As per analysis for previous years, it has been observed that students preparing for NEET find Physics out of all the sections to be complex to handle and the majority of them are not able to comprehend the reason behind it. This problem arises especially because these aspirants appearing for the examination are more inclined to have a keen interest in Biology due to their medical background.
Furthermore, sections such as Physics are dominantly based on theories, laws, numerical in comparison to a section of Biology which is more of fact-based, life sciences, and includes substantial explanations. By using the table given below, you easily and directly access to the topics and respective links of MCQs. Moreover, to make learning smooth and efficient, all the questions come with their supportive solutions to make utilization of time even more productive. Students will be covered for all their studies as the topics are available from basics to even the most advanced.
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Q1. A double convex lens of focal length 20 𝑐𝑚 is made of glass of refractive index 3/2. When placed completely in water ( 𝑎𝜇𝜔 = 4/3), its focal length will be
Solution
𝑓water = 4 × 𝑓air , air lens is made up of glass
𝑓water = 4 × 𝑓air , air lens is made up of glass
Q2. To a fish under water, viewing obliquely a fisherman standing on the bank of the lake, the man looks
Q3. The numerical aperture for a human eye is of the order of
Solution
0.001
0.001
Q4. Five 𝑙𝑢𝑚𝑒𝑛/𝑤𝑎𝑡𝑡 is the luminous efficiency of a lamp and its luminous intensity is 35 𝑐𝑎𝑛𝑑𝑒𝑙𝑎. The power of the lamp is
Solution
Efficiency of light source 𝜂 = 𝜙/𝑃 …(i) and 𝐿 = 𝜙/4𝜋 …(ii) From equation (i) and (ii) ⇒ 𝑃 = 4𝜋𝐿/𝜂 = (4𝜋 × 35) /5 ≈ 88 𝑊
Efficiency of light source 𝜂 = 𝜙/𝑃 …(i) and 𝐿 = 𝜙/4𝜋 …(ii) From equation (i) and (ii) ⇒ 𝑃 = 4𝜋𝐿/𝜂 = (4𝜋 × 35) /5 ≈ 88 𝑊
Q5. If the speed of light in vacuum is 𝐶 𝑚/𝑠𝑒𝑐, then the velocity of light in a medium of refractive index 1.5
Solution
𝜇 = 𝐶/𝐶𝑚 ⇒ 𝐶𝑚 = 𝐶/1.5 .
𝜇 = 𝐶/𝐶𝑚 ⇒ 𝐶𝑚 = 𝐶/1.5 .
Q6. When sunlight is scattered by minute particles of atmosphere, the intensity of light scattered away is proportional to
Solution
(frequency of light)4
(frequency of light)4
Q7. A ray of light is incident at the glass-water interface at an angle 𝑖it emerges finally parallel to the surface of water, then the value of μgwould be
Solution
For glass-water interface gμw = sin𝑖/sin𝑟
For glass-water interface gμw = sin𝑖/sin𝑟
For water air interface wμ𝑎 =
sin𝑟/sin90°
⇒ gμw × wμ𝑎 =
sin𝑖/sin𝑟
×
sin𝑟/sin90°
= sin𝑖
or
μw/μg
×
μ𝑎/μw
= sin𝑖
⇒ μg=
1/sin𝑖
Q8. . The wavelength of light in air and some other medium are respectively 𝜆𝑎 and 𝜆𝑚. The refractive index of medium is
Solution
𝜇𝑚 = 𝑐/𝑣 = 𝑛𝜆𝑎/𝑛𝜆𝑚 = 𝜆𝑎/𝜆𝑚
𝜇𝑚 = 𝑐/𝑣 = 𝑛𝜆𝑎/𝑛𝜆𝑚 = 𝜆𝑎/𝜆𝑚
Q9. The plane face of a planoconvex lens is silvered. If μ be the refractive index and 𝑅, the radius of curvature of curved surface, then the system will behave like a concave mirror of radius of curvature
Solution
When an object is placed in front of such a lens, the rays are first of all refracted from the convex surface and again refracted from convex surface. Let 𝑓₁,𝑓m be focal lengths of convex surface and mirror (plane polished surface) respectively, then effective focal length is
When an object is placed in front of such a lens, the rays are first of all refracted from the convex surface and again refracted from convex surface. Let 𝑓₁,𝑓m be focal lengths of convex surface and mirror (plane polished surface) respectively, then effective focal length is
1 𝐹
=
1/𝑓₁
+
1/𝑓𝑚
+
1/𝑓₁
=
2/𝑓₁
+
1/𝑓𝑚
Since,
𝑓𝑚 =𝑅/2= ∞
∴1/𝐹=2/𝑓₁
From lens formula 1/𝑓₁ = (𝜇 − 1)( 1 𝑅 )
∴1/𝐹=2(𝜇 − 1)/ 𝑅
⟹ 𝐹 =
𝑅/2(𝜇 − 1)
𝑜𝑟 𝑅𝑒𝑞 = 2𝐹 =𝑅 /(𝜇 − 1)
Q10. The slab of a material of refractive index 2 shown in figure has curved surface 𝐴𝑃𝐵 of radius of curvature 10 𝑐𝑚 and a plane surface 𝐶𝐷. On the left of 𝐴𝑃𝐵 is air and on the right of 𝐶𝐷 is water with refractive indices as given in figure. An object 𝑂 is placed at a distance of 15 𝑐𝑚 from pole 𝑃 as shown. The distance of the final image of 𝑂 from 𝑃, as viewed from the left is
Solution
In case of refraction from a curved surface, we have
In case of refraction from a curved surface, we have
𝑖.𝑒., the curved surface will form virtual image 𝐼 at distance of 30 𝑐𝑚 from 𝑃. Since the image is virtual there will be no refraction at the plane surface 𝐶𝐷 (as the rays are not actually passing through the boundary), the distance of final image 𝐼 from 𝑃 will remain 30 𝑐𝑚