Verified Solution • 2025–26 Session moderate

QJEEM18Phdf88: JEE Main 2018 Physics - Class 12 JEEM18Phdf88 Solution: Two electrons are moving with non-relativistic speed…

Two electrons are moving with non-relativistic speed perpendicular to each other. If corresponding de Broglie wavelength are λ1{\lambda _1} and λ2,{\lambda _2}, their de Broglie wavelength in the frame of reference attached to their center of masses :

Multiple Choice Options

  • A λCM=λ1=λ2{\lambda _{CM}} = {\lambda _1} = {\lambda _2}
  • B λCM=2λ1λ2λ12+λ22{\lambda _{CM}} = {{2{\lambda _1}{\lambda _2}} \over {\sqrt {\lambda _1^2 + \lambda _2^2} }}
  • C 1λCM=1λ1+1λ2{1 \over {{\lambda _{CM}}}} = {1 \over {{\lambda _1}}} + {1 \over {{\lambda _2}}}
  • D λCM=(λ1+λ22){\lambda _{CM}} = \left( {{{{\lambda _1} + {\lambda _2}} \over 2}} \right)

Step-by-Step Verified Solution

As we know,

momentum (p) = hλ{h \over \lambda }

Let one perticle is moving in x direction and other is in y dirrection.

∴    \therefore\,\,\,\, momentum of each electrons hλ1i^{h \over {{\lambda _1}}}\widehat i and hλ2j^{h \over {{\lambda _2}}}\widehat j

∴    \therefore\,\,\,\, Velocity of each electrons hmλ1i^{h \over {m{\lambda _1}}}\widehat i and hmλ2j^{h \over {m{\lambda _2}}}\widehat j

∴    \therefore\,\,\,\, Velocity of center of mass (υ→CM)\left( {{{\overrightarrow \upsilon }_{_{CM}}}} \right) = υ1i^+υ2j^2{{\upsilon _1^{\widehat i} + \upsilon _2^{\widehat j}} \over 2}

Now, velocity of first electron about center of mass,

υ→1CM{\overrightarrow \upsilon _{_{1CM}}} = υ1i^\upsilon _1^{\widehat i} −- (υ1i^+υ2j^2)\left( {{{\upsilon _1^{\widehat i} + \upsilon _2^{\widehat j}} \over 2}} \right)

= υ1i^−υ2j^2{{\upsilon _1^{\widehat i} - \upsilon _2^{\widehat j}} \over 2}

Similarly,

υ→2CM=υ2j^−υ1i^2{\overrightarrow \upsilon _{_{2CM}}} = {{\upsilon _2^{\widehat j} - \upsilon _1^{\widehat i}} \over 2}

Here,

∣υ→1CM∣=∣υ→2CM∣=12\left| {{{\overrightarrow \upsilon }_{_{1CM}}}} \right| = \left| {{{\overrightarrow \upsilon }_{_{2CM}}}} \right| = {1 \over 2}

∴    \therefore\,\,\,\, υ\upsilon = 12{1 \over 2} h2m2λ12+h2m2λ22\sqrt {{{{h^2}} \over {{m^2}\lambda _1^2}} + {{{h^2}} \over {{m^2}\lambda _2^2}}}

⇒\Rightarrow     \,\,\,\, m υ\upsilon = 12{1 \over 2} h2λ12+h2λ22{\sqrt {{{{h^2}} \over {\lambda _1^2}} + {{{h^2}} \over {\lambda _2^2}}} }

⇒\Rightarrow     \,\,\,\, hλCM{h \over {{\lambda _{CM}}}} = h 14λ12+14λ22{\sqrt {{1 \over {4\lambda _1^2}} + {1 \over {4\lambda _2^2}}} }

⇒\Rightarrow     \,\,\,\, 1λCM=λ12+λ222λ1λ2{1 \over {{\lambda _{CM}}}} = {{\sqrt {\lambda _1^2 + \lambda _2^2} } \over {2{\lambda _1}{\lambda _2}}}

⇒\Rightarrow     \,\,\,\, λCM=2λ1λ2λ12+λ22{\lambda _{CM}} = {{2{\lambda _1}{\lambda _2}} \over {\sqrt {\lambda _1^2 + \lambda _2^2} }}

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