Vector Calculus (5-12-2020)

Calculus Level pending

Closed curve C C is the intersection between the sphere ( x 2 + y 2 + z 2 = 1 ) (x^2 + y^2 + z^2 = 1) and the plane ( x + 3 y + 2 z = 1 ) (x + 3y + 2z = 1) . There is a vector field F = ( F x , F y , F z ) = ( x y 2 , y z , z x 2 ) \vec{F} = (F_x, F_y, F_z) = (x y^2, y z, z x^2) throughout all of space.

What is the absolute value of the line integral of F \vec{F} over C C ?

C F d \Big| \oint_C \vec{F} \cdot \vec{d \ell} \Big|


The answer is 0.0477.

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1 solution

Karan Chatrath
May 12, 2020

Consider the plane:

x + 3 y + 2 z = 1 x+3y+2z=1

This plane's intersection with the sphere is a circular closed curve. A unit vector normal to it is:

n ^ = 1 14 ( i ^ + 3 j ^ + 2 k ^ ) \hat{n} = \frac{1}{\sqrt{14}}\left(\hat{i} + 3 \ \hat{j} + 2 \ \hat{k}\right)

The line along this normal direction through the origin can be derived to be:

x = t x = t y = 3 t y = 3t z = 2 t z = 2t

Using this parameterization, the point of intersection between the line and the plane is found to be:

C = ( 1 14 , 3 14 , 2 14 ) C = \left(\frac{1}{14},\frac{3}{14},\frac{2}{14}\right)

This point C C is the center of the circle of the intersection of the plane and the sphere. Having found the center, consider another point on the plane. I chose:

P = ( 1 , 0 , 0 ) P = \left(1,0,0\right)

A vector joining points P P and C C directed towards P P is:

n 1 = P C \vec{n}_1 = \vec{P}-\vec{C}

The unit vector along this direction is:

n ^ 1 = n 1 n 1 \hat{n}_1 = \frac{\vec{n}_1}{\lvert \vec{n}_1 \rvert}

Now, a vector on the plane perpendicular to both n ^ \hat{n} and n ^ 1 \hat{n}_1 is:

n ^ 2 = n ^ × n ^ 1 \hat{n}_2 = \hat{n} \times \hat{n}_1

The radius of the circle of intersection can be found using Pythagoras' theorem as such:

R = 1 C 2 R = \sqrt{1 - \lvert \vec{C}\rvert^2}

Finally, any point on the circle of intersection is:

r = C + R cos θ n ^ 1 + R sin θ n ^ 2 \vec{r} = \vec{C} + R\cos{\theta} \ \hat{n}_1 + R\sin{\theta} \ \hat{n}_2

d r = ( R sin θ n ^ 1 + R cos θ n ^ 2 ) d θ d\vec{r} = \left(-R\sin{\theta} \ \hat{n}_1 + R\cos{\theta} \ \hat{n}_2\right)d\theta

d I = F d r dI = \vec{F} \cdot d\vec{r}

This dot product evaluates to some function of θ \theta times d θ d\theta , say f ( θ ) d θ f(\theta) \ d\theta

I = 0 2 π f ( θ ) d θ \implies I = \int_{0}^{2\pi} f(\theta) \ d\theta

This integral can also be done using's Stokes's theorem as such. Having parameterised the circle of intersection, it's elementary surface area can be parameterised as well. This gives:

C F d r = S ( × F ) d S \oint_{C} \vec{F} \cdot d\vec{r} = \int_{S} \left (\nabla \times \vec{F}\right)\cdot d\vec{S}

Where d S = r d r d θ n ^ d\vec{S} = r \ dr \ d\theta \ \hat{n} where r r varies from 0 0 to R R . Note that:

( × F ) = 0 \nabla \cdot \left (\nabla \times \vec{F}\right)=0

@Karan Chatrath Nice. BTW Upload the solution of Problem please sir

A Former Brilliant Member - 1 year, 1 month ago

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