# Somewhat unusual projectile motion question

A stone must fly over two walls of height $h_1$ and $h_2$ $(h_2~ > ~h_1)$ from the side of the lower wall. The distance between the upper points of the two walls near which the stone's trajectory lies is $L$. Find the minimum velocity of the stone. (source: AN Matveev's Mechanics and Relativity).

Answer:$\sqrt{g(h_1+h_2+L)}$, where $g$ is acceleration due to gravity

The rather terse nature of the problem statement is very typical of Russian texts. I'm an intermediate/advanced self-learner and I love to wrangle with these kinds of problems. This problem seemed like a basic projectile motion problem but this has got me in knots - If the limiting height is $h_2$, why does the problem need $h_1$? And, there is no angle to use either. What's the significance of the requirement for minimum velocity? Clearly, it has to cross the walls, and based on what I see, $h_1$ likely lies below the trajectory and $h_2$ must just touch the trajectory and this can potentially give the velocity. But, I'm unable to find the approach to solve this. Can anyone provide a way to think about this problem?

• The stone will be at a fixed distance from the first wall, which is point 1 on its parabolic path. Point 2 corresponds to the lower height and point 3 corresponds to the higher height. This defines 3 points on a parabola. A parabolic equation has 3 constants in it, and any given 3 points uniquely define a given parabola. Thus, there is only ONE velocity which will solve the problem ... there is no "minimum" velocity. There may be a possible problem in translation in going from Russian to English. – David White Jul 27 '18 at 5:07

The problem is kind of hard to solve if one is not careful. One can write the satisfying equations but still might not be able to find the answer. I will outline a way to this.

The idea is that at the minimum required velocity the projectile just touches the top of the walls. Let the velocity and angle of projection at the origin be $$v_0$$ and $$\theta _0$$. From the origin the projectile goes and touches the top of the first wall. You can view the rest of its motion as a projectile projected from the top of the first wall with velocity $$v_1$$ at an angle $$\theta_1$$(both are unknown at this point). The following relation holds $$v_1 ^2 = v_0 ^2 -2gh_1.$$ Define $$\sin(\phi) = \frac{h_2 - h_1}{L}$$. The projectile should now go and touch the top of the second wall which means w.r.t the new origin it must pass through the point $$(L cos(\phi), h_2 - h_1)$$. You can plug this in to the equation of projectile parabola to get.

$$h_2 - h_1 = \tan(\theta_1)[L\cos(\phi)] - \frac{gL^2\cos^2(\phi)}{2(v_0^2 -2gh_1)\cos^2(\theta_1)}$$.

Now rearrange this and write $$v_0$$ in terms of $$\theta_1$$. Everything else are parameters given in the question. Use calculus to minimize the value of $$v_0$$. You'll get the answer. Let me know if anything is not clear.

• excellent answer! I followed through the routine math and it is the best approach. I used the definition of $\sin(\phi)$ to simplify the Math. The tough part for me in this problem was seeing that $h_1$ lies on the parabola, I was thinking that the trajectory will always lie above $h_1$ But, the cool part is that when $h_1$ is arbitrarily small, this is like throwing the ball from the top of the wall at $h_1$. Thanks for an amazing insight! I love it! – R P Feb 16 '16 at 14:11
• I first saw this question in the review section and decided to give the hint that the initial launch position and angle were variables. Then I clicked over here to answer, but alas, I was too late. Good work, but I think you did a little bit too much work for the the OP, :) . +1 anyway. – Bill N Feb 18 '16 at 4:25

Interesting question.

Here's an alternative approach using a symmetrical relationship involving launch and terminal velocities that I found, which helps simplify the solution.

Let $u,v,w$ be velocities at launch, at the first wall and at the second wall respectively. Let $k$ be the horizontal distance between the two walls. Hence $k^2=L^2-(h_2-h_1)^2$.

Squaring equation $(1)$ here (${v^*}{w^*}=gk$) for minimum velocities (omitting $^*$ for minimum velocities for clarity of notation) and using the standard energy conservation/kinematics formula $V^2=U^2+2AS$ gives

\begin{align} v^2w^2&=g^2k^2\\ (u^2-2gh_1)(u^2-2gh_2)&=g^2 \big(L^2-(h_2-h_1)^2\big)\\ u^4-2g(h_1+h_2)u^2+4gh_1h_2+g^2(h_2-h_1)^2&=g^2L^2\\ u^4-2g(h_1+h_2)u^2+g^2(h_1+h_2)^2&=g^2L^2\\ \big(u^2-g(h_1+h_2)\big)^2&=g^2L^2\\ u^2-g(h_1+h_2)&=gL\\ \text{Minimum launch velocity, }\;\;\;\;\;\;\color{red}u&\color{red}{=\sqrt{g(h_1+h_2+L)}} \end{align}

No trigonometric ratios or calculus.

Alternatively, using the results here, and omitting $^*$ for minimum velocities for clarity of notation, $${v}^2=g(L+H-h)\qquad$$ Using conservation of energy, \begin{align} {u}^2 &={v}^2+2gh\\ &=g(L+H-h)+2gh\\ &=g(L+H+h)\\ &=g(L+h_1+h_2)\\ \color{red}u&\color{red}{=\sqrt{g(h_1+h_2+L)}}\end{align}

The path of the projectile will be a parabola. Let $x$ be horizontal and $y$ be vertical. It is not obvious where to place the origin, so let it be at the peak of the parabola. Let the launch velocity be $v0$ and the launch angle above the horizontal be $\theta$. Then the horizontal velocity is constant as $x'=v0 \cdot \cos \theta$ and if we let the origin of time be when the projectile hits the peak we have $x=v0 \cdot \cos \theta \cdot t$. We also have $y=-\frac 12gt^2$ as at the origin of time we have $y=0, y'=0$ Combining these, the path is $y=-\frac 12 g(\frac x{v \cdot \cos \theta})^2$. You have four unknowns, $v0, \theta,$ and the $x,y$ of the launch point. You have two equations coming from the fact that the projectile just touches the top of each wall, one from the fact that it launches at the same $y$ as the base of the walls and one because the arrival point is opposite in $x$ from the launch point.

The space between the tops of the two walls can be thought of as an inclined plane. Then the problem is to find the minimum speed to cover distance $L$ on a plane inclined at $\theta$ to the horizontal where $L\sin\theta=h_2-h_1$. (I assume we are launching up the plane. However, the projectile can follow the same total trajectory in reverse with the same launch velocity from the ground, because the trajectory is symmetrical. So we can always arrange to launch up the inclined plane.)

The maximum range on an inclined plane is given by $$R=\frac{u^2}{g(1+\sin\theta)}$$ Using $R=L$ we get a minimum launch speed of $u$ given by $$u^2=g(L+h_2-h_1)$$ To obtain speed $u$ at height $h_1$ above the ground the stone must be launched with speed $v$ given by $$v^2=u^2+2gh_1$$ Therefore $$v^2=g(L+h_1+h_2)$$

Considering the movement origin at the top of $$h_1 \le h_2$$ and calling $$v_1^2 = v_x^2+v_y^2$$ the required initial velocity at this point, we have

$$\frac{v_y}{v_x}(x_2-x_1)-\frac 12 \frac{g}{v_x^2}(x_2-x_1)^2 = h_2-h_1$$

then

$$v_y = v_x\frac{h_2-h_1}{x_2-x_1}+\frac 12\frac{g}{v_x}(x_2-x_1)$$

but calling $$v_0$$ the ground initial velocity we have

$$v_0^2 = v_1^2+2h_1 g = v_x^2+\left(v_x\frac{h_2-h_1}{x_2-x_1}+\frac 12\frac{g}{v_x}(x_2-x_1)\right)^2+2h_1g$$

Finally calculating the minimum of $$v_0^2(v_x)$$ we obtain

$$v_0^2=\left(h_1+h_2+L\right)g$$