Collision of two particles: constant velocity, constant acceleration In the figure, particle $A$ moves along the line $y = 25~\text{m}$ with a constant velocity $v$ of magnitude $3.0~\text{m}/\text{s}$ and directed parallel to the $x$ axis. At the instant particle A passes the $y$-axis, particle $B$ leaves the origin with zero initial speed and constant acceleration $a$ of magnitude $0.44~\text{m}/\text{s}^2$. What angle $\theta$ between $a$ and the positive direction of the $y$-axis would result in a collision?
I did the problem but I'm not getting the right answer? How would this be solved and/or what am I doing wrong?
You don't have to read this part but to solve it, 
Both have a same final displacement in the x direction so if you use an equation 
$3t = 0.5 \cdot 0.44 \cdot t^2$ with $t = 13.64~\text{s}$.
Since it has the same $y$ point ($25$ m height) the angle can be found with $\arctan(13.64\cdot 3/25)$. Then you subtract that from $90$ to get the angle with reference to the $y$-axis.
What am I doing wrong here?
 A: Mathematical Model
It is convenient to use vectors here. For particle $A$ we have:
$$
r_A(t) = r_A(0) + v_A t = (x_A(0), 25) + (3, 0) t = (x_A(0) + 3t, 25)
$$
where the text gives $x_A(0) = 0$.
For particle $B$ we have
$$
a_B(t) = a \\ 
v_B(t) = v_B(0) + a t = at \\
r_B(t) = r_B(0) + \frac{1}{2}a t^2 
= \frac{1}{2}a t^2
= ((1/2)\lVert a \rVert \sin(\theta) t^2,(1/2)\lVert a \rVert \cos(\theta) t^2)
$$

The above image shows the trajectory of $A$ (green) and of $B$ (blue) and where the trajectories intersect at point $X$. Also the angle is given (named $\alpha$ instead of $\theta$).
You can fiddle with a live version here.
Calculating the Collision Point
For a collision we need $r_A(t) = r_B(t) = X$ for some $t$.
The intersection point $X$ is
$$
X = (\xi, 25)
$$
with $\tan(\theta) = \xi / 25 \iff \xi = 25 \tan(\theta)$.
$A$ arrives at $X$ if
$$
t = (25/3) \tan(\theta) \quad (1)
$$
$B$ arrives at $X$ if
$$
\frac{1}{2} \lVert a \rVert \sin(\theta) t^2 = 25 \tan(\theta) \quad (2) \\
\frac{1}{2} \lVert a \rVert \cos(\theta) t^2 = 25 \quad (3)
$$
Alas equation $(2)$ and $(3)$ are equivalent, division of both sides of $(2)$ by $\tan(\theta)$ gives $(3)$.
Inserting $(1)$ into $(3)$ gives
$$
\frac{1}{2} \lVert a \rVert \cos(\theta) 
\left(\frac{25}{3}\right)^2 \tan^2(\theta) = 25 \iff \\
25 \lVert a \rVert \sin^2(\theta) = 18 \cos(\theta) \quad (4)
$$
To limit the solutions we should note that $\theta \in (0, \pi/2)$.
Algebraic Solution
Substituting (see Tangent half-angle formulas)
$$
t = \tan(\theta/2) \\
\sin(t) = \frac{2t}{1+t^2} \\
\cos(t) = \frac{1-t^2}{1+t^2} \\
$$
(note: this $t$ is not the time $t$ from further above, but just used for this intermediate calculation of $\theta$ from equation $(4)$) we get
$$ 
25 \lVert a \rVert \left(\frac{2t}{1+t^2} \right)^2 
= 18 \frac{1-t^2}{1+t^2} \iff \\
25 \lVert a \rVert 4t^2 = 18(1-t^2)(1+t^2) = 18(1-t^4) \\
t^4 + \frac{50}{9} \lVert a \rVert t^2 - 1 = 0 \quad (5)
$$
Introducing $s = t^2$ we get
$$
s^2 + \frac{50}{9} \lVert a \rVert s - 1 = 0 \quad (6)
$$
which has the solutions
$$
s = \frac{\pm \sqrt{81+25^2 \lVert a \rVert^2}-25\lVert a \rVert}{9}
$$
we discard the negative solution and apply $25 \lVert a \rVert = 11$ and get
$$
s = \frac{\sqrt{202} - 11}{9} \\
t = \frac{\sqrt{\sqrt{202}-11}}{3} \\
\theta = 2 \arctan{\frac{\sqrt{\sqrt{202}-11}}{3}} \approx 1.0771 \approx 61.714^\circ
$$
Inserting in equation $(1)$ gives
$$
t \approx (25/3) \tan(1.0771) \approx 15.485 \, \text{s}
$$
A: How can there be an angle between an acceleration and the $y$-axis? I suppose you mean there is an angle between the line along which particle $B$ moves and the $y$-axis. 
In order for $B$ to collide with $A$, it has to move farther than $A$ does, because $B$ travels the entire hypotenuse of a right triangle 
while $A$ travels just one leg of that triangle.
So your first equation for $t$ is wrong:
the time of collision, $0.5 \cdot 0.44 \cdot t^2 > 3t$;
the two are not equal.
The ratio of the distance traveled by $A$ to the distance
traveled by $B$ is just the sine of the angle $\theta$
(in fact it is practically the definition of $\sin(\theta)$).
The correct equation is
$$
3t = (0.5 \cdot 0.44 \cdot t^2) \sin(\theta).
$$
This is not enough information to solve the problem.
But you can also use the fact that the other leg of the right triangle
has length $25$, that is,
$$
25 = (0.5 \cdot 0.44 \cdot t^2) \cos(\theta).
$$
This gives you two equations in two unknowns. They are not the easiest
equations to solve simultaneously, but they are solvable.
Wolfram Alpha gives four solutions, only one of which has a
positive real value of $t$; in that solution, $t > 15$,
and the angle is about $62$ degrees.
