Differential-Equations Β· Unit 9 Β· Video 1 Β· Interactive Practice
Second-Order Linear ODEs and the SpringβMassβDashpot
IKey Formulas
Formula
Name
Role
yβ²β²+Ayβ²+By=0
Standard form
Second order, linear, homogeneous; A, B constants
y=c1βy1β+c2βy2β
General solution
y1β, y2β are solutions; two constants for a second-order equation
mxβ²β²=βkxβcxβ²βmxβ²β²+cxβ²+kx=0
Springβmassβdashpot
Newton's law with Hooke's spring force and the dashpot force
A=mcβ,B=mkβ
Coefficients
Divide by m: A is the damping, B the spring
Key Insight: Solving yβ²β²+Ayβ²+By=0 comes down to finding two solutions y1β, y2β; the two initial conditions y(0), yβ²(0) then fix c1β and c2β.
IIVisualization 1 β Two Conditions Fix Two Constants
For yβ²β²=0, every solution is a line y=c1βt+c2β: the starting value fixes c2β, the starting slope fixes c1β.
IIIVisualization 2 β Newton's Law on the Cart
The spring force βkx depends only on position, the dashpot force βcxβ² only on velocity; their sum is mxβ²β².
π‘ With xβ²=0 the dashpot exerts no force, however far the spring is stretched.
IVVisualization 3 β Only c/m and k/m Matter
Dividing mxβ²β²+cxβ²+kx=0 by m leaves A=c/m (damping) and B=k/m (spring) to govern the motion.
π‘ Challenge: find a second triple (m,c,k) whose curve lands exactly on the dashed one, which has A=1, B=4.
VQuiz Questions
Problem 1 Β· Put the Model in Standard Form
Given:3xβ²β²+6xβ²+12x=0 β find the coefficients A and B of the standard form xβ²β²+Axβ²+Bx=0.
β Correct! Dividing every term by 3 gives xβ²β²+2xβ²+4x=0.
β The leading coefficient is not yet 1. Standard form starts with xβ²β² alone, so every term must be divided by 3.
β The ratios are upside down.A=mcβ=36β, not 63β; you divide by the coefficient of xβ²β².
β Only one term was divided. Dividing the equation by 3 divides every term, including 12x.
β Not quite. Divide every term by the coefficient of xβ²β².
Show solution
Divide each term by the leading coefficient 3 (the role played by m):
Given:m=2, c=2, k=8. At one instant the cart is compressed toward the wall at x=β0.5 and moving away from the wall with xβ²=1 β find its acceleration xβ²β².
β Correct! The compressed spring pushes with +4, the dashpot resists the motion with β2, so 2xβ²β²=2.
β Check the spring force's sign.βkx=β8(β0.5)=+4: a compressed spring pushes the mass away from the wall.
β That is mxβ²β², the net force. Divide by m=2 to get the acceleration.
β Check the dashpot force's sign.βcxβ²=β2(1)=β2: the dashpot always opposes the velocity.
β Not quite. Use mxβ²β²=βkxβcxβ² with the given signs.
Show solution
Spring (Hooke's law):Fspringβ=βkx=β8(β0.5)=4, pointing away from the wall.
Dashpot:Fdashpotβ=βcxβ²=β2(1)=β2, opposing the motion.
Newton's law:
mxβ²β²=βkxβcxβ²=4β2=2βΉxβ²β²=22β=1.
Equivalently, in standard form xβ²β²+xβ²+4x=0: xβ²β²=βxβ²β4x=β1+2=1.
Problem 3 Β· Fit the Constants Together
Given:y1β=et and y2β=eβt are solutions of yβ²β²βy=0, so y=c1βet+c2βeβt. The initial conditions are y(0)=5, yβ²(0)=1 β findc1β and c2β.
What is c1β?
What is c2β?
β Correct!y=3et+2eβt has y(0)=3+2=5 and yβ²(0)=3β2=1.
β Here no condition fixes a constant on its own. At t=0 both exponentials equal 1, so y(0)=c1β+c2β and yβ²(0)=c1ββc2β: two equations, solved together.
β Check c1β. Add the equations c1β+c2β=5 and c1ββc2β=1.
β Check c2β. Subtract c1ββc2β=1 from c1β+c2β=5; the derivative of eβt carries a minus sign.
Show solution
Differentiate the general solution: yβ²=c1βetβc2βeβt.
Set t=0, where e0=1:
y(0)=c1β+c2β=5,yβ²(0)=c1ββc2β=1.
Adding: 2c1β=6, so c1β=3. Subtracting: 2c2β=4, so c2β=2.
y=3et+2eβt.
Check:y(0)=3+2=5 β and yβ²(0)=3β2=1 β.
Problem 4 Β· Two Carts, One Motion?
Given: cart P has m=1, c=3, k=5; cart Q has m=2, c=6, k=10. Both start from the same x(0) and xβ²(0) β compare their motions.
β Correct! Both reduce to xβ²β²+3xβ²+5x=0, and the same initial conditions fix the same c1β, c2β.
β The heavier mass comes with a stiffer spring. What matters is B=k/m=10/2=5, the same as for P.
β Damping counts relative to the mass.A=c/m=6/2=3, the same as for P.
β The amplitude is set by the initial conditions, which are the same for both carts; the equations reduce to the same standard form.
β Not quite. Divide each equation by its mass and compare.
Show solution
Cart P: xβ²β²+3xβ²+5x=0 directly, since m=1.
Cart Q: 2xβ²β²+6xβ²+10x=0; dividing by 2 gives xβ²β²+3xβ²+5x=0.
Both have A=c/m=3 and B=k/m=5, so they satisfy the same equation. Its general solution c1βy1β+c2βy2β is the same for both, and the same x(0), xβ²(0) fix the same c1β, c2β. The motions are identical: doubling m, c and k together changes nothing.