MadSci Network: Physics |
Well, you may already know this, but the first thing I want to address is the common misuse of centrifugal force. Centrifugal force is an imaginary force that arises when you consider noninertial frames (an inertial frame would be one of a stationary observer). This concept can be best understood with an example - take a rock on a string. When you swing the rock in a circle, an observer in the inertial frame (like the person swinging the rock), would see a centripetal force (of F=ma) of the string acting on the rock to cause it to follow the line of the circle....and not fly off on a tangent. However to a person in the same reference frame as the swinging rock (don't ask me how the person got there! :-) ) sees the rock at rest and therefore has to invent a force to counteract the tension on the string and make all the the forces balance out.- the centrifugal force. (This is the same force that seems to pull you to the side when you make a sharp turn in a car......in reality, you are just lacking a force to pull you along the circle of the turn with the car.) For your answer, I will calculate the centripetal force. This may all seem nitpickey, but it is good to understand the true nature of the forces in a system. :::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::: Now to your real question........I thought about this question for a while (mostly because most of my general physics knowledge seems to have seeped from my brain) and I seem to have an answer for you. Applying what I have just explained above, I will attempt to calculate the centripetal force at the hub of a helicopter blade. If you just consider one side of the helicopter blade at a time, you can break down the system to something that can be solved with some simple calculus and physics equations (I sincerely hope you know calculus.....if not, email me back and I will try a simpler way of explaining it). First of all, the acceleration for any particle (we will start small) moving in a circle can be described by the the equation: a = -(v^2)/r (where 'v' is the particle's velocity, and 'r' is the radius of the particle from the centre of motion) Combine this with Newton's Second Law (or F=ma) and you get the centripetal force acting on the particle: F = (mv^2)/r (where 'm' is the mass of the particle). (Note: the acceleration equation was negative because the motion is directed inward; the force is also inward, but we will not bother carrying the negative sign) This last equation is what we need to solve your question. The only problem now is that we have a radius to deal with. First of all, sub in the following equivalent equation for 'v': v = (RPM*2*pi*r)/(60 s/min) where, RPM = the revolutions per minute of the blade pi = 3.14 r = radius of the part being calculated from the hub 60 s/min = a conversion factor to get the result in terms of seconds The equation you now have (after substitution and reduction) is: F = 4*m*r*(pi*RPM/60)^2 If you integrate over the length of the one half of the helicopter blade (i.e. from the hub to one of the tips - we will call the limits 'a' and 'b'), you can derive a general equation for the centripetal force: F = 2m*(pi*RPM / 60 s/min)^2 * (b^2 - a^2) The above equation, as promised, should give you an expression to describe the centripetal force of one blade of a helicopter (from the centre to the tip) on the hub - just sub in the limits of the start of the blade and the tip for 'a' and 'b' respectively, sub in for the mass of the blade and solve. The opposite blade will have the same force, but in the opposite direction. :::::::::::::::::::::::::::::::::::::::::::::::::::: I hope this answers your question for you. It was hard trying to express these calculus and physics equations on the computer without resorting graphics. If you need any further explanation of this answer, please feel free to email me. You might also want to refer to a good physics text for further explaination....I listed the one I used below. Kurt Frost kfrost@sympatico.ca REFERENCES: Benson, H. 1991. University Physics. New York: John Wiley & Sons, Inc.
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