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Energy corresponding to threshed frequency of metal is \(6.2 \mathrm{eV}\). If stopping potential corresponding to radiation incident on surface is $5 \mathrm{~V}\(, incident radiation will be in the \)\ldots \ldots \ldots \ldots \ldots$ region. (A) X-ray (B) Ultraviolet (C) infrared (D) Visible

Short Answer

Expert verified
The incident radiation will be in the Ultraviolet region.

Step by step solution

01

Determine the equation relating the variables given

We will use the equation for the photoelectric effect to relate the stopping potential, the threshold frequency energy, and the energy of the incident radiation: \(E_{incident} = E_{threshold} + eV\), where \(E_{incident}\) = energy of incident radiation, \(E_{threshold}\) = energy corresponding to the threshold frequency of the metal, \(e\) = elementary charge (approximately \(1.6 × 10^{−19} \mathrm{C}\)), and \(V\) = stopping potential.
02

Calculate the energy of the incident radiation

We are given that: \(E_{threshold} = 6.2 \mathrm{eV}\) and \(V = 5 \mathrm{V}\). Using the equation in step 1, we can solve for the energy of the incident radiation: \(E_{incident} = 6.2 \mathrm{eV} + (1.6 × 10^{−19} \mathrm{C})(5 \mathrm{V})\) \(E_{incident} = 6.2 \mathrm{eV} + 8 × 10^{−19} \mathrm{J}\) To keep the same units, let's convert 6.2 eV to Joules: \(6.2 \mathrm{eV} = 6.2 × 1.6 × 10^{−19} \mathrm{J} = 9.92 × 10^{−19} \mathrm{J}\) Now we can find the energy of the incident radiation: \(E_{incident} = 9.92 × 10^{−19} \mathrm{J} + 8 × 10^{−19} \mathrm{J} = 17.92 × 10^{−19} \mathrm{J}\)
03

Determine the region of the incident radiation

Now that we have the energy of the incident radiation, we can use the following equation to find its frequency: \(E = h\nu\), where \(E\) = energy of the radiation, \(h\) = Planck's constant (approximately \(6.626 × 10^{−34} \mathrm{Js}\)), and \(\nu\) = frequency of the radiation. Solving for the frequency: \(\nu = \frac{E}{h} = \frac{17.92 × 10^{−19} \mathrm{J}}{6.626 × 10^{−34} \mathrm{Js}} \approx 2.7 × 10^{15} \mathrm{Hz}\) Next, we'll use the speed of light equation to find the wavelength of the radiation: \(c = \lambda\nu\), where \(c\) = speed of light (approximately \(3 × 10^8 \mathrm{m/s}\)), \(\lambda\) = wavelength of the radiation, and \(\nu\) = frequency of the radiation. Solving for the wavelength: \(\lambda = \frac{c}{\nu} = \frac{3 × 10^8 \mathrm{m/s}}{2.7 × 10^{15} \mathrm{Hz}} \approx 1.1 × 10^{−7}\mathrm{m}\) This value of the wavelength falls within the ultraviolet region (10 − 400 nm), so the correct answer is: (B) Ultraviolet

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Most popular questions from this chapter

Radius of a beam of radiation of wavelength \(5000 \AA\) is $10^{-3} \mathrm{~m}\(. Power of the beam is \)10^{-3} \mathrm{~W}$. This beam is normally incident on a metal of work function \(1.9 \mathrm{eV}\). The charge emitted by the metal per unit area in unit time is \(\ldots \ldots \ldots\) Assume that each incident photon emits one electron. $\left(\mathrm{h}=6.625 \times 10^{-34} \mathrm{~J} . \mathrm{s}\right)$ (A) \(1.282 \mathrm{C}\) (B) \(12.82 \mathrm{C}\) (C) \(128.2 \mathrm{C}\) (D) \(1282 \mathrm{C}\)

Matching type questions: (Match, Column-I and Column-II property) Column-I Column-II (I) Quantization of charge (P) Diffraction of light (II) Wave nature of light (Q) de Broglie hypothesis (III) Dual nature of matter (R) Photo-electric effect (IV) Particle nature of light (S) Millikan's drop experiment (A) $\mathrm{I}-\mathrm{P}, \mathrm{II}-\mathrm{Q}, \mathrm{III}-\mathrm{R}, \mathrm{IV}-\mathrm{S}$ (B) $\mathrm{I}-\mathrm{S}, \mathrm{II}-\mathrm{P}, \mathrm{III}-\mathrm{Q}, \mathrm{IV}-\mathrm{R}$ (C) $\mathrm{I}-\mathrm{Q}, \mathrm{II}-\mathrm{R}, \mathrm{III}-\mathrm{S}, \mathrm{IV}-\mathrm{P}$ (D) \(I-R . I I-S . I I I-P . I V-O\)

Frequency of incident light on body is \(\mathrm{f}\). Threshold frequency of body is \(f_{0}\). Maximum velocity of electron \(=\ldots \ldots \ldots\).. where \(m\) is mass of electron. (A) $\left[\left\\{2 \mathrm{~h}\left(\mathrm{f}-\mathrm{f}_{0}\right)\right\\} / \mathrm{m}\right]^{(1 / 2)}$ (B) $\left[\left\\{2 \mathrm{~h}\left(\mathrm{f}-\mathrm{f}_{0}\right)\right\\} / \mathrm{m}\right]$ (C) \([2 \mathrm{hf} / \mathrm{m}]^{(1 / 2)}\) (D) \(\mathrm{h}\left(\mathrm{f}-\mathrm{f}_{0}\right)\)

Direction Read the following question choose if: (a) Both Assertion and Reason are true and Reason is correct explanation of Assertion. (b) Both Assertion and Reason are true, but Reason is not correct explanation of Assertion. (c) Assertion is true but the Reason is false. (d) Both Assertion and Reason is false. Assertion: Photo-electric effect can take place only when frequency is greater than threshold frequency \(\left(f_{0}\right)\) Reason: Electron is Fermions and photon is boson. (A) a (B) \(b\) (C) \(\mathrm{c}\) (D) d

Photoelectric effect on surface is found for frequencies $5.5 \times 10^{8} \mathrm{MHz}\( and \)4.5 \times 10^{8} \mathrm{MHz}$ If ratio of maximum kinetic energies of emitted photo electrons is \(1: 5\), threshold frequency for metal surface is \(\ldots \ldots \ldots \ldots\) (A) \(7.55 \times 10^{8} \mathrm{MHz}\) (B) \(4.57 \times 10^{8} \mathrm{MHz}\) (C) \(9.35 \times 10^{8} \mathrm{MHz}\) (D) \(5.75 \times 10^{8} \mathrm{MHz}\)

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