Differential equation: projectiles

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SUMMARY

The discussion focuses on deriving the equation of motion for a projectile projected vertically upwards with an initial speed U, experiencing a resistive force proportional to the square of its velocity, represented by mkv². The derived equation of motion is dv/dt = -(g + kv²), where g is the acceleration due to gravity. The subsequent differential equation for velocity as a function of height z is v dv/dz = -(g + kv²), which integrates to yield the maximum height reached by the projectile as z = (1/2k) ln((g + kU²)/g). The solution confirms the behavior of the projectile under the influence of air resistance.

PREREQUISITES
  • Understanding of Newton's second law of motion
  • Familiarity with differential equations
  • Knowledge of integration techniques
  • Concept of resistive forces in physics
NEXT STEPS
  • Study the effects of air resistance on projectile motion
  • Learn about the integration of differential equations in physics
  • Explore the concept of terminal velocity in resistive motion
  • Investigate variations in projectile motion with different initial conditions
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mattgad
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Homework Statement



A projectile of mass m is projected vertically upwards with speed U. In addition to its
weight it experiences a resistive force mkv^2, where v is the speed at which the projectile is moving and k is a constant.
Derive the equation of motion of the projectile:

dv/dt = -(g + kv^2)

Derive a differential equation for v as a function of z, where z is the height of the projectile above its starting position. Solve this equation to find the maximum height reached by the projectile.

The Attempt at a Solution



F = ma = m dv/dt

-mg - mkv^2 = m dv/dt

dv/dt = -g - kv^2 = -(g + kv^2)

dv/dt = dv/dz * dz/dt = v dz/dt

v dv/dz = -(g + kv^2)

[v/(g+kv^2)] dv = - dz

Integrating:

1/2k ln(g + kv^2) = -z + C

ln(g + kv^2) = -2kz + 2kC

When v = U, z = 0, 2kC = ln(g + kU^2)

ln(g + kv^2) = -2kz + ln(g + kU^2)

2kz = ln([g+kU^2]/[g+kv^2])

Maximum z is when v = 0.
z = 1/2k ln((g + kU^2)/(g)) = 1/2k ln(1 + kU^2/g)

Is this correct?

Thankyou.
 
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Seems OK. Note that this is the eqn when the projectile is going up. When it's falling back, the eqn would be slightly different, because of the v^2 dependence of acceleration, unlike projectile motion without air resistance.
 

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