Maximum Range for Projectile Motion

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SUMMARY

The maximum range for projectile motion on an inclined plane is defined by the formula R = (2u²/g)cos(θ)sin(θ - α)sec²α, where u is the initial velocity and θ is the angle of projection. The maximum range occurs when sin(2θ) = π, leading to R_max = (u²/g)(cosα - sinα)sec²α. Differentiation of the range function R with respect to θ yields dR/dθ = (2u²sec²α/g)(cos(2θ)cosα + sin(2θ)sinα). The discussion highlights the importance of understanding trigonometric identities in deriving maximum values.

PREREQUISITES
  • Understanding of projectile motion principles
  • Familiarity with trigonometric identities
  • Knowledge of differentiation techniques in calculus
  • Basic physics concepts related to motion on inclined planes
NEXT STEPS
  • Study the derivation of projectile motion equations
  • Learn about trigonometric identities and their applications
  • Explore advanced differentiation techniques in calculus
  • Investigate the effects of angle and velocity on projectile range
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Students and educators in physics, mathematicians focusing on calculus, and engineers involved in motion analysis will benefit from this discussion.

John O' Meara
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The range of a particle from a point on a plane which is inclined at an angle alpha to the horizontal is given by R=\frac{2u^2}{g}\cos\theta\sin(\theta-\alpha)\sec^2 \alpha \\, where the velocity of projection is u at an angle theta to the horizontal. Using the trigonometrical identity 2cosAsinB=sin(A+B), find the maximum value of R as theta varies. Verify your result by differentation.(a)
R=\frac{u^2}{g}(\sin(2\theta-\alpha)-\sin\alpha)\sec^2 \alpha\\. Maximum range for a given velocity of projection: since \sin(\pi- \theta) = \cos\theta \\. Therefore the same values of R will be obtained whether the angle of projection is theta or pi-theta. Although the range will be the same for both angles, the time taken and height will be different. R is greatest when \sin2\theta = \pi \mbox{ therefore }\\ R_{max} = \frac{u^2}{g}(\sin\pi-\alpha \ - \ \sin\alpha)\sec^2 \alpha \\ \mbox{which } =\frac{u^2}{g}(\cos\alpha - \sin\alpha)\sec^2 \alpha\\.
(b) I get \frac{dR}{d\theta} = \frac{2u^2\sec^2 \alpha}{g}(\cos2\theta \cos\alpha +\sin2\theta\sin\alpha) \\. I think my reasoning is wrong in part (a), please show me where I'm wrong. Thanks.
 
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sin(A+B) = sinAcosB + cosAsinB... not 2sinAcosB
 

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