Tension in massless rope 
We are learning Newton laws in the University and were given the following problem: In the system described in the image, the man is pulling two massless ropes with a force of $F$ each. We are required to calculate the acceleration of the system.
Given $m_1$ - mass of the man, $m_2$ - mass of the platform, I thought the solution will simply be:
$$
(m_1 + m_2)a = -(m_1 + m_2)g + 2F \rightarrow a = \frac{2F}{(m_1 + m_2)} - g
$$
But apparently the answer is:
$$
a = \frac{4F}{(m_1 + m_2)} - g
$$
And I can't quite wrap my head around how the force the man put essentially "doubled". I was given an answer of how the tension in the rope needs to be uniform through the entire rope - so with accordance with Newton second law each rope is pulling the man upwards in equal force, but also the bottom of the rope pulls up the platform in an equal force, so it adds up to $4F$.
I was hoping you could help me make sense of this problem because it doesn't sit well with me.
 A: That's one thing that you can make a pulley do. There is no "conservation of force", so systems like pulleys and levers can increase or decrease applied forces.  The increased effect of and applied force by a machine is termed mechanical advantage. Because the work done is conserved, that means if a pulley changes the force required, the distance moved by the rope system changes as well.
In this problem the person on the platform is pulling each rope with a force $F$, for a total by the person of $2F$.  And we can assume that if the system is moving, the rope is pulled some length $l$ past the grip point.
Because each rope has two attachments to the platform (one fixed, one via the person), the force delivered to the platform system is $4F$.  But as the platform moves, both ends get closer to the pulley.  So by the person pulling a length $l$, the platform rises a distance $l/2$.
If we ignore the acceleration and assume the person is just lifting slowly, then the total work done by the person is $W = Fd = 2F l$, while the work done on the platform is $4F\frac{l}{2} = 2Fl$.  The pulley system has changed the force required to move the platform, but not changed the work required.
A: Think of the scenario where the two ropes at the ends are fixed to the pulleys (so they don't roll) and the person is not holding on to the ropes. In this case, the two ropes each have a force $|F_1| = g(m_1+m_2)/2$ applied to them, and by Newton's third law, each applies $|F_1|$ to the platform.
Then, instead of fixing the two ropes to the pulleys, attach both ends of each rope to the platform (the person is still not holding onto the ropes in the middle, they are just directly attached to the platform). Then, each rope end must have $|F_2| = g(m_1+m_2)/4$ applied to it, and by Newton's third law, each applies $|F_2|$ to the platform.
Let's say all ends of the ropes are still attached to the platform, but the person decides to pull down on the two rope ends in the middle, such that the force on each of the two rope ends in the middle is $F$.
What is the force that the two middle rope ends exert on the person?
What is the force that the other two ends of the rope exert on the platform?
Then, what is the total force exerted on the platform+person system by the ropes?
A: Each rope is pulling up on the man and on an end of the platform.
A: The tension in each rope the man is pulling is $F$ upwards.  For massless pulleys as well as massless ropes, the tension in the left rope is $F$ everywhere and the tension in the right rope is $F$ everywhere.  At the ends of the platform, the rope on the left pulls up due to tension with $F$, and the rope on the right pulls up due to tension with $F$.  The net force upward on the man and platform from the four ropes (the two the man is pulling plus the two ropes at the ends of the platform) is $4F$.  The force down on the mass plus platform is $(m_1 + m_2)g$.  The difference between the up and down net forces is the total mass times the acceleration; this gives you the correct answer.
This arrangement using pulleys is a "rotary lever", the rotary analog of a beam on a fulcrum. A lever allows a smaller force to create a larger force.  Look for a discussion of "level physics" on the web.
