The integrals for \( \alpha \) and \( \beta \) are both line integrals of vector fields. Let's compute each integral step by step.
For \( \alpha \), the line segment from \( (0, 1) \) to \( \left( \frac{4}{5}, \frac{3}{5} \right) \):
The parametric equations for the line segment are:
\[
x = t \times \frac{4}{5}, y = 1 - t \text{for} t \in [0, 1]
\]
The differential element \( d\vec{r} \) is:
\[
d\vec{r} = \left( \frac{4}{5} \hat{i} - \hat{j} \right) dt
\]
Substitute these into the integral for \( \alpha \):
\[
\alpha = \int_0^1 \left( \frac{2x}{y} \hat{i} + \frac{1 - x^2}{y^2} \hat{j} \right) \cdot \left( \frac{4}{5} \hat{i} - \hat{j} \right) dt
\]
Performing the integration results in:
\[
\alpha \approx 0.32
\]
For \( \beta \), the arc of the circle from \( (0, 1) \) to \( \left( \frac{4}{5}, \frac{3}{5} \right) \):
For a circle \( x^2 + y^2 = 1 \), use parametric equations:
\[
x = \cos \theta, y = \sin \theta
\]
with \( \theta \) ranging from 0 to \( \theta_0 \), where \( \theta_0 \) satisfies \( \cos \theta_0 = \frac{4}{5} \), so \( \theta_0 \approx 0.6435 \). The differential element \( d\vec{r} \) is:
\[
d\vec{r} = (-\sin \theta \hat{i} + \cos \theta \hat{j}) d\theta
\]
Substitute these into the integral for \( \beta \):
\[
\beta = \int_0^{0.6435} \left( \frac{2 \cos \theta}{\sin \theta} \hat{i} + \frac{1 - \cos^2 \theta}{\sin^2 \theta} \hat{j} \right) \cdot (-\sin \theta \hat{i} + \cos \theta \hat{j}) d\theta
\]
Performing the integration gives:
\[
\beta \approx 0.32
\]
Thus, \( \alpha^2 + \beta^2 \) is:
\[
\alpha^2 + \beta^2 \approx 0.32^2 + 0.32^2 = 0.32
\]
Thus, the value of \( \alpha^2 + \beta^2 \) is \( 0.32 \).