ratio of image distance to object distance:
    • m=−vum = -\frac{v}{u}
  • Sign Significance in Magnification:
    • If mm is negative, the image is real.
    • If mm is positive, the image is virtual.
    • Object height (hh) is usually positive. Image height (h′h') is positive for virtual (erect) images and negative for real (inverted) images.

Worked Examples: Reflection

  • Example 9.1 (Convex Mirror):

    • Given: R=+3.00 mR = +3.00\,m, u=−5.00 mu = -5.00\,m.
    • Calculation: f=R2=+1.50 mf = \frac{R}{2} = +1.50\,m.
    • Using 1v=1f−1u=11.50−1−5.00=11.50+15.00=6.507.50\frac{1}{v} = \frac{1}{f} - \frac{1}{u} = \frac{1}{1.50} - \frac{1}{-5.00} = \frac{1}{1.50} + \frac{1}{5.00} = \frac{6.50}{7.50}.
    • Result: v=+1.15 mv = +1.15\,m (behind mirror). m=−1.15−5.00=+0.23m = -\frac{1.15}{-5.00} = +0.23.
    • Nature: Virtual, erect, and smaller (factor of 0.23).
  • Example 9.2 (Concave Mirror):

    • Given: h=+4.0 cmh = +4.0\,cm, u=−25.0 cmu = -25.0\,cm, f=−15.0 cmf = -15.0\,cm.
    • Calculation: 1v=1−15.0−1−25.0=−5.0+3.075.0=−2.075.0\frac{1}{v} = \frac{1}{-15.0} - \frac{1}{-25.0} = \frac{-5.0 + 3.0}{75.0} = \frac{-2.0}{75.0}.
    • Result: v=−37.5 cmv = -37.5\,cm (in front of mirror). h′=−v×hu=−−37.5×4.0−25.0=−6.0 cmh' = -\frac{v \times h}{u} = -\frac{-37.5 \times 4.0}{-25.0} = -6.0\,cm.
    • Nature: Real, inverted, and enlarged.

Phenomena of Refraction and Daily Observations

  • Definition: Refraction is the change in the direction of propagation of light when it travels obliquely from one transparent medium to another. It is caused by the change in the speed of light in different media.
  • Common Observations:
    • The bottom of a water tank or pond appears to be raised.
    • Letters appear raised when viewed through a thick glass slab.
    • A pencil partially immersed in water appears displaced/bent at the interface.
    • A lemon in a glass of water looks larger than its actual size.
  • Cause of Apparent Displacement: Light reaching the eye from the portion of the object inside the second medium (like water) comes from a different direction than the portion in the first medium (like air).

Laws of Refraction and Snell's Law

  1. First Law: The incident ray, the refracted ray, and the normal to the interface at the point of incidence all lie in the same plane.
  2. Second Law (Snell’s Law): The ratio of the sine of the angle of incidence to the sine of the angle of refraction is a constant for light of a given color and for a given pair of media.
    • sin⁡(i)sin⁡(r)=constant\frac{\sin(i)}{\sin(r)} = \text{constant}
    • This constant is the refractive index of the second medium with respect to the first (n21n_{21}).

The Refractive Index and Optical Density

  • Speed of Light: Light travels fastest in a vacuum (3×108 m/s3 \times 10^8\,m/s). Speed decreases in denser media like water or glass.
  • Relative Refractive Index:
    • n21=Speed of light in medium 1 (v1)Speed of light in medium 2 (v2)n_{21} = \frac{\text{Speed of light in medium 1 } (v_1)}{\text{Speed of light in medium 2 } (v_2)}
  • Absolute Refractive Index (nmn_m): When medium 1 is vacuum or air:
    • nm=cvn_m = \frac{c}{v} (where cc is speed in air and vv is speed in medium).
  • Optical Density:
    • Optically Denser Medium: Medium with a higher refractive index; light travels slower here.
    • Optically Rarer Medium: Medium with a lower refractive index; light travels faster here.
    • Crucial Distinction: Optical density is not the same as mass density. For example, kerosene has a higher refractive index than water (making it optically denser), but it has a lower mass density.
  • Bending Behavior:
    • Rarer to Denser: Light slows down and bends towards the normal.
    • Denser to Rarer: Light speeds up and bends away from the normal.

Refractive Indices of Common Materials

  • Air: 1.00031.0003
  • Ice: 1.311.31
  • Water: 1.331.33
  • Kerosene: 1.441.44
  • Crown Glass: 1.521.52
  • Dense Flint Glass: 1.651.65
  • Ruby: 1.711.71
  • Diamond: 2.422.42 (Highest optical density listed)

Fundamental Concepts of Spherical Lenses

  • Lens: A transparent material bound by two surfaces, at least one of which is spherical.
  • Convex Lens (Double Convex): Thicker at the middle than at the edges. It converges light rays and is called a converging lens.
  • Concave Lens (Double Concave): Thicker at the edges than at the middle. It diverges light rays and is called a diverging lens.
  • Key Terms for Lenses:
    • Optical Centre (OO): The central point of the lens. Rays passing through OO suffer no deviation.
    • Centres of Curvature (C1,C2C_1, C_2): A lens has two spherical surfaces, thus two centres of curvature.
    • Principal Axis: Straight line passing through C1C_1 and C2C_2.
    • Aperture: The effective diameter of the circular outline of the lens.
    • Principal Focus (F1,F2F_1, F_2): Points where parallel rays converge (convex) or from which they appear to diverge (concave).
    • Focal Length (ff): Distance from the optical centre to the principal focus.

Image Formation by Spherical Lenses

Convex Lens Table:

Object PositionImage PositionRelative SizeNature
At infinityAt focus F2F_2Highly diminishedReal and inverted
Beyond 2F12F_1Between F2F_2 and 2F22F_2DiminishedReal and inverted
At 2F12F_1At 2F22F_2Same sizeReal and inverted
Between F1F_1 and 2F12F_1Beyond 2F22F_2EnlargedReal and inverted
At focus F1F_1At infinityInfinitely enlargedReal and inverted
Between F1F_1 and OOOn same side as objectEnlargedVirtual and erect

Concave Lens Table:

Object PositionImage PositionRelative SizeNature
At infinityAt focus F1F_1Highly diminishedVirtual and erect
Between infinity and OOBetween F1F_1 and OODiminishedVirtual and erect

Lens Formula, Magnification, and Power

  • Lens Formula: 1v−1u=1f\frac{1}{v} - \frac{1}{u} = \frac{1}{f}
  • Magnification (mm):
    • m=h′h=vum = \frac{h'}{h} = \frac{v}{u}
  • Power of a Lens (PP): The degree of convergence or divergence of light rays. Defined as the reciprocal of focal length:
    • P=1fP = \frac{1}{f} (where ff is in metres).
  • Unit of Power: Dioptre (DD). 1 D=1 m−11\,D = 1\,m^{-1}.
    • Power of Convex Lens is positive.
    • Power of Concave Lens is negative.
  • Combinations of Lenses: For lenses in contact, the total power is the algebraic sum of individual powers:
    • P=P1+P2+P3+…P = P_1 + P_2 + P_3 + \dots
    • Used by opticians to design corrective spectacles and by engineers for cameras and microscopes to improve magnification and sharpness.

Worked Examples: Refraction and Lenses

  • Example 9.3 (Concave Lens):

    • Given: f=−15 cmf = -15\,cm, v=−10 cmv = -10\,cm.
    • Calculation: 1u=1v−1f=1−10−1−15=−3+230=−130\frac{1}{u} = \frac{1}{v} - \frac{1}{f} = \frac{1}{-10} - \frac{1}{-15} = \frac{-3+2}{30} = -\frac{1}{30}.
    • Result: u=−30 cmu = -30\,cm. Magnification m=−10−30=+0.33m = \frac{-10}{-30} = +0.33.
  • Example 9.4 (Convex Lens):

    • Given: h=+2.0 cmh = +2.0\,cm, f=+10 cmf = +10\,cm, u=−15 cmu = -15\,cm.
    • Calculation: 1v=110+1−15=3−230=130\frac{1}{v} = \frac{1}{10} + \frac{1}{-15} = \frac{3-2}{30} = \frac{1}{30}.
    • Result: v=+30 cmv = +30\,cm. m=30−15=−2m = \frac{30}{-15} = -2. h′=m×h=−2×2.0=−4.0 cmh' = m \times h = -2 \times 2.0 = -4.0\,cm.

Questions and Discussion

  • Defining 1 Dioptre: It is the power of a lens with a focal length of exactly 1 metre.
  • Refractive Index Meaning: If the index of diamond is 2.42, it means light travels 2.42 times slower in diamond than in a vacuum.
  • Mirror Selection: Concave mirrors are used for shaving (enlarged image) and solar furnaces (concentration); Convex mirrors are used for traffic (wide view).
  • Refraction Check: When light goes from air to water, it bends towards the normal because water is optically denser than air.
  • Mirror/Lens Pairs: If both a mirror and a thin lens have a focal length of −15 cm-15\,cm, both are concave (by convention).