Using Euler’s equation for an inviscid fluid (no body forces):
\[
\nabla p = -\rho\,(\vec{V}\cdot\nabla)\vec{V}.
\]
Step 1: Compute directional derivatives.
Given
\[
u = y^{2} - x^{2}, \qquad v = 2xy.
\]
Compute:
\[
\frac{\partial u}{\partial x} = -2x, \quad \frac{\partial u}{\partial y} = 2y,
\]
\[
\frac{\partial v}{\partial x} = 2y, \quad \frac{\partial v}{\partial y} = 2x.
\]
Step 2: Compute convective acceleration $(\vec{V}\cdot\nabla)\vec{V$.}
At $(x,y)=(1,1)$:
\[
u = 0,\ v = 2.
\]
Thus,
\[
a_x = u(-2) + v(2) = 0 + 4 = 4,
\]
\[
a_y = u(2) + v(2) = 0 + 4 = 4.
\]
So,
\[
(\vec{V}\cdot\nabla)\vec{V} = 4\hat{i} + 4\hat{j}.
\]
Step 3: Apply Euler's equation.
Density $\rho = 1.5$:
\[
\nabla p = -1.5(4\hat{i} + 4\hat{j}) = -6\hat{i} - 6\hat{j}.
\]
Final Answer: $-6\hat{i} - 6\hat{j}$