He is trying to prove the opposite.
Going to be a tough one if that is the case.
So how's life Amone?
Edit: or should I say stubborn ass?
He is trying to prove the opposite.
I find several problems. In the first post, accln was 10 ms^-2, which I assume is an approximation to 9.8. Why would g be the acceleration of a horizontal ball?
Second problem is linear motion formulas are being used while the racquet tip motion is an arc.
Thirdly, in these calculations, moment of inertia and angular accln need to be used, as the racquet and ball are not point masses at this intimate scale of contact.
Something is quite not right. Very HL racquets don't put much mass behind the ball, so I don't think they are good for baseline topspin shots. Quite opposite to your results.
What are you talking about? My results showed that a racquet with a lower balance was less powerful. I think you are agreeing with me and just confused. Maybe I'm misreading.
This effect at high swingweight is mostly due to the increase in racquet velocity (much like adding a mass near the pivot of a metronome increases the oscillation frequency).
The metronome example cannot be right. There is no way that ADDING mass/inertia to something is going to increase it's velocity.
and an extra question: what university degree category does this stuff fall into? eg. engineering or physics
The laws of physics tell us that adding mass near the pivot point of a physical pendulum does in fact increase its velocity.
At low swingweight (~330), the racquet velocity depends mostly on how fast a player tries to swing the racquet. But this is not true at higher swingweights.
A racquet at high swingweight (~370) behaves on a groundstroke much like a physical pendulum, with a natural swing frequency that is almost independent of the strength of the player (but dependent on the length of the player's arm). Let's do the math now.
The formula for the frequency of a pendulum:
F = 1/(2*pi*sqrt(I/(m*g*L)))
F = frequency
I = moment of inertia about axis of rotation
m = mass
g = acceleration of gravity
L = distance between center of mass and axis of rotation
If a racquet has a swingweight of 370 kg-cm^2, a mass of 360g, a balance R of 33 cm, and the axis of rotation is 20 cm beyond the butt, then by the parallel axis theorem:
I = 370 + 0.360*(2*(33 - 10)*(20 + 10) + (20 + 10)^2) = 1191 kg-cm^2
g = 980 cm/s^2
L = 20 + 33 = 53 cm
F = 1/(2*pi*sqrt(1191/(0.360*980*53))) = 0.6306 Hz
Now add 10g to the handle at 1 cm from the butt.
New specs:
I = 1191 + 0.010*(20 + 1)^2 = 1195 kg-cm^2
m = 360 + 10 = 370g
R = (33*360 + 1*10)/370 = 32.14 cm
L = 20 + 32.14 = 52.14 cm
F = 1/(2*pi*sqrt(1195/(0.370*980*52.14))) = 0.6330 Hz
0.6330/0.6306 = 1.004
So adding 10g to the butt of the racquet with these specs increases the angular velocity by approximately 0.4%. This doesn't sound like much, but this change in swing velocity has an effect on the power level that is on the same order as changing string tension by a few pounds. You will definitely notice it.
The laws of physics tell us that adding mass near the pivot point of a physical pendulum does in fact increase its velocity.
At low swingweight (~330), the racquet velocity depends mostly on how fast a player tries to swing the racquet. But this is not true at higher swingweights.
A racquet at high swingweight (~370) behaves on a groundstroke much like a physical pendulum, with a natural swing frequency that is almost independent of the strength of the player (but dependent on the length of the player's arm). Let's do the math now.
The formula for the frequency of a pendulum:
F = 1/(2*pi*sqrt(I/(m*g*L)))
F = frequency
I = moment of inertia about axis of rotation
m = mass
g = acceleration of gravity
L = distance between center of mass and axis of rotation
If a racquet has a swingweight of 370 kg-cm^2, a mass of 360g, a balance R of 33 cm, and the axis of rotation is 20 cm beyond the butt, then by the parallel axis theorem:
I = 370 + 0.360*(2*(33 - 10)*(20 + 10) + (20 + 10)^2) = 1191 kg-cm^2
g = 980 cm/s^2
L = 20 + 33 = 53 cm
F = 1/(2*pi*sqrt(1191/(0.360*980*53))) = 0.6306 Hz
Now add 10g to the handle at 1 cm from the butt.
New specs:
I = 1191 + 0.010*(20 + 1)^2 = 1195 kg-cm^2
m = 360 + 10 = 370g
R = (33*360 + 1*10)/370 = 32.14 cm
L = 20 + 32.14 = 52.14 cm
F = 1/(2*pi*sqrt(1195/(0.370*980*52.14))) = 0.6330 Hz
0.6330/0.6306 = 1.004
So adding 10g to the butt of the racquet with these specs increases the angular velocity by approximately 0.4%. This doesn't sound like much, but this change in swing velocity has an effect on the power level that is on the same order as changing string tension by a few pounds. You will definitely notice it.
What about calculating the length of the arm? would it be lower swingweights for longer arms and higher swinweights for shorter? or vice versa?