Online Test — Optics
20 Questions • 15 min • Chapter MCQ
15:00
Question 1 of 20
The focal length of a concave mirror of radius of curvature $30\,\text{cm}$ is:
$30\,\text{cm}$
$15\,\text{cm}$
$60\,\text{cm}$
$7.5\,\text{cm}$
Explanation: $f = R/2 = 30/2 = 15\,\text{cm}$.
Question 2 of 20
A convex mirror forms an image that is always:
real and inverted
real and magnified
inverted and magnified
virtual, erect, diminished
Explanation: A convex mirror gives a virtual, erect, diminished image for all real objects.
Question 3 of 20
Magnification of a mirror is given by:
$m = v/u$
$m = -v/u$
$m = u/v$
$m = uv$
Explanation: For mirrors $m = -v/u = h\u2032/h$.
Question 4 of 20
Under the sign convention, distances measured against the incident light are taken as:
positive
zero
imaginary
negative
Explanation: Incident light travels left to right (positive); the opposite direction is negative.
Question 5 of 20
When the object is at the centre of curvature of a concave mirror, $m$ equals:
$+1$
$-1$
$+2$
$-2$
Explanation: Image at $C$, same size and inverted, so $m = -1$.
Question 6 of 20
Light bends away from the normal when entering a:
denser medium
medium of same index
vacuum
rarer medium
Explanation: Speed increases in a rarer medium, so the ray bends away from the normal.
Question 7 of 20
The critical angle for a medium of refractive index $2$ (with air) is:
$30^\circ$
$45^\circ$
$60^\circ$
$90^\circ$
Explanation: $\sin i_c = 1/2 \Rightarrow i_c = 30^\circ$.
Question 8 of 20
The power of a lens of focal length $25\,\text{cm}$ is:
$+2\,\text{D}$
$+0.25\,\text{D}$
$+25\,\text{D}$
$+4\,\text{D}$
Explanation: $P = 1/0.25 = +4\,\text{D}$.
Question 9 of 20
For a biconvex lens the radii are taken as:
both positive
both negative
$R_1$ positive, $R_2$ negative
$R_1$ negative, $R_2$ positive
Explanation: In the lens maker\u2019s convention $R_1 > 0$ and $R_2 < 0$ for a biconvex lens.
Question 10 of 20
The lens formula is:
$\dfrac{1}{v}+\dfrac{1}{u}=\dfrac{1}{f}$
$\dfrac{1}{u}-\dfrac{1}{v}=\dfrac{1}{f}$
$v+u=f$
$\dfrac{1}{v}-\dfrac{1}{u}=\dfrac{1}{f}$
Explanation: For a thin lens $\dfrac{1}{v}-\dfrac{1}{u}=\dfrac{1}{f}$.
Question 11 of 20
At minimum deviation through a prism, the refracted ray inside the prism is:
parallel to the base
perpendicular to the base
along the base
undefined
Explanation: At $\delta_m$ the ray passes symmetrically, travelling parallel to the base.
Question 12 of 20
In an astronomical telescope, high magnification needs:
large $f_e$, small $f_o$
equal $f_o$ and $f_e$
large $f_o$, small $f_e$
zero $f_e$
Explanation: $M = f_o/f_e$, so a large objective and small eyepiece focal length maximise $M$.
Question 13 of 20
Huygens\u2019 principle is used to explain:
photoelectric effect
reflection and refraction of waves
radioactivity
thermionic emission
Explanation: The wavelet construction derives the laws of reflection and refraction.
Question 14 of 20
In Young\u2019s experiment, bright fringes occur where the path difference is:
$(n+\tfrac{1}{2})\lambda$
$\lambda/4$
$n\lambda$
zero only
Explanation: Constructive interference needs $\Delta = n\lambda$.
Question 15 of 20
Fringe width $\beta = \dfrac{\lambda D}{d}$. If $d$ is doubled, $\beta$ becomes:
doubled
halved
unchanged
four times
Explanation: $\beta \propto 1/d$, so doubling $d$ halves $\beta$.
Question 16 of 20
The central maximum in single-slit diffraction is:
twice as wide as side maxima
equal in width to side maxima
narrower than side maxima
dark
Explanation: The central maximum spans between the first minima on each side, twice the width of the side maxima.
Question 17 of 20
Malus\u2019 law gives the intensity through an analyser as:
$I_0\sin\theta$
$I_0\cos^2\theta$
$I_0\sin^2\theta$
$I_0\cos\theta$
Explanation: $I = I_0\cos^2\theta$, where $\theta$ is the angle between polariser and analyser axes.
Question 18 of 20
Unpolarised light of intensity $I_0$ through one Polaroid emerges with intensity:
$I_0/2$
$I_0$
$I_0/4$
zero
Explanation: Averaging $\cos^2\theta$ over all angles gives $1/2$.
Question 19 of 20
An object at the focus of a concave mirror forms its image at:
the focus
the pole
infinity
the centre of curvature
Explanation: Rays after reflection become parallel, so the image forms at infinity.
Question 20 of 20
Total internal reflection is used in:
optical fibres
plane mirrors
concave lenses
photographic film
Explanation: Optical fibres guide light by repeated total internal reflection.