Part of JME-01 — Kinematics: Rectilinear & Projectile Motion

Projectile Trajectory Equation

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Standard form: y = xtan(theta) - gx^22u2cos2(theta\frac{2}{2u^2*cos^2(theta})

Alternative form using Range: y = x*tan(theta)(1 - x/R) where R = u2u^2*sin2thetag\frac{2*theta}{g}

This form is elegant because:

  • At x = 0: y = 0 (launch point) ✓
  • At x = R: y = 0 (landing point) ✓
  • At x = R/2: y = R4\frac{R}{4}*tan(theta) = H (maximum height) ✓

Radius of curvature at highest point: At the top, v = ucos(theta), centripetal acceleration = g rtopr_{top} = v2v^2/g = u2u^2cos^2$$\frac{theta}{g}

Radius of curvature at launch: rlaunchr_{launch} = u^2gcos(theta\frac{2}{g*cos(theta}) [velocity is u, component of g perpendicular to v is g*cos(theta)]

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