Solving Separable DEs - Calculus 2

  1. The solution to y′=ycos⁡(x)y' = y \cos(x) satisfies y(0)=1y(0) = 1. Evaluate y(π/2)y(\pi/2).
    Answer: ee When you encounter a differential equation like y′=ycos⁡(x)y' = y \cos(x), you're dealing with a separable differential equation. The key insight is recognizing that you can separate the variables and integrate both sides. Start by rewriting the equation as dydx=ycos⁡(x)\frac{dy}{dx} = y \cos(x), then separate variables: dyy=cos⁡(x)dx\frac{dy}{y} = \cos(x) dx. Now integrate both sides: ∫dyy=∫cos⁡(x)dx\int \frac{dy}{y} = \int \cos(x) dx, which gives you ln⁡∣y∣=sin⁡(x)+C\ln|y| = \sin(x) + C. Exponentiating both sides yields y=Aesin⁡(x)y = Ae^{\sin(x)} where A=eCA = e^C. Use the initial condition y(0)=1y(0) = 1 to find AA: 1=Aesin⁡(0)=Ae0=A1 = Ae^{\sin(0)} = Ae^0 = A, so A=1A = 1. Therefore, y=esin⁡(x)y = e^{\sin(x)}. To find y(π/2)y(\pi/2), substitute: y(π/2)=esin⁡(π/2)=e1=ey(\pi/2) = e^{\sin(\pi/2)} = e^1 = e. Looking at the wrong answers: Choice A, eπ/2e^{\pi/2}, results from incorrectly integrating cos⁡(x)\cos(x) as xx instead of sin⁡(x)\sin(x). Choice B, 11, comes from forgetting to apply the exponential function after integration or assuming the solution is constant. Choice D, 00, might stem from confusing this with a different type of differential equation or making algebraic errors. The correct answer is C, ee. Remember: for separable differential equations, always separate variables completely before integrating, and don't forget to use your initial conditions to determine any constants. Practice recognizing when sin⁡(π/2)=1\sin(\pi/2) = 1 to avoid computational errors.
  2. A particle moves along the y-axis such that its velocity is given by v(t)=dydt=2t(y+1)v(t) = \frac{dy}{dt} = 2t(y+1). If y(1)=e−1y(1)=e-1, find y(2)y(2).
    Answer: e4−1e^4 - 1 This is a separable differential equation problem where you need to solve for the particle's position given its velocity function and an initial condition. When you see dydt=2t(y+1)\frac{dy}{dt} = 2t(y+1), recognize this as separable since you can isolate all y terms on one side and all t terms on the other. Separate the variables: dyy+1=2t dt\frac{dy}{y+1} = 2t \, dt Integrate both sides: ∫dyy+1=∫2t dt\int \frac{dy}{y+1} = \int 2t \, dt This gives you: ln⁡∣y+1∣=t2+C\ln|y+1| = t^2 + C Exponentiate both sides: ∣y+1∣=et2+C=Aet2|y+1| = e^{t^2 + C} = Ae^{t^2} where A=eCA = e^C Since we're dealing with position, assume y+1>0y+1 > 0, so: y+1=Aet2y+1 = Ae^{t^2}, which means y=Aet2−1y = Ae^{t^2} - 1 Use the initial condition y(1)=e−1y(1) = e-1 to find A: e−1=Ae12−1=Ae−1e-1 = Ae^{1^2} - 1 = Ae - 1 Solving: e=Aee = Ae, so A=1A = 1 Therefore: y(t)=et2−1y(t) = e^{t^2} - 1 At t=2t = 2: y(2)=e22−1=e4−1y(2) = e^{2^2} - 1 = e^4 - 1 Choice A (e3−1e^3 - 1) likely comes from incorrectly computing 22=2×22^2 = 2 \times 2 as just 33. Choice C (e4e^4) results from forgetting the −1-1 constant term. Choice D (2e−12e - 1) suggests confusion with the coefficient in the original equation. Strategy tip: In separable differential equations, always check your constant of integration using the initial condition, and be careful with exponent arithmetic when substituting your final t-value.
  3. Consider the differential equation dydx=x2+1y2−4\frac{dy}{dx} = \frac{x^2 + 1}{y^2 - 4} with initial condition y(0)=3y(0) = 3. Which of the following represents the solution in implicit form?
    Answer: y33−4y=x33+x−3\frac{y^3}{3} - 4y = \frac{x^3}{3} + x - 3 When you encounter a differential equation where variables can be separated, your goal is to move all terms involving one variable to one side and all terms involving the other variable to the opposite side, then integrate both sides. Starting with dydx=x2+1y2−4\frac{dy}{dx} = \frac{x^2 + 1}{y^2 - 4}, you can separate variables by multiplying both sides by (y2−4)(y^2 - 4) and dxdx: (y2−4)dy=(x2+1)dx(y^2 - 4)dy = (x^2 + 1)dx Now integrate both sides. The left side gives: ∫(y2−4)dy=y33−4y+C1\int (y^2 - 4)dy = \frac{y^3}{3} - 4y + C_1 The right side gives: ∫(x2+1)dx=x33+x+C2\int (x^2 + 1)dx = \frac{x^3}{3} + x + C_2 Setting them equal: y33−4y=x33+x+C\frac{y^3}{3} - 4y = \frac{x^3}{3} + x + C where C=C2−C1C = C_2 - C_1 To find CC, use the initial condition y(0)=3y(0) = 3: 333−4(3)=033+0+C\frac{3^3}{3} - 4(3) = \frac{0^3}{3} + 0 + C, which gives 9−12=C9 - 12 = C, so C=−3C = -3 Therefore, the solution is y33−4y=x33+x−3\frac{y^3}{3} - 4y = \frac{x^3}{3} + x - 3, making D correct. A and C both have C=+3C = +3 instead of C=−3C = -3, showing incorrect application of the initial condition. B has C=−13C = -\frac{1}{3}, which would result from arithmetic errors when substituting the initial condition. Remember: after separating variables and integrating, always substitute your initial condition carefully to find the constant. Double-check your arithmetic since sign errors are common in these problems.
  4. A population of bacteria grows according to the differential equation dPdt=kP(1000−P)\frac{dP}{dt} = kP(1000 - P), where P(t)P(t) is the population at time tt and k>0k > 0 is a constant. If the initial population is P(0)=50P(0) = 50 and the population reaches 200 after 2 hours, what is the population after 4 hours?
    Answer: 1600041\frac{16000}{41} bacteria This is a separable differential equation. Separating variables: dPP(1000−P)=k dt\frac{dP}{P(1000-P)} = k\,dt. Using partial fractions: 1P(1000−P)=11000(1P+11000−P)\frac{1}{P(1000-P)} = \frac{1}{1000}\left(\frac{1}{P} + \frac{1}{1000-P}\right). Integrating: 11000ln⁡∣P1000−P∣=kt+C\frac{1}{1000}\ln\left|\frac{P}{1000-P}\right| = kt + C. With P(0)=50P(0) = 50: C=11000ln⁡(50950)=11000ln⁡(119)C = \frac{1}{1000}\ln\left(\frac{50}{950}\right) = \frac{1}{1000}\ln\left(\frac{1}{19}\right). Using P(2)=200P(2) = 200: 11000ln⁡(200800)=2k+11000ln⁡(119)\frac{1}{1000}\ln\left(\frac{200}{800}\right) = 2k + \frac{1}{1000}\ln\left(\frac{1}{19}\right), which gives k=12000ln⁡(194)k = \frac{1}{2000}\ln\left(\frac{19}{4}\right). For t=4t = 4: ln⁡(P1000−P)=ln⁡(1916)\ln\left(\frac{P}{1000-P}\right) = \ln\left(\frac{19}{16}\right), so P1000−P=1916\frac{P}{1000-P} = \frac{19}{16}. Solving: P=1600041P = \frac{16000}{41}.
  5. Let y=f(x)y=f(x) be the solution to the initial value problem y′+2xy=0y' + 2xy = 0 with y(0)=ey(0) = e. Find the positive value of xx for which y(x)=1y(x) = 1.
    Answer: 11 First, rewrite the equation as dydx=−2xy\frac{dy}{dx} = -2xy. Separate the variables: 1ydy=−2xdx\frac{1}{y} dy = -2x dx. Integrate both sides: ln⁡∣y∣=−x2+C\ln|y| = -x^2 + C. Use the initial condition y(0)=ey(0) = e: ln⁡∣e∣=−02+C  ⟹  1=C\ln|e| = -0^2 + C \implies 1 = C. The particular solution is ln⁡∣y∣=−x2+1\ln|y| = -x^2 + 1. Since y(0)=e>0y(0)=e>0, we can write ln⁡(y)=1−x2\ln(y) = 1 - x^2. The explicit solution is y=e1−x2y = e^{1-x^2}. Now, set y(x)=1y(x) = 1: 1=e1−x21 = e^{1-x^2}. Taking the natural logarithm of both sides gives 0=1−x20 = 1 - x^2, so x2=1x^2 = 1. The positive value is x=1x=1.
  6. Let y=f(x)y=f(x) be the solution for y′=xe−yy' = x e^{-y} with f(1)=0f(1)=0. What is the value of f(3)f(3)?
    Answer: ln⁡(5)\ln(5) This is a separable differential equation problem where you need to isolate variables and integrate both sides to find the particular solution. When you see y′=xe−yy' = xe^{-y}, recognize this as separable since you can write it as dydx=xe−y\frac{dy}{dx} = xe^{-y}. Multiply both sides by eye^y and dxdx to get ey dy=x dxe^y \, dy = x \, dx. Now integrate both sides: ∫ey dy=∫x dx\int e^y \, dy = \int x \, dx, which gives you ey=x22+Ce^y = \frac{x^2}{2} + C. Use the initial condition f(1)=0f(1) = 0 to find CC. When x=1x = 1 and y=0y = 0: e0=122+Ce^0 = \frac{1^2}{2} + C, so 1=12+C1 = \frac{1}{2} + C, meaning C=12C = \frac{1}{2}. Your general solution is ey=x22+12=x2+12e^y = \frac{x^2}{2} + \frac{1}{2} = \frac{x^2 + 1}{2}. To find f(3)f(3), substitute x=3x = 3: ey=9+12=5e^y = \frac{9 + 1}{2} = 5. Taking the natural logarithm: y=ln⁡(5)y = \ln(5), which is answer choice D. Answer A, ln⁡(11/2)\ln(11/2), would result from incorrectly adding instead of finding C=12C = \frac{1}{2}. Answer B, ln⁡(9/2)\ln(9/2), comes from forgetting to add the constant CC entirely. Answer C, 55, is the trap of stopping at ey=5e^y = 5 without taking the logarithm. Remember: with separable equations, always separate variables completely before integrating, and don't forget to apply initial conditions to find your constant of integration.
  7. A curve y=f(x)y=f(x) passes through the point (e,2)(e, 2) and its slope at any point (x,y)(x,y) is given by dydx=yxln⁡(x)\frac{dy}{dx} = \frac{y}{x \ln(x)}. What is the value of yy when x=e4x=e^4?
    Answer: 88 Separate the variables: 1ydy=1xln⁡(x)dx\frac{1}{y} dy = \frac{1}{x \ln(x)} dx. Integrate both sides. The left side is ln⁡∣y∣\ln|y|. For the right side, use u-substitution with u=ln⁡(x)u=\ln(x) and du=1xdxdu=\frac{1}{x}dx. This gives ∫1udu=ln⁡∣u∣=ln⁡∣ln⁡(x)∣\int \frac{1}{u} du = \ln|u| = \ln|\ln(x)|. So, ln⁡∣y∣=ln⁡∣ln⁡(x)∣+C\ln|y| = \ln|\ln(x)| + C. Using the point (e,2)(e,2): ln⁡(2)=ln⁡∣ln⁡(e)∣+C  ⟹  ln⁡(2)=ln⁡(1)+C  ⟹  C=ln⁡(2)\ln(2) = \ln|\ln(e)| + C \implies \ln(2) = \ln(1) + C \implies C = \ln(2). The solution is ln⁡∣y∣=ln⁡∣ln⁡(x)∣+ln⁡(2)=ln⁡(2∣ln⁡(x)∣)\ln|y| = \ln|\ln(x)| + \ln(2) = \ln(2|\ln(x)|). So, ∣y∣=2∣ln⁡(x)∣|y| = 2|\ln(x)|. Since y(e)=2>0y(e)=2>0 and for x>1x>1, ln⁡(x)>0\ln(x)>0, we have y=2ln⁡(x)y = 2\ln(x). At x=e4x=e^4, y=2ln⁡(e4)=2⋅4=8y = 2\ln(e^4) = 2 \cdot 4 = 8.
  8. Let y(t)y(t) be the solution to the initial value problem dydt=2y(1−y8)\frac{dy}{dt} = 2y(1 - \frac{y}{8}) with y(0)=2y(0) = 2. Find lim⁡t→∞y(t)\lim_{t\to\infty} y(t).
    Answer: 88 The differential equation is a logistic growth model of the form dydt=ky(1−yK)\frac{dy}{dt} = ky(1 - \frac{y}{K}), where KK is the carrying capacity. By comparing the given equation with the standard form, we can identify the carrying capacity K=8K=8. For any initial condition y(0)>0y(0) > 0, the solution y(t)y(t) will approach the carrying capacity KK as t→∞t \to \infty. Since y(0)=2>0y(0) = 2 > 0, lim⁡t→∞y(t)=8\lim_{t\to\infty} y(t) = 8.
  9. The rate of change of a quantity PP is directly proportional to the square root of PP. If P=9P=9 when t=1t=1 and P=25P=25 when t=2t=2, what is PP when t=0t=0?
    Answer: 11 When you encounter a problem stating that "the rate of change of a quantity is directly proportional to" something, you're dealing with a differential equation. The phrase "rate of change" means derivative, so you need to set up and solve dPdt=kP\frac{dP}{dt} = k\sqrt{P} where kk is the constant of proportionality. To solve this separable differential equation, separate variables: dPP=k dt\frac{dP}{\sqrt{P}} = k \, dt. Integrating both sides gives 2P=kt+C2\sqrt{P} = kt + C, or P=kt+C2\sqrt{P} = \frac{kt + C}{2}. Therefore, P=(kt+C2)2P = \left(\frac{kt + C}{2}\right)^2. Using the given conditions, when t=1t = 1, P=9P = 9: 9=(k+C2)29 = \left(\frac{k + C}{2}\right)^2, so k+C2=3\frac{k + C}{2} = 3, giving us k+C=6k + C = 6. When t=2t = 2, P=25P = 25: 25=(2k+C2)225 = \left(\frac{2k + C}{2}\right)^2, so 2k+C2=5\frac{2k + C}{2} = 5, giving us 2k+C=102k + C = 10. Solving this system: From the second equation minus the first, k=4k = 4. Substituting back: C=2C = 2. Therefore, P=(4t+22)2=(2t+1)2P = \left(\frac{4t + 2}{2}\right)^2 = (2t + 1)^2. When t=0t = 0: P=(2(0)+1)2=1P = (2(0) + 1)^2 = 1, confirming answer C. Answer A (P=0P = 0) would require C=0C = 0, which contradicts our conditions. Answer B (P=4P = 4) and D (P=2P = 2) result from arithmetic errors in solving the system of equations or incorrectly setting up the integration constant. Study tip: Always use both given conditions to find both unknown constants, and verify your final equation works for the given data points.
  10. Solve the initial value problem dydθ=sec⁡2(θ)sec⁡(y)\frac{dy}{d\theta} = \sec^2(\theta) \sec(y) with the initial condition y(π/4)=π/6y(\pi/4) = \pi/6. Find the value of y(0)y(0).
    Answer: −π/6-\pi/6 Rewrite the equation as dydθ=sec⁡2(θ)cos⁡(y)\frac{dy}{d\theta} = \frac{\sec^2(\theta)}{\cos(y)}. Separate the variables: cos⁡(y)dy=sec⁡2(θ)dθ\cos(y) dy = \sec^2(\theta) d\theta. Integrate both sides: ∫cos⁡(y)dy=∫sec⁡2(θ)dθ\int \cos(y) dy = \int \sec^2(\theta) d\theta, which gives sin⁡(y)=tan⁡(θ)+C\sin(y) = \tan(\theta) + C. Use the initial condition y(π/4)=π/6y(\pi/4) = \pi/6: sin⁡(π/6)=tan⁡(π/4)+C  ⟹  1/2=1+C  ⟹  C=−1/2\sin(\pi/6) = \tan(\pi/4) + C \implies 1/2 = 1 + C \implies C = -1/2. The particular solution is sin⁡(y)=tan⁡(θ)−1/2\sin(y) = \tan(\theta) - 1/2. To find y(0)y(0), substitute θ=0\theta=0: sin⁡(y)=tan⁡(0)−1/2=−1/2\sin(y) = \tan(0) - 1/2 = -1/2. Therefore, y=arcsin⁡(−1/2)=−π/6y = \arcsin(-1/2) = -\pi/6.
  11. The solution to the differential equation dydx=xy+xy2+1\frac{dy}{dx} = \frac{xy + x}{y^2 + 1} passes through the point (2,1)(2, 1). Which of the following equations implicitly defines this solution?
    Answer: y2−2y−x2+4ln⁡(y+1)=4ln⁡(2)−5y^2 - 2y - x^2 + 4\ln(y+1) = 4\ln(2) - 5 First, factor the numerator: dydx=x(y+1)y2+1\frac{dy}{dx} = \frac{x(y+1)}{y^2+1}. Separate variables: y2+1y+1dy=xdx\frac{y^2+1}{y+1} dy = x dx. Use polynomial long division or substitution on the left side: y2−1+2y+1=(y−1)(y+1)+2y+1=y−1+2y+1\frac{y^2-1+2}{y+1} = \frac{(y-1)(y+1)+2}{y+1} = y-1 + \frac{2}{y+1}. Now integrate: ∫(y−1+2y+1)dy=∫xdx\int (y-1 + \frac{2}{y+1}) dy = \int x dx. This gives y22−y+2ln⁡∣y+1∣=x22+C\frac{y^2}{2} - y + 2\ln|y+1| = \frac{x^2}{2} + C. Use the point (2,1)(2,1): 122−1+2ln⁡∣1+1∣=222+C  ⟹  −12+2ln⁡(2)=2+C  ⟹  C=2ln⁡(2)−52\frac{1^2}{2} - 1 + 2\ln|1+1| = \frac{2^2}{2} + C \implies -\frac{1}{2} + 2\ln(2) = 2 + C \implies C = 2\ln(2) - \frac{5}{2}. The implicit solution is y22−y+2ln⁡∣y+1∣=x22+2ln⁡(2)−52\frac{y^2}{2} - y + 2\ln|y+1| = \frac{x^2}{2} + 2\ln(2) - \frac{5}{2}. Since y(2)=1y(2)=1, y+1>0y+1>0 near the initial condition. Multiply by 2 to clear fractions: y2−2y+4ln⁡(y+1)=x2+4ln⁡(2)−5y^2 - 2y + 4\ln(y+1) = x^2 + 4\ln(2) - 5, which rearranges to y2−2y−x2+4ln⁡(y+1)=4ln⁡(2)−5y^2 - 2y - x^2 + 4\ln(y+1) = 4\ln(2) - 5.
  12. Find the particular solution to xdydx=2(y−5)x\frac{dy}{dx} = 2(y-5) that satisfies the initial condition y(1)=10y(1) = 10.
    Answer: y=5x2+5y = 5x^2 + 5 When you encounter a differential equation like xdydx=2(y−5)x\frac{dy}{dx} = 2(y-5), you're dealing with a separable differential equation. The key is to separate variables so that all terms involving yy are on one side and all terms involving xx are on the other. Start by rearranging: dydx=2(y−5)x\frac{dy}{dx} = \frac{2(y-5)}{x}. Now separate variables: dyy−5=2dxx\frac{dy}{y-5} = \frac{2dx}{x}. Integrate both sides: ∫dyy−5=∫2dxx\int \frac{dy}{y-5} = \int \frac{2dx}{x}. This gives you ln⁡∣y−5∣=2ln⁡∣x∣+C=ln⁡(x2)+C\ln|y-5| = 2\ln|x| + C = \ln(x^2) + C. Exponentiating both sides: ∣y−5∣=eln⁡(x2)+C=Ax2|y-5| = e^{\ln(x^2) + C} = Ax^2 where A=eCA = e^C. Since we can absorb the absolute value into the constant, we get y−5=Ax2y-5 = Ax^2, so y=Ax2+5y = Ax^2 + 5. Apply the initial condition y(1)=10y(1) = 10: 10=A(1)2+510 = A(1)^2 + 5, which gives A=5A = 5. Therefore, y=5x2+5y = 5x^2 + 5, which is choice B. Choice A incorrectly uses ex2e^{x^2} instead of x2x^2 - this would come from mishandling the integration. Choice C has the wrong constant term (9 instead of 5) and coefficient, suggesting errors in applying the initial condition. Choice D uses ln⁡(x2)\ln(x^2) directly without exponentiating, which represents an incomplete solution to the differential equation. Remember: for separable equations, always separate variables completely before integrating, and don't forget to apply your initial conditions to find the specific constant.
  13. The solution y(x)y(x) to dydx=2yx\frac{dy}{dx} = \frac{2y}{x} satisfies y(−1)=−3y(-1) = -3. Find the value of y(−e)y(-e).
    Answer: −3e2-3e^2 When you encounter a differential equation of the form dydx=kyx\frac{dy}{dx} = \frac{ky}{x}, you're dealing with a separable equation that requires careful handling of the initial condition and domain considerations. First, separate variables: dyy=2dxx\frac{dy}{y} = \frac{2dx}{x}. Integrating both sides gives ln⁡∣y∣=2ln⁡∣x∣+C\ln|y| = 2\ln|x| + C, which simplifies to ∣y∣=A∣x∣2|y| = A|x|^2 where A=eCA = e^C. Since we need y(x)=±A∣x∣2y(x) = \pm A|x|^2, we must determine the sign using our initial condition. With y(−1)=−3y(-1) = -3, we get −3=±A∣−1∣2=±A(1)-3 = \pm A|-1|^2 = \pm A(1), so A=3A = 3 and we need the negative branch: y(x)=−3∣x∣2y(x) = -3|x|^2. For x<0x < 0 (our domain of interest), ∣x∣=−x|x| = -x, so y(x)=−3(−x)2=−3x2y(x) = -3(-x)^2 = -3x^2. Therefore, y(−e)=−3(−e)2=−3e2y(-e) = -3(-e)^2 = -3e^2. Let's examine why the other answers are incorrect: **A) 3/e23/e^2**: This has the wrong sign (positive instead of negative) and inverts the exponential term. **B) 3e23e^2**: This only has the wrong sign—it's the positive version of our answer. **C) −3-3**: This ignores the x2x^2 factor entirely, treating the solution as constant. Strategy tip: When solving separable differential equations with initial conditions in different domains (positive vs. negative xx), always check how absolute value expressions behave in your specific region. The sign of your solution often depends on which branch you're working with.
  14. The solution to (1+x2)y′−2xy2=0(1+x^2)y' - 2xy^2 = 0 passes through the point (0,1)(0, 1). What is the value of y(1)y(1)?
    Answer: 11−ln⁡(2)\frac{1}{1 - \ln(2)} When you encounter a differential equation like (1+x2)y′−2xy2=0(1+x^2)y' - 2xy^2 = 0, recognize this as a separable differential equation. The key is to rearrange terms so all yy terms are on one side and all xx terms are on the other. First, rewrite the equation: (1+x2)y′=2xy2(1+x^2)y' = 2xy^2, so y′=2xy21+x2y' = \frac{2xy^2}{1+x^2} Since y′=dydxy' = \frac{dy}{dx}, we can separate variables: dyy2=2x1+x2dx\frac{dy}{y^2} = \frac{2x}{1+x^2}dx Integrating both sides: ∫y−2dy=∫2x1+x2dx\int y^{-2}dy = \int \frac{2x}{1+x^2}dx The left side gives −1y-\frac{1}{y}. For the right side, use substitution u=1+x2u = 1+x^2, so du=2xdxdu = 2x dx: ∫2x1+x2dx=∫duu=ln⁡∣u∣=ln⁡(1+x2)\int \frac{2x}{1+x^2}dx = \int \frac{du}{u} = \ln|u| = \ln(1+x^2) Therefore: −1y=ln⁡(1+x2)+C-\frac{1}{y} = \ln(1+x^2) + C Using the initial condition (0,1)(0,1): −11=ln⁡(1)+C-\frac{1}{1} = \ln(1) + C, so C=−1C = -1. The solution becomes: −1y=ln⁡(1+x2)−1-\frac{1}{y} = \ln(1+x^2) - 1 Solving for yy: y=−1ln⁡(1+x2)−1=11−ln⁡(1+x2)y = \frac{-1}{\ln(1+x^2) - 1} = \frac{1}{1 - \ln(1+x^2)} At x=1x = 1: y(1)=11−ln⁡(2)y(1) = \frac{1}{1 - \ln(2)} This confirms answer D. Answers A, B, and C likely result from integration errors, incorrect separation of variables, or sign mistakes during algebraic manipulation. Strategy tip: Always verify your solution satisfies both the differential equation and initial condition—this catches most algebraic errors in separable differential equations.
  15. What is the particular solution to the differential equation xy′=yxy' = \sqrt{y} given the initial condition y(1)=4y(1) = 4?
    Answer: y=14(ln⁡(x)+4)2y = \frac{1}{4}(\ln(x) + 4)^2 This is a separable differential equation, which means you can isolate all terms with yy on one side and all terms with xx on the other. When you see xy′=yxy' = \sqrt{y}, rewrite y′y' as dydx\frac{dy}{dx} to get xdydx=yx\frac{dy}{dx} = \sqrt{y}. To separate variables, divide both sides by y\sqrt{y} and multiply by dxdx: dyy=dxx\frac{dy}{\sqrt{y}} = \frac{dx}{x}. Now integrate both sides. The left side becomes ∫y−1/2dy=2y\int y^{-1/2} dy = 2\sqrt{y}, and the right side becomes ∫dxx=ln⁡(x)+C\int \frac{dx}{x} = \ln(x) + C. This gives us 2y=ln⁡(x)+C2\sqrt{y} = \ln(x) + C. Using the initial condition y(1)=4y(1) = 4: 24=ln⁡(1)+C2\sqrt{4} = \ln(1) + C, so 4=0+C4 = 0 + C, meaning C=4C = 4. Therefore, 2y=ln⁡(x)+42\sqrt{y} = \ln(x) + 4. Solving for yy: y=ln⁡(x)+42\sqrt{y} = \frac{\ln(x) + 4}{2}, so y=(ln⁡(x)+42)2=14(ln⁡(x)+4)2y = \left(\frac{\ln(x) + 4}{2}\right)^2 = \frac{1}{4}(\ln(x) + 4)^2. Answer choice A incorrectly assumes C=2C = 2 instead of C=4C = 4. Choice B treats this as a first-order linear equation rather than separable, leading to an incorrect form. Choice C has the wrong constant and missing the factor of 14\frac{1}{4} that comes from squaring the fraction. When solving separable differential equations, always check your constant of integration carefully using the initial condition, and be meticulous about algebraic manipulation when solving for the dependent variable.
  16. A particle moves along a line such that its velocity v(t)v(t) satisfies dvdt=−2tv2\frac{dv}{dt} = -2tv^2 with v(0)=13v(0) = \frac{1}{3}. At what time does the velocity reach 16\frac{1}{6}?
    Answer: t=3t = \sqrt{3} Separating variables: dvv2=−2t dt\frac{dv}{v^2} = -2t \, dt. Integrating: ∫v−2dv=∫−2t dt\int v^{-2} dv = \int -2t \, dt gives −1v=−t2+C-\frac{1}{v} = -t^2 + C. Using v(0)=13v(0) = \frac{1}{3}: −3=0+C-3 = 0 + C, so C=−3C = -3. Therefore −1v=−t2−3-\frac{1}{v} = -t^2 - 3, which gives 1v=t2+3\frac{1}{v} = t^2 + 3, so v=1t2+3v = \frac{1}{t^2 + 3}. When v=16v = \frac{1}{6}: 16=1t2+3\frac{1}{6} = \frac{1}{t^2 + 3}, so t2+3=6t^2 + 3 = 6, giving t2=3t^2 = 3 and t=3t = \sqrt{3} (taking the positive root since we're looking for a future time).
  17. A solution to dydx=3x2+12y\frac{dy}{dx} = \frac{3x^2+1}{2y} passes through the point (1,2)(1, 2). What is the value of yy when x=0x=0?
    Answer: 2\sqrt{2} This is a separable differential equation problem where you need to find a particular solution using an initial condition. When you see dydx=f(x)g(y)\frac{dy}{dx} = \frac{f(x)}{g(y)}, you can separate variables by multiplying both sides by g(y)dxg(y)dx, giving you g(y)dy=f(x)dxg(y)dy = f(x)dx. Starting with dydx=3x2+12y\frac{dy}{dx} = \frac{3x^2+1}{2y}, multiply both sides by 2ydx2y dx to get 2ydy=(3x2+1)dx2y dy = (3x^2+1)dx. Now integrate both sides: ∫2ydy=∫(3x2+1)dx\int 2y dy = \int (3x^2+1)dx, which gives you y2=x3+x+Cy^2 = x^3 + x + C. To find the constant CC, use the initial condition that the solution passes through (1,2)(1, 2). Substituting: 22=13+1+C2^2 = 1^3 + 1 + C, so 4=2+C4 = 2 + C, meaning C=2C = 2. Your particular solution is y2=x3+x+2y^2 = x^3 + x + 2. When x=0x = 0: y2=03+0+2=2y^2 = 0^3 + 0 + 2 = 2, so y=2y = \sqrt{2}, which is answer C. Looking at the wrong answers: A) 3\sqrt{3} would result from incorrectly calculating C=3C = 3 instead of C=2C = 2. B) 22 is the y-value from the initial condition, which some students mistakenly think remains constant. D) 00 would come from forgetting to include the constant of integration entirely. Remember: with separable differential equations, always separate variables first, integrate both sides, then use the initial condition to find your constant. The initial condition gives you one point, but you need it to find the entire solution curve.
  18. Find the particular solution y=f(x)y=f(x) to the differential equation y′=y2/xy' = y^2 / x with the initial condition y(1)=−1/2y(1) = -1/2. On what largest open interval is this solution defined?
    Answer: (e−2,∞)(e^{-2}, \infty) Separate the variables: 1y2dy=1xdx\frac{1}{y^2} dy = \frac{1}{x} dx. Integrate both sides: −1y=ln⁡∣x∣+C-\frac{1}{y} = \ln|x| + C. Use the initial condition y(1)=−1/2y(1) = -1/2: −1−1/2=ln⁡∣1∣+C  ⟹  2=0+C  ⟹  C=2-\frac{1}{-1/2} = \ln|1| + C \implies 2 = 0 + C \implies C = 2. The particular solution is −1y=ln⁡∣x∣+2-\frac{1}{y} = \ln|x| + 2. Since the initial condition is at x=1>0x=1>0, we can write −1y=ln⁡(x)+2-\frac{1}{y} = \ln(x) + 2. Solving for yy gives y=−1ln⁡(x)+2y = \frac{-1}{\ln(x) + 2}. The solution is defined when x>0x>0 (due to ln⁡(x)\ln(x)) and when the denominator is not zero. ln⁡(x)+2≠0  ⟹  ln⁡(x)≠−2  ⟹  x≠e−2\ln(x) + 2 \neq 0 \implies \ln(x) \neq -2 \implies x \neq e^{-2}. The domain is (0,e−2)∪(e−2,∞)(0, e^{-2}) \cup (e^{-2}, \infty). The initial condition x=1x=1 is in the interval (e−2,∞)(e^{-2}, \infty) because e−2≈0.135<1e^{-2} \approx 0.135 < 1. Therefore, the largest open interval containing x=1x=1 where the solution is defined is (e−2,∞)(e^{-2}, \infty).
  19. Consider the differential equation dydx=cos⁡(x)y2 \frac{dy}{dx} = \frac{\cos(x)}{y^2} with the initial condition y(π/2)=3y(\pi/2) = 3. What is the value of y(0)y(0)?
    Answer: 2332 \sqrt[3]{3} First, separate the variables: y2dy=cos⁡(x)dxy^2 dy = \cos(x) dx. Integrating both sides gives y33=sin⁡(x)+C\frac{y^3}{3} = \sin(x) + C. Use the initial condition y(π/2)=3y(\pi/2) = 3 to find CC: 333=sin⁡(π/2)+C  ⟹  9=1+C  ⟹  C=8\frac{3^3}{3} = \sin(\pi/2) + C \implies 9 = 1 + C \implies C = 8. The particular solution is y33=sin⁡(x)+8\frac{y^3}{3} = \sin(x) + 8, or y3=3sin⁡(x)+24y^3 = 3\sin(x) + 24. To find y(0)y(0), substitute x=0x=0: y3=3sin⁡(0)+24=24y^3 = 3\sin(0) + 24 = 24. Thus, y(0)=243=8⋅33=233y(0) = \sqrt[3]{24} = \sqrt[3]{8 \cdot 3} = 2\sqrt[3]{3}.
  20. Find the implicit solution to the differential equation (y−1)dydx=x2(y-1)\frac{dy}{dx} = x^2 with the initial condition y(3)=1y(3)=1.
    Answer: y2−2y−2x3/3=−19y^2 - 2y - 2x^3/3 = -19 When you encounter a separable differential equation like this, your goal is to separate variables and integrate both sides, then apply the initial condition to find the constant of integration. Starting with (y−1)dydx=x2(y-1)\frac{dy}{dx} = x^2, you can separate variables by moving all terms with yy to one side and all terms with xx to the other: (y−1)dy=x2dx(y-1)dy = x^2 dx. Now integrate both sides. The left side gives you ∫(y−1)dy=y22−y\int (y-1)dy = \frac{y^2}{2} - y, and the right side gives you ∫x2dx=x33\int x^2 dx = \frac{x^3}{3}. This yields y22−y=x33+C\frac{y^2}{2} - y = \frac{x^3}{3} + C. Multiplying through by 2 to clear fractions: y2−2y=2x33+2Cy^2 - 2y = \frac{2x^3}{3} + 2C. Let K=2CK = 2C, so y2−2y−2x33=Ky^2 - 2y - \frac{2x^3}{3} = K. Apply the initial condition y(3)=1y(3) = 1: 12−2(1)−2(3)33=K1^2 - 2(1) - \frac{2(3)^3}{3} = K, which gives 1−2−543=1−2−18=−191 - 2 - \frac{54}{3} = 1 - 2 - 18 = -19. Therefore, the solution is y2−2y−2x33=−19y^2 - 2y - \frac{2x^3}{3} = -19, which is answer B. Answer A has the wrong constant (-1 instead of -19). Answer C uses x3x^3 instead of 2x33\frac{2x^3}{3} and has the wrong constant. Answer D appears to use substitution methods inappropriately—this equation doesn't require logarithmic techniques since it's directly separable. Always apply initial conditions after finding the general solution to determine the specific constant value. Double-check your integration, especially with fractions.

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