Solve Forced Oscillation using Differential Equation Method

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In summary: The weight mg of the bob, which acts at its centre of gravity G. 2. Tension T of the string. 3. The force of resistance F proportional to the velocity of the bob. The bob is at a distance Lθ from the pivot. The force of gravity is resolved into mg sinθ in the direction of motion and mg cosθ at right angles to it. The equation of motion is: mLθ"=-mg sinθ-T-F F=Bθ' (B is a constant) For small oscillations, sinθ≃θ The equation of motion is: θ"+(g/L)θ=-(1/m)L(T+Bθ') This
  • #1
angelwentheng
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The differential eqn that governs the forced oscillation is shown below:
0.2(d^2 y)/(dt^2 )+ 1.2dy/dt + 2y = r(t) where r(t) is the external force

Given that r(t) = 5cos4t with y(0) = 0.5 and y'(0) = 0. Find the equation of motion of the forced oscillation..

Please help me to solve by using differential eqn method..thx!urgent
 
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  • #2
welcome to pf!

hi angelwentheng! welcome to pf! :smile:

(try using the X2 icon just above the Reply box :wink:)

show us what you've tried, and where you're stuck, and then we'll know how to help! :smile:
 
  • #3
0.2(d^2 y)/(dt^2 )+ 1.2dy/dt + 2y = r(t)
0.2(d^2 y)/(dt^2 ) + 1.2dy/dt + 2y = 5cos4t
0.2m^2 + 1.2m + 2 = 0
m = (-b±√(b^2-4ac))/2a
= (-(1.2)± √(〖(1.2)〗^2-4(0.2)(2)))/(2(0.2))
= (-1.2 ±0.4i)/0.4
= -3 ± i
y_h(t) = e^(-3t) (Acosx+Bsinx)
r (t) = 5cos4t
y_p (t) = pcos4t + qsin4t ------------ (1)
y_p^' (t)= -4psin4t + 4qcos4t---------- (2)
y_p^'' (t) = -16pcos4t – 16qsin4t ---------- (3)
Substitute (1), (2) and (3) into 0.2 (d^2 y)/(dt^2 ) + 1.2 dy/dt + 2y = 5cos4t
0.2(-16pcos4t – 16qsin4t) + 1.2(-4psin4t + 4qcos4t) + 2(pcos4t + qsin4t) = 5cos4t
-3.2pcos4t – 3.2qsin4t – 4.8psin4t + 4.8qcos4t + 2pcos4t + 2qsin4t = 5cos4t
Equate the coefficients:
For cos4t:
-3.2p + 4.8q + 2p = 5
-1.2p + 4.8q = 5 ---------- (1)
For sin4t:
-3.2q – 4.8p + 2q = 0
-1.2q – 4.8p = 0 ----------- (2)
Equation 1 x4
19.2 q – 4.8p = 20---------- (3)
-20.4q = -20
q = 50/51
Substitute q =50/51 into equation (2)
-1.2(50/51) – 4.8p = 0
- 4.8p = 20/17
P = - 25/102
y_p (t)= - 25/102cos4t + 50/51sin4t
y (t) =y_h(t) + y_p(t)
= e^(-3t)(Acos t + Bsin t) - 25/102cos4t + 50/51sin4t
Given y (0) = 0.5
A – 25/102 = 0.5
A = 38/51
y’(t) = e^(-3t )(-Asin t + Bcos t) +(Acos t + Bsin t)(-3e^(-3t)) + 50/51sin4t +200/51cos4t
Given y’ (0) = 0
B – 3A + 200/51 = 0
B – 3(38/51) + 200/51 = 0
B = -86/51
Therefore, the equation of motion of the forced oscillation is y(t) = e^(-3t)(38/51cos t – 86/51sin t) – 25/102cos4t + 50/51sin4t


pls help me to check am i correct or not.thanks:smile:
 
  • #4
sorry for not noticing the sign
 
  • #5
(please using the X2 icon just above the Reply box, to make your equations readable :redface:)
angelwentheng said:
herefore, the equation of motion of the forced oscillation is y(t) = e^(-3t)(38/51cos t – 86/51sin t) – 25/102cos4t + 50/51sin4t

well y(0) = 76/102 - 25/102 = 0.5

and y'(0) = -86/51 - 3*38/51 + 200/51 = 0,

so that looks ok :smile:
 
  • #6
Thanks~I'm wondering am I need to do the forced oscillation equation?which means using the spring equation f = kx
 
  • #7
angelwentheng said:
Thanks~I'm wondering am I need to do the forced oscillation equation?which means using the spring equation f = kx
angelwentheng said:
The differential eqn that governs the forced oscillation is shown below:
0.2(d^2 y)/(dt^2 )+ 1.2dy/dt + 2y = r(t) where r(t) is the external force

Given that r(t) = 5cos4t with y(0) = 0.5 and y'(0) = 0. Find the equation of motion of the forced oscillation..

you've solved the given equation for forced oscillation …

what does some other equation have to do with it? :confused:
 
  • #8
oh...i am blur...sorry
 
  • #9
A simple pendulum of length is oscillating through a small angle θ in a medium for which
the resistance is proportional to the velocity. Obtain the differential equation of its motion
and discuss the motion.
sorry help me with these...I'm totally blank
 
  • #10
angelwentheng said:
A simple pendulum of length is oscillating through a small angle θ in a medium for which
the resistance is proportional to the velocity. Obtain the differential equation of its motion
and discuss the motion.
sorry help me with these...I'm totally blank

well the differential equation should be easy …

what do you make it? :smile:
 
  • #11
sorry I have no idea for this ques...can u help me?
 
  • #12
angelwentheng said:
A simple pendulum of length is oscillating through a small angle θ in a medium for which
the resistance is proportional to the velocity.

just translate the English into maths …

you know what the usual equations is (without resistance) …

now add a force proportional to the speed
 
  • #13
External forces are zero, so the governing equation is homogeneous:
mx"+Bx'+kx=0

x"=d²x/dt².
x'=dx/dt
x=displacement, positive to the right
m=mass
B=resistance proportional to the velocity
k=stiffness (of a spring), which is resistance proportional to the displacement.
 
  • #14
angelwentheng said:
External forces are zero, so the governing equation is homogeneous:
mx"+Bx'+kx=0

i don't understand what you mean by "External forces are zero" …

both gravity and the resistance are external forces :confused:

but anyway, yes that's the correct equation :smile:

now the question asks you to "discuss the motion" …

so what are the solutions, and how do they change if you increase B ?
 
  • #15
external forces means f(t)...cz actually the original eqn will be mx'' + Bx' + kx = f(x)
since there is no external force...therefore f(x)=o
but why increasing the resistance?the question said directly proportional to velocity...

erm...sorry i 'm nt physics students...so i might not understand phy laws...so pls guide me
 
  • #16
angelwentheng said:
external forces means f(t)...cz actually the original eqn will be mx'' + Bx' + kx = f(x)
since there is no external force...therefore f(x)=o

actually, f(t) would be a time-dependent external force;

kx is an f(x), an external position-dependent force :smile:
but why increasing the resistance?the question said directly proportional to velocity...

yes, you can't change B in the middle of a particular motion

but you can have different experiments with different Bs, and the question is asking you to categorise the solutions …

the solutions will be of different characters, depending how large B is (think "damping" :wink:)
 
  • #17
For a pendulum of length L and mass m,
making an angle θ with the vertical, three forces act on the mass m.
The vertical force due to gravity, mg.
A horizontal restoring force (towards the equilibrium position) of mgsin(θ), and the tension, which is equal and opposite to the resultant of the two forces.
The restoring force mgsin(θ) is often approximated by
kx=mgLsin(θ)≅mgLθ for small angles (when θ is in radians).

This is my explanation for this ques...is it correct?
 
  • #18
angelwentheng said:
A simple pendulum of length is oscillating through a small angle θ in a medium for which
the resistance is proportional to the velocity. Obtain the differential equation of its motion
and discuss the motion.
angelwentheng said:
This is my explanation for this ques...

no it isn't!

its your explanation for a different question …

the question asked you to discuss the motion with a resistance proportional to the velocity
 
  • #19
then how to explain??:confused:
 
  • #20
well, first you'll have to solve the equation, won't you? :wink:
 
  • #21
angelwentheng said:
A simple pendulum of length is oscillating through a small angle θ in a medium for which
the resistance is proportional to the velocity. Obtain the differential equation of its motion
and discuss the motion.
sorry help me with these...I'm totally blank

I am stucked in this same question too!could anyone help?
 

1. What is a forced oscillation?

A forced oscillation is a type of oscillation or periodic motion that is influenced by an external force. This external force could be a constant force or a variable force that changes with time.

2. How is a forced oscillation described by a differential equation?

A forced oscillation is described by a second-order differential equation, where the acceleration of the oscillating system is equal to the sum of the natural restoring force and the external force.

3. What is the general solution to a forced oscillation differential equation?

The general solution to a forced oscillation differential equation is a combination of the homogeneous solution (solution to the corresponding homogeneous equation) and the particular solution (solution to the particular external force). The particular solution is often found using the method of undetermined coefficients.

4. How do you find the natural frequency and damping ratio of a forced oscillation system?

The natural frequency and damping ratio of a forced oscillation system can be found by solving the characteristic equation of the differential equation. The natural frequency is the square root of the coefficient of the second derivative term, and the damping ratio is the ratio of the coefficient of the first derivative term to twice the square root of the product of the coefficient of the second derivative term and the constant term.

5. What is the significance of solving forced oscillation using the differential equation method?

Solving forced oscillation using the differential equation method allows us to understand the behavior of a forced oscillation system and predict its response to different external forces. It also helps in designing and controlling systems that exhibit forced oscillations, such as electronic circuits and mechanical systems.

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