Question

Two charged particles A ($q_A = 2.84 \mu C$) and B ($q_B = 1.42 \mu C$) are fixed in place along the x-axis at x = $\pm 3.37$ cm, respectively. If a third charged particle C ($q_C = 3.96 \mu C$ and mass $m_C = 10.56$ mg) is released from rest on the y-axis at y = $2.57$ cm, what will the speed of particle C be when it reaches y = $4.47$ cm? Answer in $\frac{m}{s}$.

          Two charged particles A ($q_A = 2.84 \mu C$) and B ($q_B = 1.42 \mu C$) are fixed in place along the x-axis at x = $\pm 3.37$ cm, respectively. If a third charged particle C ($q_C = 3.96 \mu C$ and mass $m_C = 10.56$ mg) is released from rest on the y-axis at y = $2.57$ cm, what will the speed of particle C be when it reaches y = $4.47$ cm? Answer in $\frac{m}{s}$.
        
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Two charged particles A (qA = 2.84 μ C) and B (qB = 1.42 μ C) are fixed in place along the x-axis at x = ± 3.37 cm, respectively. If a third charged particle C (qC = 3.96 μ C and mass mC = 10.56 mg) is released from rest on the y-axis at y = 2.57 cm, what will the speed of particle C be when it reaches y = 4.47 cm? Answer in (m)/(s).

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University Physics with Modern Physics
University Physics with Modern Physics
Hugh D. Young 14th Edition
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Two charged particles A (qA = 2.84 μC) and B (qB = 1.42 μC) are fixed in place along the x-axis at x = ±3.37 cm, respectively. If a third charged particle C (qC = 3.96 μC and mass mC = 10.56 mg) is released from rest on the y-axis at y = 2.57 cm, what will the speed of particle C be when it reaches y = 4.47 cm? Answer in m/s.
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Transcript

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00:01 All right, hello, in this question, we have this charge configuration.
00:02 So we have two fixed charges here on the x -axis with the same charge and the same distance away from the origin.
00:08 And then we have a third charge here.
00:10 We're also given its mass.
00:12 And we're told that it's released from rest at y1.
00:15 And then we want to find the speed when it hits this point y2 up here.
00:19 We're asked to consider only electrical forces.
00:22 So in order to do this, we could do some of the forces.
00:27 But if we do that, as this particle moves away, it's going to get less and less force on it.
00:32 So we'd have to do some integral thing.
00:33 And while it's possible, it would be very messy.
00:36 Instead, i'm going to opt to use a conservation of energy approach.
00:40 So e1 and e2 are equal.
00:43 Now, what is our source of energy? well, we have electric potential here.
00:48 So initially, we have some electric potential at 1.
00:52 At the end, we're going to have some electric potential, not gravitational potential.
00:57 So at the end, we have some electric potential as well.
00:59 But then we're also going to have some kinetic energy.
01:02 So what is our electric potential? well, it's going to be our charge times the potential at 0 .1.
01:09 That is equal to charge at our potential at 0 .2 plus 1 half mv squared.
01:15 This v is speed.
01:16 It's not potential.
01:19 So i'll call it v final just to differentiate.
01:21 So we need to figure out what our potential is at 1 and 2...
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