Differential-Equations Β· Unit 9 Β· Video 1 Β· Interactive Practice

Second-Order Linear ODEs and the Spring–Mass–Dashpot

IKey Formulas

FormulaNameRole
yβ€²β€²+Ayβ€²+By=0y'' + Ay' + By = 0Standard formSecond order, linear, homogeneous; AA, BB constants
y=c1y1+c2y2y = c_1 y_1 + c_2 y_2General solutiony1y_1, y2y_2 are solutions; two constants for a second-order equation
mxβ€²β€²=βˆ’kxβˆ’cxβ€²β€…β€Šβ‡’β€…β€Šmxβ€²β€²+cxβ€²+kx=0mx'' = -kx - cx' \;\Rightarrow\; mx'' + cx' + kx = 0Spring–mass–dashpotNewton's law with Hooke's spring force and the dashpot force
A=cm,B=kmA = \dfrac{c}{m},\quad B = \dfrac{k}{m}CoefficientsDivide by mm: AA is the damping, BB the spring

Key Insight: Solving yβ€²β€²+Ayβ€²+By=0y'' + Ay' + By = 0 comes down to finding two solutions y1y_1, y2y_2; the two initial conditions y(0)y(0), yβ€²(0)y'(0) then fix c1c_1 and c2c_2.

IIVisualization 1 β€” Two Conditions Fix Two Constants

For yβ€²β€²=0y'' = 0, every solution is a line y=c1t+c2y = c_1 t + c_2: the starting value fixes c2c_2, the starting slope fixes c1c_1.

IIIVisualization 2 β€” Newton's Law on the Cart

The spring force βˆ’kx-kx depends only on position, the dashpot force βˆ’cxβ€²-cx' only on velocity; their sum is mxβ€²β€²mx''.

πŸ’‘ With xβ€²=0x' = 0 the dashpot exerts no force, however far the spring is stretched.

IVVisualization 3 β€” Only c/mc/m and k/mk/m Matter

Dividing mxβ€²β€²+cxβ€²+kx=0mx'' + cx' + kx = 0 by mm leaves A=c/mA = c/m (damping) and B=k/mB = k/m (spring) to govern the motion.

πŸ’‘ Challenge: find a second triple (m,c,k)(m, c, k) whose curve lands exactly on the dashed one, which has A=1A = 1, B=4B = 4.

VQuiz Questions

Problem 1 Β· Put the Model in Standard Form

Given: 3xβ€²β€²+6xβ€²+12x=03x'' + 6x' + 12x = 0 β€” find the coefficients AA and BB of the standard form xβ€²β€²+Axβ€²+Bx=0x'' + Ax' + Bx = 0.

βœ… Correct! Dividing every term by 33 gives xβ€²β€²+2xβ€²+4x=0x'' + 2x' + 4x = 0.
❌ The leading coefficient is not yet 11. Standard form starts with xβ€²β€²x'' alone, so every term must be divided by 33.
❌ The ratios are upside down. A=cm=63A = \frac{c}{m} = \frac{6}{3}, not 36\frac{3}{6}; you divide by the coefficient of xβ€²β€²x''.
❌ Only one term was divided. Dividing the equation by 33 divides every term, including 12x12x.
❌ Not quite. Divide every term by the coefficient of xβ€²β€²x''.
Show solution

Divide each term by the leading coefficient 33 (the role played by mm):

33xβ€²β€²+63xβ€²+123x=0β€…β€ŠβŸΉβ€…β€Šxβ€²β€²+2xβ€²+4x=0.\frac{3}{3}x'' + \frac{6}{3}x' + \frac{12}{3}x = 0 \;\Longrightarrow\; x'' + 2x' + 4x = 0.

Comparing with xβ€²β€²+Axβ€²+Bx=0x'' + Ax' + Bx = 0: A=2A = 2 and B=4B = 4.

Problem 2 Β· Signs of the Two Forces

Given: m=2m = 2, c=2c = 2, k=8k = 8. At one instant the cart is compressed toward the wall at x=βˆ’0.5x = -0.5 and moving away from the wall with xβ€²=1x' = 1 β€” find its acceleration xβ€²β€²x''.

βœ… Correct! The compressed spring pushes with +4+4, the dashpot resists the motion with βˆ’2-2, so 2xβ€²β€²=22x'' = 2.
❌ Check the spring force's sign. βˆ’kx=βˆ’8(βˆ’0.5)=+4-kx = -8(-0.5) = +4: a compressed spring pushes the mass away from the wall.
❌ That is mxβ€²β€²mx'', the net force. Divide by m=2m = 2 to get the acceleration.
❌ Check the dashpot force's sign. βˆ’cxβ€²=βˆ’2(1)=βˆ’2-cx' = -2(1) = -2: the dashpot always opposes the velocity.
❌ Not quite. Use mxβ€²β€²=βˆ’kxβˆ’cxβ€²mx'' = -kx - cx' with the given signs.
Show solution

Spring (Hooke's law): Fspring=βˆ’kx=βˆ’8(βˆ’0.5)=4F_{\text{spring}} = -kx = -8(-0.5) = 4, pointing away from the wall.

Dashpot: Fdashpot=βˆ’cxβ€²=βˆ’2(1)=βˆ’2F_{\text{dashpot}} = -cx' = -2(1) = -2, opposing the motion.

Newton's law:

mxβ€²β€²=βˆ’kxβˆ’cxβ€²=4βˆ’2=2β€…β€ŠβŸΉβ€…β€Šxβ€²β€²=22=1.mx'' = -kx - cx' = 4 - 2 = 2 \;\Longrightarrow\; x'' = \frac{2}{2} = 1.

Equivalently, in standard form xβ€²β€²+xβ€²+4x=0x'' + x' + 4x = 0: xβ€²β€²=βˆ’xβ€²βˆ’4x=βˆ’1+2=1x'' = -x' - 4x = -1 + 2 = 1.

Problem 3 Β· Fit the Constants Together

Given: y1=ety_1 = e^{t} and y2=eβˆ’ty_2 = e^{-t} are solutions of yβ€²β€²βˆ’y=0y'' - y = 0, so y=c1et+c2eβˆ’ty = c_1 e^{t} + c_2 e^{-t}. The initial conditions are y(0)=5y(0) = 5, yβ€²(0)=1y'(0) = 1 β€” find c1c_1 and c2c_2.

What is c1c_1?

What is c2c_2?

βœ… Correct! y=3et+2eβˆ’ty = 3e^{t} + 2e^{-t} has y(0)=3+2=5y(0) = 3 + 2 = 5 and yβ€²(0)=3βˆ’2=1y'(0) = 3 - 2 = 1.
❌ Here no condition fixes a constant on its own. At t=0t = 0 both exponentials equal 11, so y(0)=c1+c2y(0) = c_1 + c_2 and yβ€²(0)=c1βˆ’c2y'(0) = c_1 - c_2: two equations, solved together.
❌ Check c1c_1. Add the equations c1+c2=5c_1 + c_2 = 5 and c1βˆ’c2=1c_1 - c_2 = 1.
❌ Check c2c_2. Subtract c1βˆ’c2=1c_1 - c_2 = 1 from c1+c2=5c_1 + c_2 = 5; the derivative of eβˆ’te^{-t} carries a minus sign.
Show solution

Differentiate the general solution: yβ€²=c1etβˆ’c2eβˆ’ty' = c_1 e^{t} - c_2 e^{-t}.

Set t=0t = 0, where e0=1e^{0} = 1:

y(0)=c1+c2=5,yβ€²(0)=c1βˆ’c2=1.y(0) = c_1 + c_2 = 5, \qquad y'(0) = c_1 - c_2 = 1.

Adding: 2c1=62c_1 = 6, so c1=3c_1 = 3. Subtracting: 2c2=42c_2 = 4, so c2=2c_2 = 2.

y=3et+2eβˆ’t.y = 3e^{t} + 2e^{-t}.

Check: y(0)=3+2=5y(0) = 3 + 2 = 5 βœ“ and yβ€²(0)=3βˆ’2=1y'(0) = 3 - 2 = 1 βœ“.

Problem 4 Β· Two Carts, One Motion?

Given: cart PP has m=1m = 1, c=3c = 3, k=5k = 5; cart QQ has m=2m = 2, c=6c = 6, k=10k = 10. Both start from the same x(0)x(0) and xβ€²(0)x'(0) β€” compare their motions.

βœ… Correct! Both reduce to xβ€²β€²+3xβ€²+5x=0x'' + 3x' + 5x = 0, and the same initial conditions fix the same c1c_1, c2c_2.
❌ The heavier mass comes with a stiffer spring. What matters is B=k/m=10/2=5B = k/m = 10/2 = 5, the same as for PP.
❌ Damping counts relative to the mass. A=c/m=6/2=3A = c/m = 6/2 = 3, the same as for PP.
❌ The amplitude is set by the initial conditions, which are the same for both carts; the equations reduce to the same standard form.
❌ Not quite. Divide each equation by its mass and compare.
Show solution

Cart PP: xβ€²β€²+3xβ€²+5x=0x'' + 3x' + 5x = 0 directly, since m=1m = 1.

Cart QQ: 2xβ€²β€²+6xβ€²+10x=02x'' + 6x' + 10x = 0; dividing by 22 gives xβ€²β€²+3xβ€²+5x=0x'' + 3x' + 5x = 0.

Both have A=c/m=3A = c/m = 3 and B=k/m=5B = k/m = 5, so they satisfy the same equation. Its general solution c1y1+c2y2c_1 y_1 + c_2 y_2 is the same for both, and the same x(0)x(0), xβ€²(0)x'(0) fix the same c1c_1, c2c_2. The motions are identical: doubling mm, cc and kk together changes nothing.

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