- #1
Roboto
- 13
- 1
I am working on modeling the acceleration and initial launch angle of an arrow shot from a bow during the power stroke. From an aiming point of view, the launch angle of the arrow doesn't change with respect to the target. But changing the nock position where the arrow nock attaches to the string does change where the arrow strikes the target. The nock position causes the arrow to pitch forward during the power stroke. It will acquire an angular rotation, and its vertical component of the initial velocity will be reduced.
I am using that actual measured force as a function of the draw length, and it is being assumed that the nock point is constrained and only moves/accelerates in the horizontal plane. The other assumption is that at the instant the arrow is loosed, there are no vertical supports holding the arrow in position, other that the nock end of the arrow on the string The nock point will set an initial angle of the arrow with respect to the horizontal plane. Intuition states that because of the initial angle present, the horizontal force on the end of the arrow will induce a torque into the arrow. As the arrow accelerates, the gravitational pull on the arrow also adds to the torque of the arrow.
When using the nock end as my reference. The angular acceleration becomes only a function of gravity.
Inertia*alpha=-r*m*at-m*g*cos(theta)
where Inertia is the inertia of the arrow. r is the distance from the nock to the center of gravity, m and the arrow mass, (at) is the tangential acceleration of the center of gravity relative to the nock end of the arrow, g is gravity, and theta is the angle of the arrow shaft with respect to the horizontal plane.
Then the summation of forces in the horizontal direction
m*ax=F(x)+m*r*omega^2*cos(theta)-m*r*alpha*sin(theta)
where ax is the horizontal acceleration, F(x) is the measured draw force as a function of x, omega is the angular velocity. Acceleration is the y direction (vertical) at the nock is zero since it is constrained from vertical movement. F(x) is non linear, and goes from 48 pounds to zero in 19 inches.
Intuition states that angular acceleration should also include the applied force. But it is dropping out. I think I am doing something wrong here. Thoughts, comments?
I am using that actual measured force as a function of the draw length, and it is being assumed that the nock point is constrained and only moves/accelerates in the horizontal plane. The other assumption is that at the instant the arrow is loosed, there are no vertical supports holding the arrow in position, other that the nock end of the arrow on the string The nock point will set an initial angle of the arrow with respect to the horizontal plane. Intuition states that because of the initial angle present, the horizontal force on the end of the arrow will induce a torque into the arrow. As the arrow accelerates, the gravitational pull on the arrow also adds to the torque of the arrow.
When using the nock end as my reference. The angular acceleration becomes only a function of gravity.
Inertia*alpha=-r*m*at-m*g*cos(theta)
where Inertia is the inertia of the arrow. r is the distance from the nock to the center of gravity, m and the arrow mass, (at) is the tangential acceleration of the center of gravity relative to the nock end of the arrow, g is gravity, and theta is the angle of the arrow shaft with respect to the horizontal plane.
Then the summation of forces in the horizontal direction
m*ax=F(x)+m*r*omega^2*cos(theta)-m*r*alpha*sin(theta)
where ax is the horizontal acceleration, F(x) is the measured draw force as a function of x, omega is the angular velocity. Acceleration is the y direction (vertical) at the nock is zero since it is constrained from vertical movement. F(x) is non linear, and goes from 48 pounds to zero in 19 inches.
Intuition states that angular acceleration should also include the applied force. But it is dropping out. I think I am doing something wrong here. Thoughts, comments?