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Re: Engineering Challenge- Spring Loaded Kicker Edition
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#2
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Re: Engineering Challenge- Spring Loaded Kicker Edition
I would go with D; it would mean less momentum and energy loss due to friction on the way down. Assuming! that the kicker was put together by a bunch of monkeys (I'm a programmer), it might just have too much friction loss to get 100% effiiciency from the spring.
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Re: Engineering Challenge- Spring Loaded Kicker Edition
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#4
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Re: Engineering Challenge- Spring Loaded Kicker Edition
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1) Assuming that both the strong spring and the weak spring have the same pre-load force, then the weak spring will be pulled back further and have more stored energy. or 2) Assuming you increase the pre-load on the weaker spring just enough that the motor stalls at the same position as the strong spring, you will also have more stored energy in the weaker spring. If you have trouble believing this, make a simple graph of force versus distance for each case and look at the area under the curve. ~ |
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#5
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Re: Engineering Challenge- Spring Loaded Kicker Edition
In short: make the kicker lighter, it will more efficiently transfer momentum to the soccer ball
I like to look at these sorts of problems holistically. Your motor can only put out a certain force and your kicker can only retract a certain distance, so you have a maximum amount of energy you can store in the springs. EDIT: Lowering the spring rate *might* help if you can work out all the details, i.e. fit a spring on that will get you a greater amount of stored energy, K*x^2. Constant-force springs would be an interesting option to explore, they would allow you to maximize the energy extracted from the motor by keeping it under a higher constant load, rather than a progressive load as shown in Ether's plot. When considering elastic impacts I found through momentum calculations that for the same amount of applied energy (Force*distance or torque*swept angle) it was beneficial to decrease the mass/inertia of the kicker to improve kicking distance. If you need a 10% increase in range you might need to decrease your kicker's inertia by ~10% but I cannot give you exact numbers without knowing details about your kicker. This is a good simple paper explaining basic physics behind kicking a soccer ball: http://www.serioussoccer.net/Documen...csofSoccer.pdf Last edited by JamesCH95 : 25-03-2010 at 11:53. |
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#6
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Re: Engineering Challenge- Spring Loaded Kicker Edition
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If you run some numbers with Va = 0 and Vb = 1, and the coefficient of restitution equal to 1 in the equation given at Wikipedia, you will find that equal masses of the two objects will result in perfect momentum transfer. I'm going to go out on a limb and guess that since our kickers are swinging around an axis, what you really want is equal moments of inertia around the axis for perfect energy transfer. |
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#7
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Re: Engineering Challenge- Spring Loaded Kicker Edition
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#8
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Re: Engineering Challenge- Spring Loaded Kicker Edition
Mass of a kicker is important to a point. the kicker and the ball need to be in the same order of magnitude otherwise there are different governing equations.
Think of it in terms of tiny mass or really big masses. The ball itself weighs about 0.5kg or roughly 1.25 lbs. If your kicker is really light. Like 1.25 OZ. then in order to impart the kinetic energy needed on the ball it will need to go at sqrt(16) or 4 times the speed. This is really fast. If we go a step further, then say about 1/16th of an ounce, then it would need to be another 4x of 16x faster. For something this light, it would have to go really fast and might puncture the ball. Thus more surface area would be required, and it would loose a lot to areo losses before striking the ball. Now go the other extreme. Say you use a 16 lbs sledge hammer. From an energy standpoint, you would only need to go 1/4 the speed for the ball, but in this senraio you would likely just push the ball instead and not get a big kick out of it. Too little and it is difficult to store and transmit enough kinetic energy. Too massive and it is difficult to get the mass up to an effective speed. |
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#9
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Re: Engineering Challenge- Spring Loaded Kicker Edition
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A large contact area on the ball is also important for good momentum transfer, large deformations of the ball result in lost energy, so a big striking surface is probably better than a small one, in general. I would imagine your small thin piece of metal was not very stiff, again a very inefficient way to transfer momentum because the kicker will deform and absorb energy. Things designed to transfer momentum like pool balls and sledge hammers are all very stiff. Quote:
Any kicker of reasonable design (i.e. not a giant flat board) would have to be traveling incredibly fast to see any sort of significant aerodynamic losses, I would consider them negligible for any design. Final point is again correct, but I feel that as long as the kicker is stiff enough (ours is 4130 steel tubing) then faster is better. IIRC the PGA has banned the use of certain clubs that are super-light and have extra-hard striking faces because they can drive a golf ball significantly further than a softer, heavier club. |
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#10
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Re: Engineering Challenge- Spring Loaded Kicker Edition
Assuming a COR != 1, we get that the kicker should weigh M_ball / COR. What ever initial conditions exist, it is trivial to find a mass of the kicker that will result in the kicker transferring all it's energy to the ball. And for most sane initial conditions, you will want the masses to be within a factor of 2 of each other.
I've been thinking about this for a while, and this post finally got me to sit down and derive what happens when the kicker is spinning and hits a ball. Something bugged me about using equations derived for linear impacts when modeling something that is swinging. Lets start with the assumption that angular momentum is conserved. I_a w_a + I_b w_b = I_a w'_a + I_b w'_b Then define an "angular coefficient of restitution" that's similar to the coefficient of restitution for linear collisions. -w'_a + w'_b = COR (w_a - w_b) Solving the linear system of equations gets us that w'_a = (I_a w_a + I_b w_b + I_b COR (w_b - w_a)) / (I_a + I_b) w'_b = (I_b w_b + I_a w_a + I_a COR (w_a - w_b)) / (I_a + I_b) So, when a rotating kicker is hitting something, we want the moments of inertia to be similar. Or, if the COR isn't one, then the moment of inertia of the kicker should be I_ball / COR, where I_ball is the moment of inertia of the ball around the axis that the kicker spins around. Very similar to the original billiard ball case. Our small piece of metal was the end of one of the old IFI frames that looked like a U. So, it was a ~1/2 lb quite stiff piece of aluminum that had about a 4" radius. It's moment of inertia around the kicker axis would have been quite a bit lower than the ball's around the kicker axle, resulting in a shortened kick distance because the kicker would bounce off the ball instead of kicking it. Which is consistent with what we observed. |
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#11
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Re: Engineering Challenge- Spring Loaded Kicker Edition
Alright, I've seen enough answers that I think are wrong to make begin to wonder if it is me that's wrong so here's what I got:
To get the farthest kick we want to impart the maximum kinetic energy on the ball. Assuming all the potential energy in the spring is converted to kinetic energy when firing, this means we want to maximize the potential energy stored in the spring. F=kx E = 1/2*kx*x F in this case is the max motor force which is constant, therefore kx is constant. If kx is constant then E is proportional to x, therefore we want to maximize x. Going back to the first equation we now know F (the max force the motor can apply to the spring based on gearing and lever arm) and X (the max spring extension before reaching the mechanical limits) so we can solve for k. For x to increase, k will have to decrease so my answer is B, less spring rate. Last edited by Vikesrock : 24-03-2010 at 20:19. |
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#12
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Re: Engineering Challenge- Spring Loaded Kicker Edition
Ok, in case this is stumping anyone this weekend, I will put my thoughts down in White:
So with the spring loaded kickers, most need a mechanical endstop to avoid penalty. Because of this, the ball will tend to follow a given trajectory. If you use trajectory physics, you can calculate the given distance if you know a couple parameters for this problem, ball speed and angle would give you distance. How? and How is velocity related to the distance? Well the lateral distance covered will be equal to the time in flight multiplied by the lateral component of the ball velocity. The time in flight is dictated by the vertical component of the ball velocity. Since gravity only slows the vertical component, 1/2*t=Vy/g with g being the gravity constant. Therefore the distance (d) traveled is d=Vx*t=Vx*2*Vy/g. This means that really distance is proportional to a constant (c) multiplied by the square of the velocity (since Vx and Vy have a constant relationship). Thus d is proportions to V^2. So how do we find V? Well 1/2mV^2 is the kinetic energy imparted on the ball by the kicker. Where does this energy come from? The spring. Thus the spring energy 1/2K*x^2 is directly proportional to the ball kinetic energy 1/2*mV^2. From this we realise we want to maximize the kinetic energy. Now for this particular problem, as many have noticed, the motor stalls thus it is torque limited thus Kx (spring force) is maximized. As we have seen though, energy is really what we are looking for. lets assume both K = 2 and X = 1 Then the energy stored is 1/2K*x^2=1/2*2*1^2=1 Now if we reduce the spring rate and hold the force constant Kx so that K = 1 and X = 2 then 1/2*1*2^2=4/2=2. We actually doubled the energy going into the kicker. This assumes though that you have the extra travel. what if you don't have the extra travel? Can weaker springs still give you more energy? Initially you would say no, if they both pull the same distance, then the stronger spring should store more energy. This assumes no preload though! so back to our earlier example. K=2 and X=1 gives us an energy of 1. Now with k =1, X can equal 2, but there isn't enough room. therefore we pre-stretch the spring so that it ends up with a total stretch of 2. Thus the energy for that is E= 1/2*K*(x2)^2-1/2*k*(x1)^2 where x2=2 and x1=1 thus E=1/2*k*(x2^2-x1^2) or E= 1/2*1*(2^2-1^2)=3/2 thus even in a restricted space, we still have 50% more energy with the weaker spring rate. So my answer is B sometimes with springs, less rate is more. Good luck to the teams competing this weekend. |
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#13
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Re: Engineering Challenge- Spring Loaded Kicker Edition
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Re: Engineering Challenge- Spring Loaded Kicker Edition
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#15
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Re: Engineering Challenge- Spring Loaded Kicker Edition
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