Solving Non-Linear Differential Equations for Free Fall Due to Gravity

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SUMMARY

The discussion focuses on solving non-linear differential equations related to free fall due to gravity, specifically addressing the equations dv/dt = -g - kv and z'' + kz' + GMz^-2 = 0. The user initially attempts to solve the second-order differential equation but encounters difficulties when applying the First Shift Theorem due to the non-exponential form of the right-hand side. The conversation emphasizes the need to transform the first-order equation for velocity and find an integrating factor to make the equation exact for successful resolution.

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  • Understanding of non-linear second-order differential equations
  • Familiarity with gravitational concepts, including the gravitational constant (G) and mass of the Earth (M)
  • Knowledge of differential operators and their applications in solving equations
  • Proficiency in integrating factors and exact equations in differential calculus
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  • Study the application of integrating factors in differential equations
  • Explore the concept of exact equations and conditions for their applicability
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Pete69
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Homework Statement



I was given a problem to solve for the speed of a body falling under gravity [equation (1)] where g is acceleration due to gravity, which was easy enough.. but then i thought i would extend it to the case where g is non-constant, and so arrived at equation (2), (where where z is the height above Earth [z'=dz/dt and z=dv/dt and z^-2 means z to power -2], and M is the mass of the Earth and G is the gravitational constant)

Homework Equations



(1) : dv/dt = - g - kv

(2) : z'' + kz' + GMz^-2 = 0

The Attempt at a Solution



I believe this is a non-linear second order DE?? i attempted to solve by setting

z'' + kz' = 0

and solving the complimentary equation, which was OK, but when i came to solve for the particular integral

z'' + kz' = -GMz^-2

i ran into problems, as after substituting in the D and Q operators (http://silmaril.math.sci.qut.edu.au/~gustafso/mab112/topic12/ ), i could not use the First Shift Theorem, as the RHS is not in an exponential form...

Any ideas anyone?
 
Last edited by a moderator:
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Pete69 said:
I believe this is a non-linear second order DE?? i attempted to solve by setting

Yes, but rather than get into that let's look at your first order equation for [itex]v[/itex].

Do the following.

1.) Show that [itex]\frac{dv}{dt}=v\frac{dv}{dz}[/itex].
2.) Insert [itex]g=\frac{GM}{z^2}[/itex] into the equation.
3.) Find an integrating factor that makes this equation exact (it can be done).
4.) Solve.
 
Pete69 said:

Homework Statement



I was given a problem to solve for the speed of a body falling under gravity [equation (1)] where g is acceleration due to gravity, which was easy enough.. but then i thought i would extend it to the case where g is non-constant, and so arrived at equation (2), (where where z is the height above Earth [z'=dz/dt and z=dv/dt and z^-2 means z to power -2], and M is the mass of the Earth and G is the gravitational constant)

Homework Equations



(1) : dv/dt = - g - kv

(2) : z'' + kz' + GMz^-2 = 0

The Attempt at a Solution



I believe this is a non-linear second order DE?? i attempted to solve by setting

z'' + kz' = 0

and solving the complimentary equation, which was OK, but when i came to solve for the particular integral
There is no "complementary equation" nor is there a "particular integral". Those are both concepts in linear differential equations where the non-homogeneous part is a function of the independent variable only.

z'' + kz' = -GMz^-2

i ran into problems, as after substituting in the D and Q operators (http://silmaril.math.sci.qut.edu.au/~gustafso/mab112/topic12/ ), i could not use the First Shift Theorem, as the RHS is not in an exponential form...

Any ideas anyone?
 
Last edited by a moderator:

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