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Q.(i) What will be de-Broglie wavelength associated with-

(a) An electron moving with a speed of 5.4×1065.4\times10^{6} m/s.
(b) A ball of mass 150 gm travelling with a speed of 30 m/s. [2 marks]
(ii) Why macroscopic objects in our daily life do not show wave-like properties? [1 mark]
(OR)
Write two characteristic properties of nuclear force. Draw a plot of potential energy of a pair of nucleons as a function of their separation.
Uttarakhand UbseUttarakhand Board Intermediate (Class 12) 2025Subjective· 3mImportance★★★★★
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Figure — The 'Draw a plot' instruction belongs to the OR alternative (nuclear force PE curve), which the long answer fu
Figure — The 'Draw a plot' instruction belongs to the OR alternative (nuclear force PE curve), which the long answer fu

de Broglie wavelength λ=h/(mv)\lambda=h/(mv) is appreciable only for particles of very small mass, like electrons; for macroscopic masses it is utterly negligible.

(i)(a) Electron: me=9.1×10−31m_e = 9.1\times10^{-31} kg, v=5.4×106v = 5.4\times10^{6} m/s, h=6.6×10−34h=6.6\times10^{-34} Js.

λ=hmv=6.6×10−34(9.1×10−31)(5.4×106)=6.6×10−344.914×10−24≈1.34×10−10 m (≈1.34 A˚)\lambda = \frac{h}{mv} = \frac{6.6\times10^{-34}}{(9.1\times10^{-31})(5.4\times10^{6})} = \frac{6.6\times10^{-34}}{4.914\times10^{-24}} \approx 1.34\times10^{-10}\ \text{m}\ (\approx 1.34\ \text{Å})

(i)(b) Ball: m=150 gm=0.150m = 150\ \text{gm} = 0.150 kg, v=30v = 30 m/s.

λ=hmv=6.6×10−34(0.150)(30)=6.6×10−344.5≈1.47×10−34 m\lambda = \frac{h}{mv} = \frac{6.6\times10^{-34}}{(0.150)(30)} = \frac{6.6\times10^{-34}}{4.5} \approx 1.47\times10^{-34}\ \text{m}

(ii) Macroscopic objects do not show observable wave-like properties because their mass mm is enormously large compared to atomic particles, so their de Broglie wavelength λ=h/(mv)\lambda=h/(mv) (as computed above, ∼10−34\sim10^{-34} m for an everyday-sized object) is far smaller than any length that could ever be measured or that could produce observable diffraction/interference effects — hence their wave nature is completely masked, and they appear to obey purely classical (particle) mechanics.

OR (alternative) — nuclear force:

Two characteristic properties of the nuclear force: (1) it is a short-range force, effectively zero beyond a separation of about 3–4 fm (unlike gravitational or Coulomb forces which act over unlimited range); (2) it is charge-independent — the force between two protons, two neutrons, or a proton and a neutron is approximately the same, regardless of their charge.

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