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Section:
Physics
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© examsnet.com
Question : 1 of 16
Marks:
+1
,
-0
In a scattering experiment, a particle of mass
2
m
2 \text{ m}
2
m
collides with another particle of mass
m
m
m
, which is initially at rest. Assuming the collision to be perfectly elastic, the maximum angular deviation
θ
\theta
θ
of the heavier particle, as shown in the figure, in radians is:
[JEE Adv 2025 P1]
π
\pi
π
tan
−
1
(
1
2
)
\tan^{-1} \left( \frac{1}{2} \right)
tan
−
1
(
2
1
)
π
3
\frac{\pi}{3}
3
π
π
6
\frac{\pi}{6}
6
π
Validate
Solution:
In centre of mass frame
Speed does not change only orientation does
For
θ
\theta
θ
to maximize
v
1
,
C
M
→
⊥
v
1
→
\overrightarrow{v_{1, C M}} \perp \overrightarrow{v_1}
v
1
,
CM
⊥
v
1
⇒
sin
θ
=
v
1
,
C
M
v
C
M
\Rightarrow \sin \theta = \frac{v_{1, C M}}{v_{C M}}
⇒
sin
θ
=
v
CM
v
1
,
CM
v
1
,
C
M
=
m
2
v
12
→
m
1
+
m
2
⇒
v
1
→
=
m
2
u
1
→
m
1
+
m
2
v_{1, C M} = \frac{\overrightarrow{m_2 v_{12}}}{m_1+m_2} \Rightarrow \overrightarrow{v_1} = \frac{\overrightarrow{m_2 u_1}}{m_1+m_2}
v
1
,
CM
=
m
1
+
m
2
m
2
v
12
⇒
v
1
=
m
1
+
m
2
m
2
u
1
v
C
M
=
m
1
v
1
+
m
2
v
2
→
→
m
1
+
m
2
=
m
1
u
1
→
m
1
+
m
2
v_{C M} = \frac{\overrightarrow{m_1 v_1 + m_2 \overrightarrow{v_2}}}{m_1+m_2} = \frac{\overrightarrow{m_1 u_1}}{m_1+m_2}
v
CM
=
m
1
+
m
2
m
1
v
1
+
m
2
v
2
=
m
1
+
m
2
m
1
u
1
⇒
sin
θ
=
m
2
m
1
⇒
sin
θ
=
m
2
m
\Rightarrow \sin \theta = \frac{m_2}{m_1} \Rightarrow \sin \theta = \frac{m}{2 m}
⇒
sin
θ
=
m
1
m
2
⇒
sin
θ
=
2
m
m
θ
=
3
0
∘
=
π
6
\theta = 30^{\circ} = \frac{\pi}{6}
θ
=
3
0
∘
=
6
π
© examsnet.com
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