A particle having charge ( − 2 0 2 0 C ) and mass 2 0 2 1 k g moves in x − y plane. A constant electric field E = 2 N C − 1 is present in the region along positive y direction. The equation of motion of the particle has form y = 3 x − 4 x 2 . Find the speed of the particle at the origin. If your answer comes in the form of 1 4 . 5 9 ,then type it as 1 5 (round off to nearest integer)
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@Steven Chase I was getting 1 . 9 9 9
Did you get 0.5 for the horizontal speed?
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I get v x = 2 q a where a = − y ¨
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@Steven Chase Btw how to write that double derivative in dot form. I just get tired by finding that sign in latex.???
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@A Former Brilliant Member – Just add another d in the latex. \ddot{x}
Where does that expression come from?
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@Steven Chase – @Steven Chase Did you find out any mistake. Link?
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@A Former Brilliant Member – What link?
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@Steven Chase – @Steven Chase Check your notifications
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@A Former Brilliant Member – I don't see a link anywhere
@Steven Chase
I wanted to show this through that link. Now forget that link.
I am also little comfused in this question. The solution of this question which I get on the web few days ago is this
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The first line of the solution is obviously wrong
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@Steven Chase – @Steven Chase well this solution is provided ny a website which is wrong and I have attached answer according to this only.as therefore I was also little bit confused.differentiating with respect to x in left . And differentiating with respect to t in right. Yes I also faced this problems.i will correct the problem according to your answer. Cheers!!
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@A Former Brilliant Member – Sounds good, thanks
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@Steven Chase – @Steven Chase will you make a problem on M a g n e t i s m which is entirely new. By doing these flux problem I am getting bored Now I want to do NEW problems.
Let the horizontal and the vertical components of the velocity of the particle at the origin be u and v respectively. There is no acceleration in the horizontal direction, and hence u is constant. Acceleration of the particle along the downward vertical direction is w = 2 0 2 1 2 0 2 0 × 2 m/s 2 . Hence the equation of the trajectory of the particle is y = u v x − 2 1 w u 2 x 2 . Comparing with the given equation, we get v = 3 u , u 2 = 8 × 2 0 2 1 2 0 2 0 × 2 ⟹ the magnitude of velocity at the origin = u 2 + v 2 = u 1 0 = 2 0 2 1 5 0 5 0 ≈ 1 . 5 8 . So the answer is [ 1 . 5 8 ] = 2 .
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Assume that the electric force is solely responsible for the trajectory. The position, velocity, and acceleration are:
x = x y = 3 x − 4 x 2 x ˙ = x ˙ y ˙ = 3 x ˙ − 8 x x ˙ x ¨ = x ¨ y ¨ = 3 x ¨ − 8 ( x x ¨ + x ˙ 2 )
At x = 0 :
x ¨ = x ¨ y ¨ = 3 x ¨ − 8 x ˙ 2
We know that the electric field is only in the y direction, so this further reduces to:
x ¨ = 0 y ¨ = − 8 x ˙ 2
Setting the force equal to the y acceleration:
m a = q E 2 0 2 1 ( 8 x ˙ 2 ) = 2 0 2 0 ( 2 )
This yields:
∣ x ˙ ∣ ≈ 0 . 5 ∣ y ˙ ∣ ≈ 1 . 5 x ˙ 2 + y ˙ 2 ≈ 1 . 5 8