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Engineering Physics B.E. First Semester / 20 Practice Questions PDF

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Summary

This document provides practice questions and solutions related to Engineering Physics, focusing on the theoretical calculation of electron wavelength, the Compton effect, de Broglie's wavelength, and solved numerical examples.

Full Transcript

## Engineering Physics B.E. First Semester / 20 ### Theoretical Calculation of λ By using de Broglie hypothesis, the wavelength of an electron can be calculated as: $λ_{theoretical} = \frac{12.27}{√V}= \frac{12.27}{√54} =1.67 Å$ The agreement between theoretical and experimental values obtained from...

## Engineering Physics B.E. First Semester / 20 ### Theoretical Calculation of λ By using de Broglie hypothesis, the wavelength of an electron can be calculated as: $λ_{theoretical} = \frac{12.27}{√V}= \frac{12.27}{√54} =1.67 Å$ The agreement between theoretical and experimental values obtained from different considerations is excellent and constitutes a convincing proof for the wave characteristics of electron and hence the de Broglie hypothesis. ### 1.6 List of Formulae * Compton shift in terms of modified and unmodified component: $Δλ = λ' - λ$ * Compton shift in terms scattering angle: $Δλ = \frac{h}{m_0c} (1- cosφ)$ * Modified wavelength: $λ' = λ + \frac{h}{m_0c} (1-cosφ) $ * Unmodified wavelength: $λ = λ' - \frac{h}{m_0c} (1- cosφ) $ * Energy of recoiled electron: $E = \frac{hcΔλ}{λλ'}$ * Velocity of recoil electron: $v = √\frac{2E}{m}$ * de Broglie wavelength in terms of velocity/ momentum: $λ = \frac{h}{mv} = \frac{h}{p}$ * de Broglie wavelength in terms of kinetic energy: $λ = \frac{h}{√2mE}$ * de Broglie wavelength in terms of accelerating potential: $λ = \frac{h}{√2meV}$ * de-Broglie wavelength of an electron: $λ = \frac{12.27}{√V} * 10^{-10}$ * Diffraction equation (Bragg's law): $2d sin θ= ηλ $ ## Engineering Physics B.B. First Semester /21 ### 1.7 Solved Numerical 1. X-rays of wavelength 0.5 A° are scattered by free electrons in a block of carbon through 90°. Find the kinetic energy and velocity of recoiled electrons. Solution: λ = 0.5 A°, φ = 90°, K.E. = ?, v =? $λ' = λ + \frac{h}{m_0c}(1-cosφ) $ $λ' = 0.5 + 0.02427 (1 - cos 90) = 0.52427 A°$ $Δλ = λ' - λ = 0.02427 A°$ $E = \frac{hcΔλ}{λλ'} $ $E = \frac{6.626×10^{-34}×3×10^8×0.02427×10^{-10}}{0.5×10^{-10} ×0.52427×10^{-10}} = 1.84×10^{-16} J$ $V = √\frac{2×K.E}{m} = √\frac {2×1.84×10^{-16}}{9.1×10^{-31}} = 2×10^7 m/sec.$ 2. Calculate the de Broglie wavelength of the orbital electron of hydrogen atom given that its energy is 13.6 eV. Solution: E = 13.6 eV, λ = ? $λ = \frac{h}{√2mE} = \frac{6.626×10^{-34}}{√2 × 9.1×10^{-31}×13.6×1.602×10^{-19}}=3.327×10^{-10}m = 3.327 A°$ 3. Calculate the de-Broglie wavelength associated with an alpha particle accelerated by a potential difference of 100V. Solution: V =100V, m = 6.68x10^-27kg, q = 2e= 2x1.6x10^-19C, λ = ? $λ = \frac{h}{√2mqV} = \frac{6.632×10^{-34}}{√2×6.68×10^{-27}×2×1.602×10^{-19}×100} = 1.014×10^{-13}m.$ 4. A bullet of mass 45 gms and an electron both travel with velocity of 1000m/s. What wavelength can be associated with them? What Inference can be drawn from this result? Solution: m=45 gms = 45x10^-3 Kg v = 1000m/s $λ_{bullet} = ? $, $λ_{electron} = ?$ $λ_{bullet} = \frac{h}{mv} = \frac{6.632×10^{-34}}{45×10^{-3}×1000}= 1.474×10^{-35} m = 1.474×10^{-25} Å$ $λ_{electron} = \frac{h}{mv} = \frac{6.632×10^{-34}}{9.1×10^{-31}×1000} = 7.2799×10^{-7} m = 7279.9×10^{-10} m = 7279.9 Å$ Inference: Since the wavelength of matter wave associated with the bullet is of the order of 10^-35m, the wave nature cannot be revealed. But, the wavelength of the matter wave associated with electron is large almost 10 times more than the size of the electron (10^-15m), hence the wave nature of electron is revealed in diffraction experiment. 5. A photon of energy 1MeV is scattered through 90º by a free electron. Calculate the change in energy of photon and electron after the interaction. Solution: E = 1 MeV = 1x10^6 eV = 1.602 X 10^-13 J φ = 90° E_{recoil}? $λ = \frac{hc}{E} = \frac{6.63×10^{-34}×3×10^8}{1.602×10^{-13}} = 12.41×10^{-13} m$ $λ' - λ = \frac{h}{m_0c}(1-cosφ)$ $λ' = λ + \frac{6.63×10^{-34}}{9.1×10^{-31}×3×10^8}(1-cos90°) $ $λ' = 3.66×10^{-12} m $ $E' = \frac{hc}{λ'} = \frac{6.63×10^{-34}×3×10^8}{3.66×10^{-12}} = 5.442×10^{-14} J$ Energy of recoil electron = E_{recoil} = E - E' = 1.057×10^-13 J 6. What would be the de-Broglie wavelength associated with (i) 2000 kg car having a constant speed of 25 m/s. (ii)80 kg scooter having a speed of 10m/s. Give your conclusion. Solution: For car: m=2000 Kg V=25 m/s For Scooter: m=80 kg V= 10m/s $λ_{car} = \frac{h}{mv} = \frac {6.632×10^{-34}}{2000×25}= 1.324×10^{-38} m$ $λ_{scooter} = \frac{h}{mv} =\frac {6.632×10^{-34}}{80×10}= 8.295×10^{-37} m$ Conclusion: Wavelength associated with car is less due to its larger mass. ## Engineering Physics B.E. First Semester /22 7. An x-ray photon of wavelength 0.5A is scattered through an angle 60º by a loosely bound electron. Calculate recoil energy and velocity of an electron. Solution: λ=0.5A, θ=60° $ \frac{h}{m_0c} = 0.024264 A°$ The energy of the recoil electrons should be equal to the difference in energies of the incident and scattered photons. Thus $E-E' = K.E.= hc(\frac{1}{λ} - \frac{1}{λ'}) = \frac{h}{m_0c} (\frac{1}{λ} - \frac{1}{λ'})$ $λ' = λ + \frac{h}{m_0c}(1 - cos θ)$ $λ = λ + (1 - cos θ) = 0.5 + 0.2426(1 - cos 60°) = 0.6213 A = 0.512 A $ $K.E = hc(\frac{1}{λ} - \frac{1}{λ'}) = 12400 (\frac{1}{λ} - \frac{1}{λ'}) = 12400 (1 - \frac{λ}{λ'})×1.602×10^{-19} J$ $K.E = 12400 (\frac{1}{0.5} - \frac{1}{0.6213} )×1.602×10^{-19} = 1.84×10^{-16} J$ $V = √\frac{2×K.E}{m} = √\frac{2×1.84×10^{-16}}{9.1×10^{-31}} = 2×10^7 m/s$ 8. An electron and a particle of mass 10 gm both are moving with velocity 300m/s. Calculate the wavelengths associated with them and interpret the results. Solution: m = 10gm, v = 300 m/s, λ = ?, λ' = ? $λ_{e} = \frac{h}{mv} = \frac{6.6260 ×10^{-34}}{10 × 10^{-3} × 300} = 2.2086 × 10^{-34} m = 2.2086 × 10^{-24} A°.$ $λ_{p} = \frac{h}{mv} = \frac{6.6260 ×10^{-34}}{9.1×10^{-31} × 300} = 2.4244 × 10^{-6} m$ Interpretation: Since the wavelength of the matter wave associated with the particle is very small of the order of 10^-24 A and therefore the wave nature of the particle is not revealed through the diffraction experiment. But the wavelength of matter wave associated with electron is large almost 10^5 times more than the size of the electron (10^-15m), hence the wave nature of electron is revealed in diffraction experiment. ## Engineering Physics B.E. First Semester / 23 9. Incident radiation of wavelength 1.087A is scattered from a scatterer at an angle of 30°. Calculate the wavelength of scattered photon and kinetic energy of recoil electron. Solution: λ =1.0872 A°, φ = 30°, λ' = ?, Κ.Ε. = ? $λ' = λ + \frac{h}{m_0c} (1 - cos φ) = 1.0872 + 0.02427(1 - cos 30°) = 1.09045 A.$ $E = \frac{hcΔλ}{λλ'} = \frac{6.626×10^{-34}×3×10^8×0.02427×10^{-10}}{1.0872×10^{-10} ×1.09045×10^{-10}} = 4.069×10^{-17} J.$ 10. Calculate the wavelength associated with a stone of mass 50gms moving with speed of 50m/s and an electron with kinetic energy of 100eV. Solution: m-50gms = 0.5 kg v = 50m/s K.E = 100eV $λ_{stone}= ?$, $λ_{e} = ?$ $λ_{stone} = \frac{h}{mv} = \frac{6.626×10^{-34}}{0.5×50}= 2.65×10^{-35} m$ $λ_{e}= \frac{h}{√2mE} = \frac {6.626×10^{-34}}{√2×9.1×10^{-31} ×1.602×10^{-19} ×100} = 1.224 A°$ 11. X-ray photon of wavelength 0.3A is scattered through an angle 40º by a loosely bound electron, find the energy of scattered photon. Solution: λ = 0.3A° φ = 40° E' = ? $λ' = λ + \frac{h}{m_0c} (1 - cos φ)$ $λ' = 0.3 + 0.02427(1 - cos 40) = 0.3056 Å = 0.3056 × 10^{-10} m $ $E' = \frac{hc}{λ'} = \frac{6.64×10^{-34} ×3×10^8}{0.3056×10^{-10}} = 6.5183 × 10^{-15} J$ ## Engineering Physics B.E. First Semester / 24 12. A bullet of mass 50 grams and an electron both travel with a velocity of 1000m/s. What wavelength can be associated with them? Solution: m₁ = 50 gms = 50 x 10^-3 kg v= 1000m/s m = 9.11 x10^-31 kg λ with bullet and electron = ? For bullet: $λ_b = \frac{h}{mv} = \frac{6.64×10^{-34}}{50 × 10^{-3} × 1000} = 0.1328 × 10^{-35} m$ For electron: $λ_e = \frac{h}{mv} = \frac{6.64×10^{-34}}{9.1 × 10^{-31} × 1000} = 7.288 × 10^{-7} m$ 13. X-ray photon of wavelength 1A are scattered from a carbon block in a direction 90°. Calculate the observed Compton shift. How much kinetic energy is imparted to the recoil electron? Solution: λ = 1A°, φ = 90°, Δλ = ?, Κ.Ε. = ? $Δλ = λ' - λ = \frac{h}{m_0c} (1 - cos φ) $ $λ' = λ + \frac{h}{m_0c} (1 - cos φ) $ $λ' = 1 + 0.02427(1 - cos90) = 1.02427 A°$ $E = \frac{hcΔλ}{λλ'} = \frac{6.626×10^{-34}×3×10^8×1.02427 × 10^{-10}}{1 × 10^{-10} × 1.02427 × 10^{-10}} = 1.9878 × 10^{-15} J$ 14. A bullet of mass 45 gm and an electron both travel with a velocity of 1200m/s. What wavelength can be associated with them? Why is the wave nature of bullet not revealed through diffraction effect? Solution: m = 45 gms = 45x10^-3 Kg v = 1200m/s $λ_b = ?$, $λ_e = ?$ $λ_{bullet} = \frac{h}{mv} = \frac{6.632×10^{-34}}{45×10^{-3}×1200} = 1.228 * 10^{-35} m = 1.228 * 10^{-25} A°$ $λ_{electron} = \frac{h}{mv} = \frac{6.632×10^{-34}}{9.1×10^{-31}×1200} = 6.07326×10^{-7} m = 6073.26×10^{-10}m= 6073.2A$ Inference: Since the wavelength of matter wave associated with the bullet is of the order of 10^-35m, therefore the wave nature cannot be revealed in diffraction experiment. ## Engineering Physics B.E. First Semester / 25 15. In Compton effect, a photon is scattered by a free electron at rest through an angle of 90°. What is the energy of scattered photon if the wavelength of incident photon is 12nm. Solution: $Δλ = \frac{h}{m_0c} (1 - cosφ) = 0.02426 (1-cos 90) $ $ = 0.02426 A = 0.2426 nm$ $λ' = λ + Δλ = 12.2426 nm $ $E' = \frac{hc}{λ'}= \frac{6.63 × 10^{-34} × 3 × 10^8}{12.2426 × 10^{-9}} = 1.62 × 10^{-17} J = 101.62 eV$. 16. Find the de-Broglie wavelength of: i) An electron accelerated through a potential difference of 144V. ii) 10gm object moving with a speed of 10m/s Solution: m=10gms = 0.1kg V=144V V=10m/s $λ_{object} = ?$, $λ_{e} = ?$ $λ_{object} = \frac{h}{mv} = \frac {6.626×10^{-34}}{10×10×10} = 6.63×10^{-33} m$ $λ_{e} = \frac{h}{√2meV} = \frac{6.626×10^{-34}}{√2×9.1×10^{-31} ×1.602×10^{-19} ×144} = 1.0225 A°$ 17. An X-ray photon of wavelength 0.3 Aº is scattered through an angle of 45º by a loosely bound electron. Find the wavelength of the scattered photon. Solution: λ = 0.3 A° φ = 45° λ' = ? $λ' = λ + \frac{h}{m_0c} (1 - cos φ)$ $λ' = 0.3 + \frac{6.626×10^{-34}}{9.1×10^{-31} *3 * 10^8}(1 - cos 45) = 0.3071 A° $ 18. A beam of X-rays are scattered by loosely bounded electrons at 45° from the direction of the beam. The wave length of the scattered X-rays is 0.22 A.What is the wavelength of incident X-rays. Solution: λ' = 0.22 A° λ = ? φ = 45° $λ = λ' - \frac{h}{m_0c} (1 - cos φ) $ $λ = 0.22 - \frac{6.626×10^{-34}}{ 9.1×10^{-31} * 3 * 10^8} (1 - cos 45) = 0.212 A $ ## Engineering Physics B.E. First Semester / 26 19. Calculate the wavelength of scattered radiation and velocity of recoil electron when wavelength of incident radiation is 1.0872A and angle of scattering is 30º. Solution: λ = 1.0872 A° φ = 30° λ' = ? v = ? $λ' = λ + \frac{h}{m_0c} (1 - cos φ) = 1.0872 + 0.02427(1 - cos 30) = 1.09045 A° $ $E = \frac{hcΔλ}{λλ'} = \frac{6.626×10^{-34}×3×10^8×0.02427×10^{-10}}{1.0872×10^{-10} ×1.09045×10^{-10}} = 4.069×10^{-17} J $ $v = √\frac{2×K.E.}{m}=√\frac{2×4.071×10^{-17}}{9.1×10^{-31}} = 9.45×10^6 m/s$ 20. X-rays of wavelength 4Aº are scattered from a block of carbon. The scattered x-rays are observed at an angle of 45º to the incident beam. Calculate the Compton shift and the fraction of energy lost by the photon in this collision. Solution: λ=4 A° φ = 45° λ' = ? Fraction of energy lost = ? $λ' = λ + \frac{h}{m_0c} (1 - cos φ) = 4 + 0.02427(1 - cos 45) = 4.00710 A°$ Fraction of energy lost = $\frac{E-E'}{E} = \frac{hc}{λ'} - \frac{hc}{λ} = \frac{hc}{λ} * \frac{Δλ}{λ'} $ $Δλ = λ' - λ = 4.00710 - 4 = 0.007104 A°$ $\frac{Δλ}{λ'} = \frac{0.00710}{4.00710} = 0.00177 $ Thus, the fraction of energy lost by the photon in this collision is 0.177 %. ##Engineering Physics B.E. First Semester / 27 21. Using de Broglie hypothesis calculate the wavelength associated with the stone of mass 50 gms moving with speed of 50 m/s and an electron with K.E. of 100 eV. Solution: m=50gms = 0.5 kg v= 50m/s K.E = 100eV $λ_{stone}= ?$, $λ_{e} = ?$ $λ_{stone} = \frac{h}{mv} = \frac{6.626×10^{-34}}{0.5×50}= 2.65×10^{-35} m$ $λ_{e}= \frac{h}{√2mE} = \frac {6.626×10^{-34}}{√2×9.1×10^{-31} ×1.602×10^{-19} ×100} = 1.224 A°$ 22. Calculate the de Broglie wavelength associated with an electron with energy 60 eV. Solution: E = 60 eV, λ = ? $λ_{e} = \frac{h}{√2mE} = \frac {6.626×10^{-34}}{√2×9.1×10^{-31} ×60×1.602×10^{-19}} = 1.5844 A°$ ## Engineering Physics B.E. First Semester / 28 23. Calculate de Broglie wavelength of an electron subjected to a potential difference of 1.5kV. Solution: V=1.5kV, λ = ? $λ_{e} = \frac{h}{√2meV} = \frac {6.626×10^{-34}}{√2×9.1×10^{-31} ×1.602×10^{-19} ×1.5×1000} = 0.317 A°$ 24. Electrons of energy 10 KeV are passed through a thin film of metal for which atomic spacing is 5.5x10^-11 m. What is the angle of deviation of the first order diffraction maxima? Solution: d=5.5x10 ^-11 m, E=10 KeV, θ₁ =? $λ = \frac{h}{√2mE} = \frac {6.626×10^{-34}}{√2×9.1×10^{-31} ×10^4×1.602×10^{-19}} = 1.22×10^{-11} m$ $θ₁ = sin^{-1} \frac{ηλ}{2d} = sin^{-1} \frac{1 × 1.22 × 10^{-11}}{2×5.5 × 10^{-11}} = 6.36 ° $ 25. Electrons of are accelerated from rest through a potential difference of 150 V. These electron waves are diffracted by a grating with a spacing of 2A°. (i) Calculate the de Broglie wavelength of the electron. (ii) At what angle measured from the main axis will the first order maximum be observed? Solution: V = 150V m = 9.1x10^-31 kg d = 2A° = 2x10^-10 m n = 1 λ = ? θ₁ = ? $λ = \frac{h}{√2meV} = \frac {6.626×10^{-34}}{√2×9.1×10^{-31} ×1.602×10^{-19} ×150} = 1.001 × 10^{-10} A°$ $θ₁ = sin^{-1} (\frac{ηλ}{2d}) = sin^{-1} (\frac{1 × 1.001 × 10^{-10}}{2×2 × 10^{-10}}) = 14.50°$ 26. Find the de Broglie wavelength of (i) an electron accelerated through a potential difference of 182 V and (ii)1 Kg object moving with speed of 1 m/sec. Solution: V = 182V, m=1 kg, v=1m/s $λ_{e} = \frac{12.27}{√V} = \frac{12.27}{√182} = 0.9094 A°$ $λ_{object} = \frac{h}{mv} = \frac {6.626×10^{-34}}{1×1} = 6.626 × 10^{-34} m$

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