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garylau
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Did i make mistake in my calculation?blue_leaf77 said:Yes you can also do that, and may be in the third line you can use the fact that the derivative of ##\sec x## is ##\sec x \tan x##. But your way is kind of longer than necessary.
Looks good. Now you only need to do the last integral and change back to the original variable ##u## and plug in the integral limits.garylau said:Did i make mistake in my calculation?
If you use this substitution,cnh1995 said:Use the substitution
√(2u+z2)=t.
Oh i see thank youcnh1995 said:If you use this substitution,
du/√(2u+z2) can be replaced by 'dt' and u+z2=(t2+z2)/2.
So, you'll simply get it as ∫2dt/(t2+z2) which is (2/z)tan-1(t/z).
You get your answer in just two steps.
blue_leaf77 said:Looks good. Now you only need to do the last integral and change back to the original variable ##u## and plug in the integral limits.
i don't know why i do it wrong (is there a minus sign??)blue_leaf77 said:Looks good. Now you only need to do the last integral and change back to the original variable ##u## and plug in the integral limits.
I don't know why you are redoing your work, you are almost there in post #5.garylau said:i don't know why i do it wrong (is there a minus sign??)
can you help me to check it
thank
blue_leaf77 said:I missed one mistake in your work in post #5. In the last line, you should have removed the integral and the integration element. There should only be #\theta## there.
I don't know why you are redoing your work, you are almost there in post #5.
yesblue_leaf77 said:I missed one mistake in your work in post #5. In the last line, you should have removed the integral and the integration element. There should only be #\theta## there.
I don't know why you are redoing your work, you are almost there in post #5.
what if i try to integrate it using multiple integration...seems quite tough then...can you help regarding that??cnh1995 said:If you use this substitution,
du/√(2u+z2) can be replaced by 'dt' and u+z2=(t2+z2)/2.
So, you'll simply get it as ∫2dt/(t2+z2) which is (2/z)tan-1(t/z).
You get your answer in just two steps.
The electric field of a square sheet can be calculated by dividing the total charge of the sheet by the area of the sheet. This gives the electric field strength at any point on the sheet.
The direction of the electric field of a square sheet is perpendicular to the surface of the sheet, pointing away from the sheet if it is positively charged and towards the sheet if it is negatively charged.
The electric field of a square sheet follows an inverse relationship with distance. This means that as the distance from the sheet increases, the electric field strength decreases.
The electric field of a square sheet is uniform at all points on the sheet, while the electric field of a point charge decreases as the distance from the point charge increases. Additionally, the direction of the electric field of a square sheet is always perpendicular to the surface, while the direction of the electric field of a point charge depends on the location of the point charge.
Yes, the electric field of a square sheet can be integrated to find the potential. The potential at any point is equal to the negative integral of the electric field from that point to a reference point.