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Tuesday, November 29, 2011

The Magnus Force



The Magnus effect, demonstrated on a ball. v represents the wind velocity, the arrow F the resulting force towards the side of lower pressure. (from: wikipedia)


The Magnus effect is the phenomenon whereby a spinning object flying in a fluid creates a whirlpool of fluid around itself, and experiences a force perpendicular to the line of motion.
In fluid dynamicsBernoulli's principle states that for an inviscid flow, an increase in the speed of the fluid occurs simultaneously with a decrease in pressure or a decrease in the fluid's potential energy. But it doesn't mention the effect when an object is spinning through a fluid (that's what happened in Magnus effect), that has an incremental energy due to the spinning object.


Principle

When a body (such as a sphere or circular cylinder) is spinning in a viscous fluid, it creates a boundary layer around itself, and the boundary layer induces a more widespread circular motion of the fluid. One explanation of the Magnus effect is since there is more (forward) acceleration of air on the forward-moving side than the backward-moving side, there is more pressure on the forward-moving side, resulting in a perpendicular component of force from the air towards the backward-moving side (watch the video bellow).

\begin{figure}
\epsfysize =2.75in
\centerline{\epsffile{magnus.eps}}
\end{figure}

Calculation of Magnus force

Given the angular velocity vector \vec{\omega} and velocity \vec{v} of the object, the resulting force \vec{F_M} can be calculated using the following formula:

\vec{F_M} = S (\vec{\omega}\times\vec{v})
where S is dependent on the average of the air resistance coefficient across the surface of the object.[8] The \times denotes the vector cross product.


An example of spin ball in the air

The following equation demonstrates the lift force induced on a ball that is spinning along an axis of rotation perpendicular to the direction of its translational motion:
{F}=\frac{1}{2} \rho  v^2 A C_L
F = lift force
ρ = density of the fluid
r = radius of the ball
v = velocity of the ball
A = cross-sectional area of ball
CL = lift coefficient
The lift coefficient CL may be determined from graphs of experimental data using Reynolds numbers and spin ratios.[9] For a smooth ball with spin ratio of 0.5 to 4.5, typical lift coefficients range from 0.2 to 0.6.




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