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Mathematically, how would air resistance affect trajectory?
Suppose I shoot a cannonball with initial velocity [itex]v_0[/itex] at an angle of elevation [tex]\theta[/tex]. Air resistance is a force antiparallel to velocity, represented by the equation (according to Barron's Physics C review book!) [itex]\vec F_{air} = - c \cdot \vec v[/itex], where [itex]c[/itex] is a constant SI-expressed in kg/sec.
Because the direction of velocity changes with [itex]t[/itex], so does, as well, the direction of air resistance. To represent its effect in the x & y directions, let [itex]\alpha[/itex] represent the instantaneous angle that [itex]\vec v[/itex] makes with the x-axis. Thus, using 2D Cartesian, I represent the velocities as
[tex]\left\{ \begin{gathered} \vec v_x = \left| {v_0 } \right|\cos \theta - t\left( {c \cdot \vec v} \right)\cos \alpha \hfill \\<br /> \vec v_y = \left| {v_0 } \right|\sin \theta - t\left( {\vec g + c \cdot \vec v \cdot \sin \alpha } \right) \hfill \\ \end{gathered} \right\}[/tex]
*But how do I find y(t) and x(t) ?
?
Suppose I shoot a cannonball with initial velocity [itex]v_0[/itex] at an angle of elevation [tex]\theta[/tex]. Air resistance is a force antiparallel to velocity, represented by the equation (according to Barron's Physics C review book!) [itex]\vec F_{air} = - c \cdot \vec v[/itex], where [itex]c[/itex] is a constant SI-expressed in kg/sec.
Because the direction of velocity changes with [itex]t[/itex], so does, as well, the direction of air resistance. To represent its effect in the x & y directions, let [itex]\alpha[/itex] represent the instantaneous angle that [itex]\vec v[/itex] makes with the x-axis. Thus, using 2D Cartesian, I represent the velocities as
[tex]\left\{ \begin{gathered} \vec v_x = \left| {v_0 } \right|\cos \theta - t\left( {c \cdot \vec v} \right)\cos \alpha \hfill \\<br /> \vec v_y = \left| {v_0 } \right|\sin \theta - t\left( {\vec g + c \cdot \vec v \cdot \sin \alpha } \right) \hfill \\ \end{gathered} \right\}[/tex]
*But how do I find y(t) and x(t) ?
?
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