1. **Integrate \( v_x \) to find \( x(t) \):**
The velocity component in the \( x \)-direction is given by
v_x = a
which leads to the differential equation
\frac{dx}{dt} = a
Integrating with respect to \( t \):
\int dx = \int a \, dt
x(t) = at + C
Given the initial condition \( x(0) = 0 \):
x(t) = at
2. **Substitute \( x(t) \) into \( v_y \) and find \( y(t) \):**
Substitute \( x = at \) into the expression for \( v_y \), where
v_y = bx
so
v_y = b(at) = bat
Now we integrate with respect to \( t \):
\frac{dy}{dt} = b(at)
\int dy = \int bat \, dt
y(t) = \frac{ba}{2} t^2 + C
With the initial condition \( y(0) = 0 \):
y(t) = \frac{ba}{2} t^2
3. **Eliminate \( t \) to get \( y(x) \):**
Since \( x = at \), solve for \( t \):
t = \frac{x}{a}
Substitute back into \( y(t) \):
y = \frac{ba}{2} \left( \frac{x}{a} \right)^2
y = \frac{ba}{2} \cdot \frac{x^2}{a^2}
y = \frac{b}{2a} x^2
Thus, the trajectory of the particle is
y(x) = \frac{b}{2a} x^2