A ring of mass m and radius r and made of an insulating material carries uniform charge. Initially it rests vertically on a frictionless horizontal tabletop on the left side of the vertical plane AA'. In the region to the right side of AA' is a uniform horizontal magnetic field of induction B pointing everywhere parallel to the axis of the ring. The ring is pushed forward with velocity v but no rotation. If q is the charge on the ring so that it just starts rolling on the tabletop on entering completely into the magnetic field, what is [200q] in SI units?
details and Assumptions
∙ In the given figure cross sign indicates that the field is towards us.
∙ neglect induced electric fields.
∙ the mass per unit length λ
∙ λ = 7
∙ v = 3 m / s
∙ B = 4 T
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Lots of mistakes: (Not offensive)
1) You don't consider induced electric field , which is necessary.
2) Even if you don't consider the induced electric field, how can you state that when v f = ω R , rolling without slipping has started. The net torque and net force both are backwards. When for the first time v = ω R , the velocity of bottom point is 2 v .
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Yes, there are many things that the solution is missing.
Thanks for pounting out Sorry the magetic field direction must be towards us is out of the plane.
i was trying using the induced electric field,but the answer came out to be different from the given answer. I don't see a reason why induced field was not taken into account in this solution.
too easy,,, but the magnetic field should be at us now away,, unless the charge given is negative,,, But u solved in too complex manner,. heres how you should do it,, see when it completely enters magnetic field,.,. each point on the ring rotates at v and translates at v (pure rolling) thus net velocity is root 2 * v ,, now use the formula qvB= mv^2/r and substitute v root 2 for v and put values,, then get q multiply by 200 u will get 9330.05 then take greatest integer function to get 9330
can u explain torque equation
But, when the ring has traveled a distance x , wouldn't it be rotating as well? So, why didn't you consider the Force due the rotational interaction with the magnetic field?
To make it clear, let the angular velocity of the ring at a distance x be w .
Taking the element at θ with an angular width of d θ , the Lorentz force due to this w will be,
d F = B ( w R ) ( λ R d θ ) (Note that d F acts towards the center of the ring)'
As d F acts towards the center of the ring, it won't produce a torque, but surely the summation of d F cos θ (vertical component of d F cancels out due to symmetry) would result in a net force, acting opposite to the motion of the ring (towards left).
So, why didn't you consider the work done due to this force?
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The net work done by magnetic field is 0 . Divide the ring in elements, and on each element, force is perpendicular to velocity. Hence, it does no work on any element and hence on the ring.
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I agree with you work done due to magnetic force ie passing through the cm Is zero torque is also zero. The only mistake is that I didn't mention to neglect induced electric field and also I made a silly mistake while mentioning the direction of magnetic field. I have made corrections. Thank you for the clarification.
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@Milun Moghe – Torque of magnetic field due to rotation is 0 , not due to translation. Net torque due to magnetic field is not 0. You too know that as you used it in solution :P
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@Jatin Yadav – yes i mean due to rotation torque as well as work is zero
Well considered torque about cm so due to the angular velocity the force will pass through the cm
Hats off to the question maker
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Let us consider a moment when the cm of the ring travels a distance x. Applying torque equation
τ = ∫ − θ θ B ( v c o s θ ) λ ( R d θ ) R = m R 2 d t d ω
m 2 B v λ q s i n θ = d t d ω here v is a variable velocity of cm at a certain instant at distance x
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Applying energy conservation , for initial and when just starts rolling Remember that torque due to rotation is zero because the force all the force is passing through the cm therefore i only considered torque due to translation.
2 1 m v 2 = 2 1 m v f 2 + 2 1 m R 2 ω 2
v f = ω R
∫ 0 2 R λ q 2 B R 2 R x − x 2 d x = ∫ 0 2 R V d ω
we get q = B R 2 m v = 2 2 π B λ m v
[ 2 0 0 q ] = 9 3 3 0 C