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Given:

  • Initial speed $$v_{\text{initial}} = k \space \text{m/s}$$ in the positive x-direction $$\hat{i}$$
  • Applied force $$\mathbf{F} = n \, \text{N} $$ in the positive y-direction $$\hat{j}$$
  • $$ Mass = m \space \text{kg} $$

If this force is applied to the particle, I feel that the resultant velocity would have both i and j components, and so speed cannot remain constant

but since the force is perpendicular and no work is done, speed cannot change. I would like to see this solution work out vectorally so I see where I'm going wrong.

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    $\begingroup$ If this force is constantly applied then obviously it will stop being perpendicular and then the speed can change. You need a force that is perpendicular to the velocity at all times for the speed to stay constant. $\endgroup$ Commented Oct 17, 2023 at 13:26
  • $\begingroup$ @naturallyInconsistent I'm referring to a one time application of the force though. $\endgroup$ Commented Oct 17, 2023 at 13:47
  • $\begingroup$ You mean for one instant? Are you sure it is a finite force and not infinite force, i.e. a one-instant finite impulse? Forces are such things that "one time" does not make sense for them. $\endgroup$ Commented Oct 17, 2023 at 14:08
  • $\begingroup$ I could be wrong here, just trying to understand how this would work. What is the right way to think about this then? adding a force along the y axis to a particle moving along the x axis with speed v_x should result in v_x + something*v_y (since the force is along the y axis) which means the kinetic energy should change since speed now has two components but since W = FdCos(theta) and the angle is 90, W is zero and the kinetic energy should remain constant Im trying to reconcile these two ideas $\endgroup$ Commented Oct 17, 2023 at 15:14
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    $\begingroup$ That's the thing, you cannot apply a force at one instant and no more. $\endgroup$ Commented Oct 17, 2023 at 18:49

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The force has to last some $\Delta t$ so $v_y=\frac{F}{m}*\Delta t, s_y=a/2*t^2$ so Sped is not constant, but also you have Work $F\cdot s_y$

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