UrbanXrisis
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My question involves two example problems.
1. A ring of radius a carries a uniforly distributed positive total charge Q. Calculate the electrical field due to the ring at a point P lying a distance x from its center along the central axis perpendicular to the plane of the ring.
dE_x=dEcos \theta = (k \frac{dq}{r^2})\frac {x}{r} = \frac{kx}{(x^2+a^2)^{3/2}} dq
E_x= \int \frac{kx}{(x^2+a^2)^{3/2}}dq=\frac{kx}{(x^2+a^2)^{3/2}} \int dq
E_x= \frac{kx}{(x^2+a^2)^{3/2}}Q
2. A disk of radius R has a uniform surface charge density \sigma. Calculate the electrical field at a point P that lies along the central perpendicular axis of the disk and a distance x from the center of the disk.
dq=2 \pi \sigma r dr
dE=\frac{kx}{(x^2+a^2)^{3/2}}(2 \pi \sigma r dr)
E=kx \pi \sigma \int_0 ^R \frac{2r dr}{(x^2+a^2)^{3/2}}
My question is:
In problem #1 vs Problem #2, why are there limits on #2 and why does #1 only integrate the dq?
1. A ring of radius a carries a uniforly distributed positive total charge Q. Calculate the electrical field due to the ring at a point P lying a distance x from its center along the central axis perpendicular to the plane of the ring.
dE_x=dEcos \theta = (k \frac{dq}{r^2})\frac {x}{r} = \frac{kx}{(x^2+a^2)^{3/2}} dq
E_x= \int \frac{kx}{(x^2+a^2)^{3/2}}dq=\frac{kx}{(x^2+a^2)^{3/2}} \int dq
E_x= \frac{kx}{(x^2+a^2)^{3/2}}Q
2. A disk of radius R has a uniform surface charge density \sigma. Calculate the electrical field at a point P that lies along the central perpendicular axis of the disk and a distance x from the center of the disk.
dq=2 \pi \sigma r dr
dE=\frac{kx}{(x^2+a^2)^{3/2}}(2 \pi \sigma r dr)
E=kx \pi \sigma \int_0 ^R \frac{2r dr}{(x^2+a^2)^{3/2}}
My question is:
In problem #1 vs Problem #2, why are there limits on #2 and why does #1 only integrate the dq?