To solve this integral, we need to integrate both sides with respect to their respective variables:
∫ S'dt = ∫ S'a dz
Since S' represents the velocity and S'a represents the acceleration, we can rewrite the equation as:
∫ v dt = ∫ a dz
where v is the velocity and a is the acceleration.
Integrating both sides with respect to time, we get:
∫ v dt = ∫ a dz
∫ v dt = vz + C1
where C1 is the constant of integration.
Integrating both sides with respect to displacement (z), we get:
∫ a dz = ∫ dv dt dz
∫ a dz = ∫ dv dz dt
∫ a dz = v(dv/dz)
where dv/dz represents the gradient of the velocity curve.
Substituting this back into the original equation:
∫ v dt = ∫ a dz
vz + C1 = ∫ v(dv/dz) dz
vz + C1 = 1/2 v^2 + C2
where C2 is the constant of integration.
Rearranging the terms, we get:
1/2 v^2 - vz = C1 - C2
We can simplify this by setting C3 = C1 - C2, giving us:
1/2 v^2 - vz = C3
This is the equation of motion, which relates the velocity and displacement of an object undergoing constant acceleration.
Solve the following integral and find the equation of motion. S'do (1) dt = S'a dz
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