A jumper of mass m and length t is placed on two parabolic rails in x-y plane. Shape of the rails can be described by |
\[~Rail\text{ 1}:y={{x}^{2}}\text{ }\left( and\text{ }z=0 \right)\] |
\[Rail\,2:y={{x}^{2}}(and=\ell )\] |
If x is horizontal and y is vertical direction and magnetic field in the space is\[{{b}_{0}}j,\] the jumper can remain in equilibrium when y coordinate of its ends is (\[i\]= current in jumper) |
A) \[\frac{i{{B}_{0}}\ell }{2mg}\]
B) \[\frac{i{{B}_{0}}\ell }{mg}\]
C) \[{{\left( \frac{i{{B}_{0}}\ell }{mg} \right)}^{2}}\]
D) \[{{\left( \frac{i{{B}_{0}}\ell }{2mg} \right)}^{2}}\]
Correct Answer: D
Solution :
F= \[{{B}_{0}}i\ell \],y=\[{{x}^{2}}\] |
For equilibrium, \[F\cos \theta =mgsin\theta \] |
Or \[\tan \theta =\frac{F}{mg}=\frac{{{B}_{0}}i\ell }{mg}\] |
Or \[\frac{dy}{dx}=\frac{{{B}_{0}}i\ell }{mg}\] Or \[2x=\frac{{{B}_{0}}i\ell }{mg}\] |
Or \[x=\frac{{{B}_{0}}i\ell }{2mg}\] Or \[\sqrt{y}=\frac{{{B}_{0}}i\ell }{2mg}\] Or \[y={{\left( \frac{{{B}_{0}}i\ell }{2mg} \right)}^{2}}\] |
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