Magnetic induction of circular loop at axial point

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BREAD
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Homework Statement


Typed homework problem 6 about a circular wire loop of radius a in the XY-plane, centred at the origin and carrying current I, asking for the magnetic induction on the axis and for derivatives of B_y and components of B near the axis.


Homework Equations

The Attempt at a Solution


Handwritten solution to a magnetic field problem: a diagram of a current loop of radius R with axis z and point P at height z, followed by the Biot-Savart expressions for dB and the axial field Bz = mu0 I a^2 / (2 (a^2 + z^2)^(3/2)), and part (b) asking for the partial derivative of Bz with respect to y.


This is what i did about (a)
but i don't know how to approach (b), it doesn't have x,y components, only Bz component.
 
I think your answer to a is right - not expert in this area.
For b, a dependent variable being zero at some value of the independent variable does not imply that its derivative is also zero there.
I suggest working on b2, returning to b1 afterwards.
 
BREAD said:
I think i solve (1)
And very neatly too.
BREAD said:
the problem is (2),(3)
These are easy. Fundamental differential calculus: f(x+Δx)≈f(x)+f'(x)Δx.
 
haruspex said:
And very neatly too.

These are easy. Fundamental differential calculus: f(x+Δx)≈f(x)+f'(x)Δx.
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Handwritten derivation on lined paper: a Taylor expansion of B_z(0, Δy, z) − B_z(0, 0, z) ≈ ∂B_z/∂y at (0,0,z) times Δy, with ∂B_z/∂y and ∂B_y/∂z circled, and curl-zero relations ∂B_z/∂y = ∂B_y/∂z listed on the right.


I tried it , but is (2) right? and idw how to get ∂(B_z)/∂y|_(0, 0, z). I heard somewhere that by properties of curl of B (as i wrote)
∂(B_z)/∂y|_(0, 0, z) is changed to ∂(B_y)/∂z|_(0, 0, z), but i can't solve this.
 
BREAD said:
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View attachment 114508

I tried it , but is (2) right? and idw how to get ∂(B_z)/∂y|_(0, 0, z). I heard somewhere that by properties of curl of B (as i wrote)
∂(B_z)/∂y|_(0, 0, z) is changed to ∂(B_y)/∂z|_(0, 0, z), but i can't solve this.
Isn't By identically zero on the z axis?