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Dual Nature of Radiation question

2010 · Shift 1 · Q82
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Dual Nature of Radiation question

2010 · Shift 1 · Q82

JEE AdvancedPhysicsDual Nature of RadiationNumerical+3 / −1
An α\alphaα-particle and a proton are accelerated from the rest by a potential difference of 100 V. After this, their de Broglie wavelengths are λα\lambda\alphaλα and λ\lambdaλ p, respectively. The ratio λpλα{{{\lambda _p}} \over {{\lambda _\alpha }}}λα​λp​​, to the nearest integer, is ‾\underline{\hspace{2cm}}​.
Numerical answer
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Correct answer: 3

Step-by-step Derivation

  1. Relating de Broglie Wavelength, Kinetic Energy, and Accelerating Potential The de Broglie wavelength (lambda\\\\lambdalambda) of a particle is given by the formula: λ=hp\lambda = \frac{h}{p}λ=ph​ where hhh is Planck's constant and ppp is the momentum of the particle.

    The kinetic energy (KKK) of a particle with mass mmm and momentum ppp is related by K=p22mK = \frac{p^2}{2m}K=2mp2​, which can be rearranged to give p=2mKp = \sqrt{2mK}p=2mK​.

    Substituting this expression for momentum into the de Broglie wavelength formula, we get: λ=h2mK\lambda = \frac{h}{\sqrt{2mK}}λ=2mK​h​

    When a particle with charge qqq is accelerated from rest through a potential difference VVV, it gains kinetic energy equal to K=qVK = qVK=qV. Substituting this into the wavelength equation gives: λ=h2mqV\lambda = \frac{h}{\sqrt{2mqV}}λ=2mqV​h​

  2. Properties of the Proton and Alpha-particle We need to identify the mass and charge for both particles.

    • Proton (p):
      • Mass: mpm_pmp​
      • Charge: qp=eq_p = eqp​=e (where eee is the elementary charge)
    • Alpha-particle (alpha\\\\alphaalpha): An alpha-particle is a helium nucleus (24He{}^4_2\text{He}24​He), which consists of 2 protons and 2 neutrons.
      • Mass: mα≈4mpm_\alpha \approx 4 m_pmα​≈4mp​
      • Charge: qα=2eq_\alpha = 2eqα​=2e
  3. Writing Expressions for Wavelengths Using the general formula from Step 1, we can write the de Broglie wavelengths for the proton (lambdap\\\\lambda_plambdap​) and the alpha-particle (lambdaα\\\\lambda_\alphalambdaα​). Both are accelerated by the same potential difference V=100V = 100V=100 V.

    • For the proton: λp=h2mpqpV=h2mpeV\lambda_p = \frac{h}{\sqrt{2m_p q_p V}} = \frac{h}{\sqrt{2m_p eV}}λp​=2mp​qp​V​h​=2mp​eV​h​

    • For the alpha-particle: λα=h2mαqαV=h2(4mp)(2e)V=h16mpeV\lambda_\alpha = \frac{h}{\sqrt{2m_\alpha q_\alpha V}} = \frac{h}{\sqrt{2(4m_p)(2e)V}} = \frac{h}{\sqrt{16m_p eV}}λα​=2mα​qα​V​h​=2(4mp​)(2e)V​h​=16mp​eV​h​

  4. Calculating the Ratio {{{\\\lambda _p}} \\over {{\\\\lambda _\\alpha }}} Now we can find the ratio of the two wavelengths: λpλα=h2mpeVh16mpeV\frac{\lambda_p}{\lambda_\alpha} = \frac{\frac{h}{\sqrt{2m_p eV}}}{\frac{h}{\sqrt{16m_p eV}}}λα​λp​​=16mp​eV​h​2mp​eV​h​​

    The constants hhh, mpm_pmp​, eee, and the potential difference VVV cancel out, simplifying the expression: λpλα=16mpeV2mpeV=162=8\frac{\lambda_p}{\lambda_\alpha} = \frac{\sqrt{16m_p eV}}{\sqrt{2m_p eV}} = \sqrt{\frac{16}{2}} = \sqrt{8}λα​λp​​=2mp​eV​16mp​eV​​=216​​=8​

  5. Final Numerical Value To find the answer to the nearest integer, we calculate the numerical value of 8\\\sqrt{8}8​. 8=22≈2×1.4142=2.8284\sqrt{8} = 2\sqrt{2} \approx 2 \times 1.4142 = 2.82848​=22​≈2×1.4142=2.8284

    Rounding 2.8284 to the nearest integer gives 3.

Final Answer

Thus, the ratio {{{\\\lambda _p}} \\over {{\\\\lambda _\\alpha }}} to the nearest integer is 3.

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