The electric field in a region of space has the components \(E_y = E_z = 0\) and \(E_x = (4.30 N/(C·m))x\). Point A is on the y axis at y = 3.10 m, and point B is on the x axis at x = 2.00 m. What is the potential difference (in V) \(V_B – V_A\)?
@TuringTest Mi amigo, are you any good with this sort of stuff? It seems like it should be easy, but then I start thinking... then things go downhill after that.
draw the pic first
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\[\Delta V=\int\vec E\cdot d\vec s=\vec E\cdot \vec s\]
so what's the equation for \(\vec s\) is the real question here
*expression
Stupid question, but, what is \(\vec s\) And you just kinda beat me to the punch lol
well, it's the vector representation of the path from A to B so how might you represent the path from A to B in terms of \(\hat i\) and \(\hat j\) ?
\(\vec s=-3.1\hat i + 2 \hat j\) Does that seem right?
exactly now just do the dot product
\(\vec E=4.30\hat i\) Is this correct, as it is denoted x?
argh sorry bad connection :P yes, your notation is better than theirs haha, using x for a direction confuses things eventually
If so, it would be \(\Delta V=-13.33\hat i\)
how did you get that?
first of all, you should *never* have a vector left over after taking the dot product, since \(\hat i\cdot\hat i=1\)
Voltage is a scalar quantity like energy. It can be positive or negative between two points, but has no direction; only magnitude
your expression for \(\vec s\) is right, and your expression for \(\vec E\) is right, so you just didn't take the dot product right
Sorry, this connection is killing me. I think I just forgot to drop the \(\hat i\)
No, the magnitude it wrong, too
\(4.3\times -3.1~?\)
write out \(\vec E\cdot\vec s\)
which direction is 3.1 in?
\(\large{\Delta V = \vec E \cdot \vec s=4.3\hat i \cdot [2\hat i -3.1\hat j]=8.6}\) Stupid error haha
oh I see, this is my fault, I let you get away with writing the equation for s wrong the first time yes you got it :)
I just plugged it into WileyPLUS and it said it was wrong....
let's see...
hm... if it's not a sig fig issue I'm pretty puzzled. This is a pretty straight-forward question
unless by them saying \[\vec E=4.3x\]they mean\[\vec E=4.3x\hat i\]
in which case you have to integrate, as that would mean that E changes along x...
That could be... how would I go about doing that then?
Here is what it looks like exactly.
they probably mean the fiels is proportional to x I guess, as they did in that cube problem. To get the answer you do basically the same thing, but you have to integrate at the end\[\int\vec E\cdot d\vec s=\int(4.30x\hat i)\cdot(\hat j+\hat i)ds=\int_0^24.3xdx\]then integrate from x=0 to x=2...
field*
I literally get the same answer.
the details of the math are out of scope of the class, so I would use a symmetry argument instead of the "line integral" that I did oh yeah?
oh yeah, you would, by halving and then squaring x
@TuringTest are you any good at circuits?
@austinL how's it going?
Wait... are we doing \(V_A-V_B\) Don't we need to do \(V_B-V_A\)?
um... right... so we are going from higher potential to lower potential, so could the problem be a minus sign? do you have unlimited chances?
AHA!!!! :D That was the problem, we were doing it backwards. The answer is -8.6
And no, 4 tries total on all of my problems
I see, I always forget that detail :P The idea there is that because we integrated in the direction of the E-field, we are basically moving away from a positive charge, which means we are going from a higher to lower potential. Oh damn you, Benjamin Franklin, for making the electron negative and not positive.
I have always wondered how they picked these things... make North, North when referring to magnetism and negative, negative when referring to electricity.
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