A ball is launched from the ground at a 45 degree angle above the horizontal (which we take to be the x-axis). It rises to a maximum height, falls back down to the ground and bounces. After the bounce its velocity again makes a 45◦ angle to the horizontal x-axis, but the magnitude of the velocity right after the bounce is a factor of 3 times the magnitude before the bounce.

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Letting the time of the launch be t = 0, the bounce occurs at t = T. After the bounce the ball rises to a new maximum height and then bounces a second time. You can ignore air resistance. Take the acceleration of gravity to be g.

To tackle this problem, let's break it down into steps:

Step 1: Determine the initial velocity and angle
Since the ball is launched at a 45-degree angle, we can determine the initial velocity in terms of its horizontal and vertical components. Let's assume the magnitude of the initial velocity is "v". For a 45-degree launch angle, the vertical and horizontal components of velocity are the same, which means the initial vertical component of velocity is v and the initial horizontal component of velocity is also v.

Step 2: Calculate the maximum height reached in the first phase
To determine the maximum height reached by the ball, we need to use the kinematic equation for vertical motion. At the maximum height, the vertical velocity is zero (since the ball momentarily stops at the highest point). The initial vertical velocity is "v", and the acceleration is -g (negative because it acts against the motion). The equation we can use is:

v^2 = u^2 + 2as

where v is the final velocity (0 m/s), u is the initial vertical velocity, a is the acceleration, and s is the displacement (maximum height).

Plugging in the values, we have:

0 = v^2 + 2(-g)s
0 = v^2 - 2gs

Solving for "s", we get:

s = v^2 / (2g)

Step 3: Determine the time of flight for the first phase
To find the time of flight for the ball's first phase (from launch to maximum height), we can use the equation of motion for vertical motion:

s = ut + (1/2)at^2

where s is the displacement, u is the initial velocity, a is the acceleration, and t is the time of flight.

Plugging in the values, the equation becomes:

s = vt + (1/2)(-g)t^2
s = vt - (1/2)gt^2

Substituting the value of "s" from Step 2:

(v^2 / (2g)) = vt - (1/2)gt^2

Simplifying, we have:

v^2 = 2gvt - g(t^2)

Step 4: Calculate the time of flight for the first phase
Using the equation from Step 3, we can solve for the time of flight (t). Rearranging the equation from Step 3, we get:

gt^2 - 2vt + 2s = 0

This is a quadratic equation in terms of "t". Solving it will give us two solutions. We choose the positive solution since time cannot be negative.

Using the quadratic formula:

t = (-b + sqrt(b^2 - 4ac)) / (2a)

where a = g, b = -2v, and c = 2s:

t = (-(-2v) + sqrt((-2v)^2 - 4(g)(2s))) / (2g)
t = (2v + sqrt(4v^2 - 8gs)) / (2g)
t = (v + sqrt(v^2 - 2gs)) / g

Step 5: Calculate the time of the first bounce
The time of the first bounce (T) is the time when the ball returns to the ground after reaching the maximum height. Since the ball is launched at t = 0, the time of the first bounce occurs twice the time of flight (T = 2t).

T = 2t = 2((v + sqrt(v^2 - 2gs)) / g)

Step 6: Determine the velocity after the bounce
After the first bounce, the magnitude of the velocity is 3 times the magnitude before the bounce. Let's call the velocity right before the bounce "v_b" and the velocity right after the bounce "v_a". We can set up the following equation:

3v_b = v_a

From the conservation of energy, the kinetic energy before the bounce is equal to the kinetic energy after the bounce. The kinetic energy is given by:

KE = (1/2)mv^2

Using this, we can write:

(1/2)mv_b^2 = (1/2)mv_a^2

Since the mass (m) is canceled out on both sides, we can rewrite the equation as:

v_b^2 = v_a^2

Using the relationship between v_b and v_a, we can write:

v_a = 3v_b

Substituting this into the equation above, we get:

v_b^2 = (3v_b)^2
v_b^2 = 9v_b^2

Simplifying, we find:

8v_b^2 = 0

Since velocity cannot be zero, this equation has no solution.

Therefore, it is not possible for the ball to bounce according to the given conditions.