Class 12 Dual Nature Of Radiation And Matter CBSE Questions & Answers
Class 12 · Dual Nature Of Radiation And Matter
This is Physics Class 12 Dual Nature Of Radiation and Matter CBSE Questions & Answers. There are 15 questions in this test with each question having around four answer choices.
Questions & Answers
1
If the energy of a photon corresponding to a wave length of 6000 \(\mathop A\limits^0 \) is 3.32 \( \times {\rm{ 1}}{0^{{\rm{19}}}}\) joule, the photon energy for a wavelength of 4000 \(\mathop A\limits^0 \) will be
- A4.98\( \times {\rm{ 1}}{0^{{\rm{19}}}}\) joulesCorrect
- B6.98\( \times {\rm{ 1}}{0^{{\rm{19}}}}\) joules
- C5.98\( \times {\rm{ 1}}{0^{{\rm{19}}}}\) joules
- D2.22 \( \times {\rm{ 1}}{0^{{\rm{19}}}}\) joules
2
The work function for aluminium surface is 4.2 eV. The cutoff wavelength for the photo electric effect for the surface is
- A3100 \(\mathop A\limits^0 \)
- B1500 \(\mathop A\limits^0 \)
- C2400 \(\mathop A\limits^0 \)
- D2955 \(\mathop A\limits^0 \)Correct
3
The work function of a photoelectric material is 3.32 eV. The threshold frequency will be equal to
- A8 \( \times {\rm{1}}{0^{{\rm{14}}}}\) HZCorrect
- B6 \( \times {\rm{1}}{0^{{\rm{14}}}}\) HZ
- C7 \( \times {\rm{1}}{0^{{\rm{14}}}}\) HZ
- D9 \( \times {\rm{1}}{0^{{\rm{14}}}}\) HZ
4
Light of wavelength 4000 \(\mathop A\limits^0 \) is incident on a metal plate whose work function is 2 eV. The maximum kinetic energy of the emitted photoelectrons would be
- A1.1eVCorrect
- B1.5eV
- C2.0eV
- D0.5eV
5
Given h = 6.6 \( \times {\rm{1}}{0^{ - {\rm{34}}}}\) joule sec, the momentum of each photon in a given radiation is 3.3 \( \times {\rm{1}}{0^{ - {\rm{29}}}}\) kg metre/sec. The frequency of radiation is
- A1.6 \( \times {\rm{1}}{0^{{\rm{13}}}}\) Hz
- B1.7 \( \times {\rm{1}}{0^{{\rm{13}}}}\) Hz
- C1.5 \( \times {\rm{1}}{0^{{\rm{13}}}}\) HzCorrect
- D1.8 \( \times {\rm{1}}{0^{{\rm{13}}}}\) Hz
6
In a Milikan’s oil drop apparatus an oil drop of radius 6 \( \times {\rm{1}}{0^{ - {\rm{5}}}}\) m and of density 0.85 \( \times {\rm{1}}{0^{ - {\rm{5}}}}\) kg/m3 is seen to fall freely (without any field). The velocity of drop, given viscosity of air to be 1.83\( \times {\rm{1}}{0^{ - {\rm{5}}}}\) \({\rm{N}} - {\rm{s}}/{{\rm{m}}^{\rm{2}}}\) and neglecting the effect of up thrust force due to air, is
- A35.45\( \times {\rm{1}}{0^{ - {\rm{6}}}}\) m/sec
- B34.45\( \times {\rm{1}}{0^{ - {\rm{6}}}}\) m/sec
- C33.45\( \times {\rm{1}}{0^{ - {\rm{6}}}}\) m/sec
- D36.45\( \times {\rm{1}}{0^{ - {\rm{6}}}}\) m/secCorrect
7
If the wavelength of light falling on a surface is increased from 3000 \(\mathop A\limits^0 \) to 3040 \(\mathop A\limits^0 \), then what will be the corresponding change in the stopping potential (given that hc = 12.4\( \times {\rm{1}}{0^{\rm{7}}}\) eVÅ)?
- A-6.5 \( \times {\rm{1}}{0^{ - {\rm{12}}}}\) V
- B-8.5 \( \times {\rm{1}}{0^{ - {\rm{12}}}}\) V
- C-5.5 \( \times {\rm{1}}{0^{ - {\rm{12}}}}\) VCorrect
- D-7.5 \( \times {\rm{1}}{0^{ - {\rm{12}}}}\) V
8
If the wavelength of light incident on photo-electric cell be reduced from 4000\(\mathop A\limits^0 \) to3600\(\mathop A\limits^0 \),then what will be the change in the cut off potential. {tex}\left( {{\rm{h }} = {\rm{ 6}}.{\rm{6 }} \times {\rm{1}}{0^{ - {\rm{34}}}}{\rm{J }}-{\rm{ s}},{\rm{ c }} = {\rm{ 3}}.0{\rm{ }} \times {\rm{1}}{0^{\rm{8}}}{\rm{m}}/{\rm{s}},{\rm{ e }} = {\rm{ 1}}.{\rm{6 }} \times {\rm{ 1}}{0^{ - {\rm{19}}}}{\rm{C}}} \right){tex}
- A0.30Volt
- B0.34VoltCorrect
- C0.42Volt
- D0.43Volt
9
If the voltage across the electrodes of a cathode ray tube is 500 volts then energy gained by the electrons is
- A8 \( \times {\rm{1}}{0^{ - {\rm{17}}}}\) JCorrect
- B7 \( \times {\rm{1}}{0^{ - {\rm{17}}}}\) J
- C9 \( \times {\rm{1}}{0^{ - {\rm{17}}}}\) J
- D6 \( \times {\rm{1}}{0^{ - {\rm{17}}}}\) J
10
If an electron is accelerated by 8.8\( \times {\rm{1}}{0^{{\rm{14}}}}{\rm{m}}/{{\rm{s}}^{\rm{2}}}\)then electric field required for acceleration is (given specific charge of the electron = 1.76\( \times {\rm{1}}{0^{{\rm{11}}}}{\rm{Ck}}{{\rm{g}}^{ - {\rm{1}}}}\))
- A56 V \({\rm{c}}{{\rm{m}}^{ - {\rm{1}}}}\)
- B50 V \({\rm{c}}{{\rm{m}}^{ - {\rm{1}}}}\)Correct
- C52 V \({\rm{c}}{{\rm{m}}^{ - {\rm{1}}}}\)
- D54 V \({\rm{c}}{{\rm{m}}^{ - {\rm{1}}}}\)
11
If a beam goes undeflected in Thomson’s experiment, then speed of the electron is (given E = 30 V \({\rm{c}}{{\rm{m}}^{ - {\rm{1}}}}\) and B = 6.06 T)
- A6.5 \( \times {\rm{1}}{0^{\rm{6}}}\) m/s
- B5 \( \times {\rm{1}}{0^{\rm{6}}}\) m/sCorrect
- C6 \( \times {\rm{1}}{0^{\rm{6}}}\) m/s
- D5.5 \( \times {\rm{1}}{0^{\rm{6}}}\) m/s
12
When an electron enters a magnetic field of 0.01 T with a speed of \({\rm{1}}{0^{\rm{7}}}{\rm{m }}{{\rm{s}}^{ - {\rm{1}}}}\) it describes a circle of radius 6 mm there. Then specific charge of the electron is given by
- A1.87 \( \times {\rm{1}}{0^{{\rm{11}}}}{\rm{Ck}}{{\rm{g}}^{ - {\rm{1}}}}\)
- B1.67 \( \times {\rm{1}}{0^{{\rm{11}}}}{\rm{Ck}}{{\rm{g}}^{ - {\rm{1}}}}\)Correct
- C1.57 \( \times {\rm{1}}{0^{{\rm{11}}}}{\rm{Ck}}{{\rm{g}}^{ - {\rm{1}}}}\)
- D1.77 \( \times {\rm{1}}{0^{{\rm{11}}}}{\rm{Ck}}{{\rm{g}}^{ - {\rm{1}}}}\)
13
1.If an electron moving with a speed of 2.5\( \times {\rm{1}}{0^{\rm{7}}}{\rm{m }}{{\rm{s}}^{ - {\rm{1}}}}\) is deflected by an electric field of 1.6 k V \({{\rm{m}}^{ - {\rm{1}}}}\)perpendicular to its circular path, then e/m for the electron will be (given radius of circlar path = 2.3 m)
- A1.7 \( \times {\rm{1}}{0^{{\rm{11}}}}{\rm{C k}}{{\rm{g}}^{ - {\rm{1}}}}\)Correct
- B1.9 \( \times {\rm{1}}{0^{{\rm{11}}}}{\rm{C k}}{{\rm{g}}^{ - {\rm{1}}}}\)
- C1.85 \( \times {\rm{1}}{0^{{\rm{11}}}}{\rm{C k}}{{\rm{g}}^{ - {\rm{1}}}}\)
- D1.8 \( \times {\rm{1}}{0^{{\rm{11}}}}{\rm{C k}}{{\rm{g}}^{ - {\rm{1}}}}\)
14
If an electron accelerated through a potential difference of 500 volt attains a speed of 1.33 \( \times {\rm{1}}{0^{\rm{7}}}{\rm{m }}{{\rm{s}}^{ - {\rm{1}}}}\) then specific charge of the electron should be
- A1.76 \( \times {\rm{1}}{0^{{\rm{11}}}}{\rm{C k}}{{\rm{g}}^{ - {\rm{1}}}}\)Correct
- B1.86 \( \times {\rm{1}}{0^{{\rm{11}}}}{\rm{C k}}{{\rm{g}}^{ - {\rm{1}}}}\)
- C1.96 \( \times {\rm{1}}{0^{{\rm{11}}}}{\rm{C k}}{{\rm{g}}^{ - {\rm{1}}}}\)
- D1.66 \( \times {\rm{1}}{0^{{\rm{11}}}}{\rm{C k}}{{\rm{g}}^{ - {\rm{1}}}}\)
15
If an electron accelerated from rest through a potential of 200 V acquires a speed of 84\( \times {\rm{1}}{0^{{\rm{16}}}}{\rm{m }}{{\rm{s}}^{ - {\rm{1}}}}\), then its e/m is
- A1.66 \( \times {\rm{1}}{0^{{\rm{11}}}}{\rm{C k}}{{\rm{g}}^{ - {\rm{1}}}}\)
- B1.76 \( \times {\rm{1}}{0^{{\rm{11}}}}{\rm{C k}}{{\rm{g}}^{ - {\rm{1}}}}\)Correct
- C1.96 \( \times {\rm{1}}{0^{{\rm{11}}}}{\rm{C k}}{{\rm{g}}^{ - {\rm{1}}}}\)
- D1.86 \( \times {\rm{1}}{0^{{\rm{11}}}}{\rm{C k}}{{\rm{g}}^{ - {\rm{1}}}}\)