Projectile subject to air resistance

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SUMMARY

The discussion focuses on the mathematical modeling of a projectile subject to air resistance, defined by the drag force equation F=-v C v^{a}. The problem is constrained to two dimensions, with initial conditions set at the origin. The dimensionless coordinates X, Y, and T are introduced to simplify the equations of motion, leading to the second-order differential equations for Y and X. The participants clarify the derivation of these equations, emphasizing the correct application of derivatives in the context of projectile motion.

PREREQUISITES
  • Understanding of classical mechanics, specifically projectile motion.
  • Familiarity with differential equations and their applications in physics.
  • Knowledge of dimensionless analysis and coordinate transformations.
  • Proficiency in calculus, particularly in taking derivatives and integrals.
NEXT STEPS
  • Study the derivation of the drag force in fluid dynamics, focusing on the implications of the constants C and a.
  • Explore the application of dimensionless variables in simplifying complex physical equations.
  • Learn about numerical methods for solving second-order differential equations, particularly in the context of projectile motion.
  • Investigate the effects of varying the exponent 'a' in the drag force equation on projectile trajectories.
USEFUL FOR

This discussion is beneficial for physics students, educators, and researchers interested in the dynamics of projectile motion and the effects of air resistance on trajectories.

rg2004
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Homework Statement



Consider a projectile subject to air resistance. The drag force is F=-\hat{v} C v^{a} where C and a are constants and v=\dot{r}. Restrict the problem to 2-D and take y in the vertical direction. Take the magnitude of initial velocity to be v_{0} and the initial position to be the origin. Introduce dimensionless coordinates X,Y,Z by relations

x=\frac{v_{0}^{2}}{g}X
y=\frac{v_{0}^{2}}{g}Y
t=\frac{v_{0}}{g}T

Given the above definitions show that

\frac{d^2Y}{dT^2}=-1-k V^{a-1} \frac{dY}{dT}
\frac{d^2X}{dT^2}=-k V^{a-1} \frac{dX}{dT}

where k=\frac{C v_{0}^a}{m g}

V=\sqrt{(\frac{dY}{dT})^2+(\frac{dX}{dT})^2}

The Attempt at a Solution

x=\frac{v_{0}^{2}}{g}X
dx=\frac{v_{0}^{2}}{g}dX

y=\frac{v_{0}^{2}}{g}Y
dy=\frac{v_{0}^{2}}{g}dY

t=\frac{v_{0}}{g}T
dt=\frac{v_{0}}{g}dT

finding d?/dT equations
\frac{dx}{dt}=\frac{\frac{v_{0}^{2}}{g}dX}{\frac{v_{0}}{g}dT}<br /> =v_0\frac{dX}{dT}<br />

\frac{dy}{dt}=\frac{\frac{v_{0}^{2}}{g}dY}{\frac{v_{0}}{g}dT}<br /> =v_0\frac{dY}{dT}<br />

finding \frac{d^2?}{dT^2}
\frac{d^2x}{dt^2}=\frac{dx}{dt}\frac{dx}{dt}=v_0^2\frac{d^2X}{dT^2}

\frac{d^2y}{dt^2}=\frac{dy}{dt}\frac{dy}{dt}=v_0^2\frac{d^2Y}{dT^2} From force equation:
F_{d,x}=m \ddot{x}=-\hat{v} C v^{a}=\frac{-\dot{x}}{\sqrt{\dot{x}^2+\dot{y}^2}} C (\sqrt{\dot{x}^2+\dot{y}^2})^{a}
=-\dot{x} C \sqrt{\dot{x}^2+\dot{y}^2}^{a-1}m v_0^2\frac{d^2X}{dT^2}=-(v_0\frac{dX}{dT}) C \sqrt{(v_0\frac{dX}{dT})^2+(v_0\frac{dY}{dT})^2}^{a-1}

m v_0^2\frac{d^2X}{dT^2}=-v_0^a \frac{dX}{dT} C \sqrt{(\frac{dX}{dT})^2+(\frac{dY}{dT})^2}^{a-1}

\frac{d^2X}{dT^2}=-\frac{v_0^a C}{m v_0^2} V^{a-1} \frac{dX}{dT}

\frac{d^2X}{dT^2}=-k \frac{g}{v_0^2} V^{a-1} \frac{dX}{dT}
Which is not what I'm supposed to get. I must be messing up a rule or two somewhere.

Thank you.
 
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rg2004 said:
finding d?/dT equations
\frac{dx}{dt}=\frac{\frac{v_{0}^{2}}{g}dX}{\frac{v_{0}}{g}dT}<br /> =v_0\frac{dX}{dT}<br />

\frac{dy}{dt}=\frac{\frac{v_{0}^{2}}{g}dY}{\frac{v_{0}}{g}dT}<br /> =v_0\frac{dY}{dT}<br />

finding \frac{d^2?}{dT^2}
\frac{d^2x}{dt^2}=\frac{dx}{dt}\frac{dx}{dt}=v_0^2\frac{d^2X}{dT^2}

\frac{d^2y}{dt^2}=\frac{dy}{dt}\frac{dy}{dt}=v_0^2\frac{d^2Y}{dT^2}

Do the second derivatives again. They are not the squares of the first derivatives, as you wrote.

ehild
 
So then would the derivative be

\frac{d^2x}{dt^2t}=\frac{d}{dt}\frac{dx}{dt}=\frac{d}{dt}(v_0 \frac{dX}{dT})=\frac{d}{dT}(\frac{g}{v_0})(v_0 \frac{dX}{dT})

\frac{d^2x}{dt^2}=g\frac{d^2X}{dT^2}

similarly

\frac{d^2y}{dt^2}=g\frac{d^2Y}{dT^2}

Thanks for your help
 

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