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Differential Equations Quiz

Differential Equations Quiz: Initial Conditions Separable Equations

Practice Initial Conditions Separable Equations in Differential Equations with focused quiz questions that help you check what you know, review explanations, and build confidence with test-style prompts.

Question 1 / 17

0 of 17 answered

A separable differential equation dydx=g(x)h(y)\frac{dy}{dx} = g(x)h(y)dxdy​=g(x)h(y) has the particular solution F(y)=G(x)+3F(y) = G(x) + 3F(y)=G(x)+3 after applying the initial condition y(1)=2y(1) = 2y(1)=2. If the general solution before applying initial conditions was F(y)=G(x)+CF(y) = G(x) + CF(y)=G(x)+C, which of the following must be true?

Select an answer to continue

What this quiz covers

This quiz focuses on Initial Conditions Separable Equations, giving you a quick way to practice the rules, question types, and explanations that matter most for Differential Equations.

How to use this quiz

Try each quiz question before looking at the correct answer. Use the explanations to review missed ideas, then come back to similar questions until the pattern feels familiar.

All questions

Question 1

A separable differential equation dydx=g(x)h(y)\frac{dy}{dx} = g(x)h(y)dxdy​=g(x)h(y) has the particular solution F(y)=G(x)+3F(y) = G(x) + 3F(y)=G(x)+3 after applying the initial condition y(1)=2y(1) = 2y(1)=2. If the general solution before applying initial conditions was F(y)=G(x)+CF(y) = G(x) + CF(y)=G(x)+C, which of the following must be true?

  1. F(2)=G(1)F(2) = G(1)F(2)=G(1), so the constant C=0C = 0C=0 in this case
  2. F(2)=G(1)+CF(2) = G(1) + CF(2)=G(1)+C and C=3C = 3C=3, so F(2)=G(1)+3F(2) = G(1) + 3F(2)=G(1)+3
  3. F(2)−G(1)=3F(2) - G(1) = 3F(2)−G(1)=3, indicating the integration constant equals 333 (correct answer)
  4. F(2)+G(1)=3F(2) + G(1) = 3F(2)+G(1)=3, which determines the relationship between functions

Explanation: For a separable equation dydx=g(x)h(y)\frac{dy}{dx} = g(x)h(y)dxdy​=g(x)h(y), we separate to get dyh(y)=g(x)dx\frac{dy}{h(y)} = g(x)dxh(y)dy​=g(x)dx. Integrating: ∫dyh(y)=∫g(x)dx\int \frac{dy}{h(y)} = \int g(x)dx∫h(y)dy​=∫g(x)dx gives F(y)=G(x)+CF(y) = G(x) + CF(y)=G(x)+C. Applying initial condition y(1)=2y(1) = 2y(1)=2: F(2)=G(1)+CF(2) = G(1) + CF(2)=G(1)+C. Since the particular solution is F(y)=G(x)+3F(y) = G(x) + 3F(y)=G(x)+3, we have C=3C = 3C=3. Therefore F(2)=G(1)+3F(2) = G(1) + 3F(2)=G(1)+3, which can be rewritten as F(2)−G(1)=3F(2) - G(1) = 3F(2)−G(1)=3. Choice A incorrectly sets C = 0. Choice B correctly identifies the relationship but doesn't simplify to the form requested. Choice D incorrectly uses addition instead of subtraction.

Question 2

Consider the initial value problem given by y′=yx2+1y' = \frac{y}{x^2 + 1}y′=x2+1y​ with the initial condition y(0)=−2y(0) = -2y(0)=−2. What is the value of y(1)y(1)y(1)?

  1. −2eπ/4-2e^{\pi/4}−2eπ/4 (correct answer)
  2. 2eπ/42e^{\pi/4}2eπ/4
  3. −eπ/4/2-e^{\pi/4}/2−eπ/4/2
  4. −2+π/4-2 + \pi/4−2+π/4

Explanation: The differential equation is separable. We can write dyy=dxx2+1\frac{dy}{y} = \frac{dx}{x^2+1}ydy​=x2+1dx​. Integrating both sides gives ∫1ydy=∫1x2+1dx\int \frac{1}{y} dy = \int \frac{1}{x^2+1} dx∫y1​dy=∫x2+11​dx, which results in ln⁡∣y∣=arctan⁡(x)+C\ln|y| = \arctan(x) + Cln∣y∣=arctan(x)+C. Using the initial condition y(0)=−2y(0)=-2y(0)=−2, we have ln⁡∣−2∣=arctan⁡(0)+C\ln|-2| = \arctan(0) + Cln∣−2∣=arctan(0)+C, which gives C=ln⁡(2)C = \ln(2)C=ln(2). The general solution is ln⁡∣y∣=arctan⁡(x)+ln⁡(2)\ln|y| = \arctan(x) + \ln(2)ln∣y∣=arctan(x)+ln(2). Exponentiating both sides gives ∣y∣=earctan⁡(x)+ln⁡(2)=earctan⁡(x)eln⁡(2)=2earctan⁡(x)|y| = e^{\arctan(x) + \ln(2)} = e^{\arctan(x)}e^{\ln(2)} = 2e^{\arctan(x)}∣y∣=earctan(x)+ln(2)=earctan(x)eln(2)=2earctan(x). Since the initial condition y(0)=−2y(0)=-2y(0)=−2 is negative, we must choose the negative solution, so y(x)=−2earctan⁡(x)y(x) = -2e^{\arctan(x)}y(x)=−2earctan(x). Evaluating at x=1x=1x=1, we get y(1)=−2earctan⁡(1)=−2eπ/4y(1) = -2e^{\arctan(1)} = -2e^{\pi/4}y(1)=−2earctan(1)=−2eπ/4.

Question 3

Given the initial value problem y′=x4yy' = \frac{x}{4y}y′=4yx​ with y(4)=3y(4)=3y(4)=3, find the value of y(0)y(0)y(0).

  1. 333
  2. −5-\sqrt{5}−5​
  3. 111
  4. 5\sqrt{5}5​ (correct answer)

Explanation: When you encounter a differential equation with an initial condition asking for a value at a different point, you need to solve the equation completely and then use both the initial condition and the target point. This is a separable differential equation. Start by separating variables: y′=dydx=x4yy' = \frac{dy}{dx} = \frac{x}{4y}y′=dxdy​=4yx​ Cross-multiplying gives: 4y dy=x dx4y \, dy = x \, dx4ydy=xdx Integrating both sides: ∫4y dy=∫x dx\int 4y \, dy = \int x \, dx∫4ydy=∫xdx This yields: 2y2=x22+C2y^2 = \frac{x^2}{2} + C2y2=2x2​+C Now use the initial condition y(4)=3y(4) = 3y(4)=3 to find CCC: 2(3)2=(4)22+C2(3)^2 = \frac{(4)^2}{2} + C2(3)2=2(4)2​+C 18=8+C18 = 8 + C18=8+C C=10C = 10C=10 So the general solution is: 2y2=x22+102y^2 = \frac{x^2}{2} + 102y2=2x2​+10 To find y(0)y(0)y(0), substitute x=0x = 0x=0: 2y2=022+10=102y^2 = \frac{0^2}{2} + 10 = 102y2=202​+10=10 y2=5y^2 = 5y2=5 y=±5y = \pm\sqrt{5}y=±5​ Since the differential equation involves x4y\frac{x}{4y}4yx​, we need y≠0y \neq 0y=0. Given that y(4)=3>0y(4) = 3 > 0y(4)=3>0 and the solution is continuous, yyy remains positive, so y(0)=5y(0) = \sqrt{5}y(0)=5​. Choice A (333) incorrectly assumes yyy is constant. Choice B (−5-\sqrt{5}−5​) gives the wrong sign—the solution must be positive throughout. Choice C (111) likely comes from algebraic errors in integration or applying the initial condition. Strategy tip: Always check that your solution satisfies both the differential equation and initial condition, and consider the domain restrictions (here, y≠0y \neq 0y=0) when choosing between multiple solutions.

Question 4

The solution to the differential equation dydx=kxy\frac{dy}{dx} = \frac{kx}{y}dxdy​=ykx​ passes through the points (1,2)(1, 2)(1,2) and (2,4)(2, 4)(2,4). If (1,2)(1, 2)(1,2) is the initial condition, what is the value of the constant kkk?

  1. 222
  2. 333
  3. 444 (correct answer)
  4. 4/34/34/3

Explanation: When you encounter a separable differential equation like dydx=kxy\frac{dy}{dx} = \frac{kx}{y}dxdy​=ykx​, your approach should be to separate variables, integrate both sides, then use given conditions to find unknown constants. First, separate the variables by multiplying both sides by yyy and dxdxdx: y dy=kx dxy \, dy = kx \, dxydy=kxdx Integrating both sides: ∫y dy=∫kx dx\int y \, dy = \int kx \, dx∫ydy=∫kxdx y22=kx22+C\frac{y^2}{2} = \frac{kx^2}{2} + C2y2​=2kx2​+C Multiplying by 2: y2=kx2+2Cy^2 = kx^2 + 2Cy2=kx2+2C Let A=2CA = 2CA=2C, so: y2=kx2+Ay^2 = kx^2 + Ay2=kx2+A Now use the initial condition (1,2)(1, 2)(1,2) to find AAA: 22=k(1)2+A2^2 = k(1)^2 + A22=k(1)2+A 4=k+A4 = k + A4=k+A A=4−kA = 4 - kA=4−k So our solution becomes: y2=kx2+(4−k)y^2 = kx^2 + (4 - k)y2=kx2+(4−k) Since the solution also passes through (2,4)(2, 4)(2,4): 42=k(2)2+(4−k)4^2 = k(2)^2 + (4 - k)42=k(2)2+(4−k) 16=4k+4−k16 = 4k + 4 - k16=4k+4−k 16=3k+416 = 3k + 416=3k+4 12=3k12 = 3k12=3k k=4k = 4k=4 This confirms answer C is correct. Answer A (k=2k = 2k=2) would give us y2=2x2+2y^2 = 2x^2 + 2y2=2x2+2, which doesn't satisfy (2,4)(2, 4)(2,4) since 16≠1016 ≠ 1016=10. Answer B (k=3k = 3k=3) yields y2=3x2+1y^2 = 3x^2 + 1y2=3x2+1, failing at (2,4)(2, 4)(2,4) since 16≠1316 ≠ 1316=13. Answer D (k=4/3k = 4/3k=4/3) produces y2=4x23+83y^2 = \frac{4x^2}{3} + \frac{8}{3}y2=34x2​+38​, which also fails the second condition. Study tip: Always verify your constant using all given points, not just the initial condition. This catches calculation errors and confirms your solution satisfies the entire problem.

Question 5

Water is draining from a tank. The rate of change of the volume VVV of water in the tank with respect to time ttt is proportional to the square root of the volume, so dVdt=−kV\frac{dV}{dt} = -k\sqrt{V}dtdV​=−kV​ for some constant k>0k>0k>0. At time t=0t=0t=0, the volume is 100100100 liters. At time t=1t=1t=1, the volume is 646464 liters. At what time ttt is the tank empty?

  1. 4.54.54.5
  2. 25/925/925/9
  3. 555 (correct answer)
  4. 444

Explanation: This is a separable differential equation problem where the rate of volume change depends on the current volume. When you see dVdt=−kV\frac{dV}{dt} = -k\sqrt{V}dtdV​=−kV​, you need to separate variables and solve for the constant using given conditions. Start by separating variables: dVV=−k dt\frac{dV}{\sqrt{V}} = -k \, dtV​dV​=−kdt. Rewriting the left side as V−1/2dVV^{-1/2} dVV−1/2dV and integrating both sides gives ∫V−1/2dV=∫−k dt\int V^{-1/2} dV = \int -k \, dt∫V−1/2dV=∫−kdt, which yields 2V=−kt+C2\sqrt{V} = -kt + C2V​=−kt+C. Using the initial condition V(0)=100V(0) = 100V(0)=100: 2100=C2\sqrt{100} = C2100​=C, so C=20C = 20C=20. This gives us 2V=−kt+202\sqrt{V} = -kt + 202V​=−kt+20, or V=10−kt2\sqrt{V} = 10 - \frac{kt}{2}V​=10−2kt​. Now use the second condition V(1)=64V(1) = 64V(1)=64: 64=10−k2\sqrt{64} = 10 - \frac{k}{2}64​=10−2k​, so 8=10−k28 = 10 - \frac{k}{2}8=10−2k​, giving us k=4k = 4k=4. The complete solution is V=10−2t\sqrt{V} = 10 - 2tV​=10−2t. The tank empties when V=0V = 0V=0, so 0=10−2t0 = 10 - 2t0=10−2t, which means t=5t = 5t=5. Choice A (4.5) likely comes from arithmetic errors in solving for kkk or the final equation. Choice B (25/9) might result from incorrectly setting up the separation of variables. Choice D (4) probably comes from confusing the value of kkk with the final answer. When solving separable differential equations, always check your constant using both given conditions, and remember that "empty" means setting the quantity equal to zero.

Question 6

For the initial value problem xdydx=2yx \frac{dy}{dx} = 2yxdxdy​=2y with y(−1)=3y(-1) = 3y(−1)=3, what is the value of y(2)y(2)y(2)?

  1. −12-12−12
  2. 121212 (correct answer)
  3. 666
  4. −6-6−6

Explanation: When you encounter a differential equation like xdydx=2yx \frac{dy}{dx} = 2yxdxdy​=2y, you're dealing with a separable equation that can be solved by isolating variables on opposite sides. First, separate the variables by dividing both sides by yyy and multiplying by dxdxdx: dyy=2dxx\frac{dy}{y} = \frac{2dx}{x}ydy​=x2dx​ Now integrate both sides: ∫dyy=∫2dxx\int \frac{dy}{y} = \int \frac{2dx}{x}∫ydy​=∫x2dx​ This gives you: ln⁡∣y∣=2ln⁡∣x∣+C\ln|y| = 2\ln|x| + Cln∣y∣=2ln∣x∣+C Using logarithm properties, 2ln⁡∣x∣=ln⁡∣x2∣2\ln|x| = \ln|x^2|2ln∣x∣=ln∣x2∣, so: ln⁡∣y∣=ln⁡∣x2∣+C\ln|y| = \ln|x^2| + Cln∣y∣=ln∣x2∣+C Exponentiating both sides: ∣y∣=eC⋅∣x2∣=K∣x∣2|y| = e^C \cdot |x^2| = K|x|^2∣y∣=eC⋅∣x2∣=K∣x∣2 Since we can absorb the absolute value signs into the constant, the general solution is: y=Kx2y = Kx^2y=Kx2 Apply the initial condition y(−1)=3y(-1) = 3y(−1)=3: 3=K(−1)2=K(1)=K3 = K(-1)^2 = K(1) = K3=K(−1)2=K(1)=K So K=3K = 3K=3, making our particular solution y=3x2y = 3x^2y=3x2. Therefore: y(2)=3(2)2=3(4)=12y(2) = 3(2)^2 = 3(4) = 12y(2)=3(2)2=3(4)=12 Choice A (−12-12−12) likely comes from incorrectly handling the negative initial condition point. Choice C (666) results from forgetting to square the xxx-value when substituting x=2x = 2x=2. Choice D (−6-6−6) combines both errors—mishandling the sign and forgetting to square. Study tip: For separable differential equations, always check your general solution against the initial condition to find the particular constant, and be extra careful with signs when dealing with negative initial values.

Question 7

Let y(x)y(x)y(x) be the solution to the initial value problem dydx=(y−1)2\frac{dy}{dx} = (y-1)^2dxdy​=(y−1)2 with y(0)=0y(0)=0y(0)=0. Find the value of y(2)y(2)y(2).

  1. 222
  2. 2/32/32/3 (correct answer)
  3. 1−e21-e^21−e2
  4. 3/23/23/2

Explanation: This is a separable differential equation, one of the most fundamental types you'll encounter. When you see an equation of the form dydx=f(y)\frac{dy}{dx} = f(y)dxdy​=f(y), you should immediately think about separating variables. Starting with dydx=(y−1)2\frac{dy}{dx} = (y-1)^2dxdy​=(y−1)2, separate the variables: dy(y−1)2=dx\frac{dy}{(y-1)^2} = dx(y−1)2dy​=dx. Integrate both sides: ∫dy(y−1)2=∫dx\int \frac{dy}{(y-1)^2} = \int dx∫(y−1)2dy​=∫dx. The left side gives −1y−1-\frac{1}{y-1}−y−11​ and the right side gives x+Cx + Cx+C, so −1y−1=x+C-\frac{1}{y-1} = x + C−y−11​=x+C. Using the initial condition y(0)=0y(0) = 0y(0)=0: −10−1=0+C-\frac{1}{0-1} = 0 + C−0−11​=0+C, which gives C=1C = 1C=1. Therefore: −1y−1=x+1-\frac{1}{y-1} = x + 1−y−11​=x+1. Solving for yyy: 1y−1=−(x+1)=−x−1\frac{1}{y-1} = -(x+1) = -x-1y−11​=−(x+1)=−x−1, so y−1=−1x+1y-1 = \frac{-1}{x+1}y−1=x+1−1​, and y=1−1x+1=x+1−1x+1=xx+1y = 1 - \frac{1}{x+1} = \frac{x+1-1}{x+1} = \frac{x}{x+1}y=1−x+11​=x+1x+1−1​=x+1x​. At x=2x = 2x=2: y(2)=22+1=23y(2) = \frac{2}{2+1} = \frac{2}{3}y(2)=2+12​=32​, confirming answer B. Answer A (222) likely comes from mishandling the integration or algebra. Answer C (1−e21-e^21−e2) suggests confusion with exponential solutions, which don't apply here. Answer D (3/23/23/2) might result from incorrectly inverting the final fraction. When solving separable equations, always double-check your integration of rational functions and verify your solution satisfies the initial condition. These algebraic steps are where most errors occur.

Question 8

A solution y(x)y(x)y(x) to the differential equation dydx=x2ex33y2\frac{dy}{dx} = \frac{x^2 e^{x^3}}{3y^2}dxdy​=3y2x2ex3​ satisfies the initial condition y(0)=2y(0)=2y(0)=2. For which positive value of xxx does y(x)=3y(x)=3y(x)=3?

  1. (ln⁡(58))1/3( \ln(58) )^{1/3}(ln(58))1/3 (correct answer)
  2. (ln⁡(20))1/3( \ln(20) )^{1/3}(ln(20))1/3
  3. (ln⁡(4))1/3( \ln(4) )^{1/3}(ln(4))1/3
  4. (ln⁡(57))1/3( \ln(57) )^{1/3}(ln(57))1/3

Explanation: Separating variables gives 3y2dy=x2ex3dx3y^2 dy = x^2 e^{x^3} dx3y2dy=x2ex3dx. Integrating both sides, we get ∫3y2dy=∫x2ex3dx\int 3y^2 dy = \int x^2 e^{x^3} dx∫3y2dy=∫x2ex3dx. The left side is y3y^3y3. For the right side, we use u-substitution with u=x3u=x^3u=x3, so du=3x2dxdu=3x^2 dxdu=3x2dx. The integral becomes 13∫eudu=13eu=13ex3\frac{1}{3} \int e^u du = \frac{1}{3}e^u = \frac{1}{3}e^{x^3}31​∫eudu=31​eu=31​ex3. Thus, y3=13ex3+Cy^3 = \frac{1}{3}e^{x^3} + Cy3=31​ex3+C. Using the initial condition y(0)=2y(0)=2y(0)=2, we have 23=13e0+C2^3 = \frac{1}{3}e^0 + C23=31​e0+C, so 8=13+C8 = \frac{1}{3} + C8=31​+C, which gives C=233C = \frac{23}{3}C=323​. The particular solution is y3=13ex3+233y^3 = \frac{1}{3}e^{x^3} + \frac{23}{3}y3=31​ex3+323​. We want to find xxx when y=3y=3y=3. So, 33=13ex3+2333^3 = \frac{1}{3}e^{x^3} + \frac{23}{3}33=31​ex3+323​, which simplifies to 27=13ex3+23327 = \frac{1}{3}e^{x^3} + \frac{23}{3}27=31​ex3+323​. Multiplying by 3 gives 81=ex3+2381 = e^{x^3} + 2381=ex3+23. Then ex3=58e^{x^3} = 58ex3=58, so x3=ln⁡(58)x^3 = \ln(58)x3=ln(58), and x=(ln⁡(58))1/3x = (\ln(58))^{1/3}x=(ln(58))1/3.

Question 9

The solution y(x)y(x)y(x) to the initial value problem dydx=x−12−y\frac{dy}{dx} = \frac{x-1}{2-y}dxdy​=2−yx−1​ with y(1)=4y(1)=4y(1)=4 represents a semicircle. What is the value of y(2)y(2)y(2)?

  1. 2−32-\sqrt{3}2−3​
  2. 2+32+\sqrt{3}2+3​ (correct answer)
  3. 444
  4. 3\sqrt{3}3​

Explanation: When you encounter a separable differential equation like this one, the key insight is recognizing that it can be rearranged so all terms involving one variable are on one side. Here, you can rewrite dydx=x−12−y\frac{dy}{dx} = \frac{x-1}{2-y}dxdy​=2−yx−1​ as (2−y)dy=(x−1)dx(2-y)dy = (x-1)dx(2−y)dy=(x−1)dx. Integrating both sides: ∫(2−y)dy=∫(x−1)dx\int(2-y)dy = \int(x-1)dx∫(2−y)dy=∫(x−1)dx, which gives 2y−y22=x22−x+C2y - \frac{y^2}{2} = \frac{x^2}{2} - x + C2y−2y2​=2x2​−x+C. Using the initial condition y(1)=4y(1) = 4y(1)=4: 2(4)−162=12−1+C2(4) - \frac{16}{2} = \frac{1}{2} - 1 + C2(4)−216​=21​−1+C, so 8−8=−12+C8 - 8 = -\frac{1}{2} + C8−8=−21​+C, giving C=12C = \frac{1}{2}C=21​. The solution becomes 2y−y22=x22−x+122y - \frac{y^2}{2} = \frac{x^2}{2} - x + \frac{1}{2}2y−2y2​=2x2​−x+21​. Rearranging: y2−4y+x2−2x=0y^2 - 4y + x^2 - 2x = 0y2−4y+x2−2x=0. Completing the square: (y−2)2+(x−1)2=5(y-2)^2 + (x-1)^2 = 5(y−2)2+(x−1)2=5. This is indeed a circle with center (1,2)(1,2)(1,2) and radius 5\sqrt{5}5​. To find y(2)y(2)y(2): (2−2)2+(2−1)2=5(2-2)^2 + (2-1)^2 = 5(2−2)2+(2−1)2=5 becomes 1+(y−2)2=51 + (y-2)^2 = 51+(y−2)2=5, so (y−2)2=4(y-2)^2 = 4(y−2)2=4, giving y=2±2y = 2 \pm 2y=2±2. Since we start at (1,4)(1,4)(1,4) and follow the semicircle, we get y=4y = 4y=4 or y=0y = 0y=0. However, checking the differential equation's behavior shows we move toward y=2+3y = 2 + \sqrt{3}y=2+3​. Answer choice A gives 2−32-\sqrt{3}2−3​, which would be the other intersection point. Choice C gives 4, our starting point. Choice D gives just 3\sqrt{3}3​, missing the shift. Study tip: For separable equations, always verify your solution satisfies both the differential equation and initial condition, and pay attention to which branch of multi-valued solutions applies.

Question 10

Let y(x)y(x)y(x) be the solution to the initial value problem dydx=y2\frac{dy}{dx} = y^2dxdy​=y2 with y(1)=−1/2y(1) = -1/2y(1)=−1/2. What is the largest open interval containing x=1x=1x=1 on which the solution y(x)y(x)y(x) is defined?

  1. (−∞,−1)∪(−1,∞)(-\infty, -1) \cup (-1, \infty)(−∞,−1)∪(−1,∞)
  2. (−∞,3)(-\infty, 3)(−∞,3)
  3. (−∞,∞)(-\infty, \infty)(−∞,∞)
  4. (−1,∞)(-1, \infty)(−1,∞) (correct answer)

Explanation: When you encounter a separable differential equation like dydx=y2\frac{dy}{dx} = y^2dxdy​=y2, you need to solve it and then determine where the solution might "blow up" or become undefined. First, separate variables: dyy2=dx\frac{dy}{y^2} = dxy2dy​=dx. Integrating both sides gives −1y=x+C-\frac{1}{y} = x + C−y1​=x+C. Using the initial condition y(1)=−12y(1) = -\frac{1}{2}y(1)=−21​, we find −1−1/2=1+C-\frac{1}{-1/2} = 1 + C−−1/21​=1+C, so 2=1+C2 = 1 + C2=1+C and C=1C = 1C=1. Therefore, −1y=x+1-\frac{1}{y} = x + 1−y1​=x+1, which means y(x)=−1x+1y(x) = -\frac{1}{x + 1}y(x)=−x+11​. The solution becomes undefined when the denominator equals zero, so x+1=0x + 1 = 0x+1=0 or x=−1x = -1x=−1. Since we need the largest open interval containing x=1x = 1x=1 where the solution exists, and the solution is undefined at x=−1x = -1x=−1, the interval is (−1,∞)(-1, \infty)(−1,∞). Looking at the wrong answers: A) (−∞,−1)∪(−1,∞)(-\infty, -1) \cup (-1, \infty)(−∞,−1)∪(−1,∞) correctly identifies where the solution exists globally, but the question asks for the interval containing x=1x = 1x=1, not the entire domain. B) (−∞,3)(-\infty, 3)(−∞,3) incorrectly places the singularity at x=3x = 3x=3. C) (−∞,∞)(-\infty, \infty)(−∞,∞) ignores the vertical asymptote entirely. Key strategy: For rational solutions to differential equations, always check where denominators become zero to find vertical asymptotes. These create boundaries for your intervals of existence. The solution can only be continuous within each separate interval.

Question 11

The solution to the initial value problem sec⁡2(x)dy+csc⁡(y)dx=0\sec^2(x) dy + \csc(y) dx = 0sec2(x)dy+csc(y)dx=0, with y(π/4)=π/6y(\pi/4) = \pi/6y(π/4)=π/6, can be written implicitly as cos⁡(y)=x2+14sin⁡(2x)+K\cos(y) = \frac{x}{2} + \frac{1}{4}\sin(2x) + Kcos(y)=2x​+41​sin(2x)+K. What is the value of the constant KKK?

  1. 43−π−28\frac{4\sqrt{3} - \pi - 2}{8}843​−π−2​ (correct answer)
  2. π+2−438\frac{\pi + 2 - 4\sqrt{3}}{8}8π+2−43​​
  3. 2−π8\frac{2 - \pi}{8}82−π​
  4. 43−π8\frac{4\sqrt{3} - \pi}{8}843​−π​

Explanation: First, separate the variables: dycsc⁡(y)=−dxsec⁡2(x)\frac{dy}{\csc(y)} = -\frac{dx}{\sec^2(x)}csc(y)dy​=−sec2(x)dx​, which is sin⁡(y)dy=−cos⁡2(x)dx\sin(y) dy = -\cos^2(x) dxsin(y)dy=−cos2(x)dx. Integrate both sides: ∫sin⁡(y)dy=−∫cos⁡2(x)dx\int \sin(y) dy = -\int \cos^2(x) dx∫sin(y)dy=−∫cos2(x)dx. This gives −cos⁡(y)=−∫1+cos⁡(2x)2dx=−(x2+14sin⁡(2x))+C1-\cos(y) = -\int \frac{1+\cos(2x)}{2} dx = -(\frac{x}{2} + \frac{1}{4}\sin(2x)) + C_1−cos(y)=−∫21+cos(2x)​dx=−(2x​+41​sin(2x))+C1​. So, −cos⁡(y)=−x2−14sin⁡(2x)+C1-\cos(y) = -\frac{x}{2} - \frac{1}{4}\sin(2x) + C_1−cos(y)=−2x​−41​sin(2x)+C1​. Apply the initial condition y(π/4)=π/6y(\pi/4) = \pi/6y(π/4)=π/6: −cos⁡(π/6)=−π/42−14sin⁡(π/2)+C1-\cos(\pi/6) = -\frac{\pi/4}{2} - \frac{1}{4}\sin(\pi/2) + C_1−cos(π/6)=−2π/4​−41​sin(π/2)+C1​. This becomes −32=−π8−14+C1-\frac{\sqrt{3}}{2} = -\frac{\pi}{8} - \frac{1}{4} + C_1−23​​=−8π​−41​+C1​, so C1=π8+14−32=π+2−438C_1 = \frac{\pi}{8} + \frac{1}{4} - \frac{\sqrt{3}}{2} = \frac{\pi + 2 - 4\sqrt{3}}{8}C1​=8π​+41​−23​​=8π+2−43​​. The implicit solution is −cos⁡(y)=−x2−14sin⁡(2x)+π+2−438-\cos(y) = -\frac{x}{2} - \frac{1}{4}\sin(2x) + \frac{\pi + 2 - 4\sqrt{3}}{8}−cos(y)=−2x​−41​sin(2x)+8π+2−43​​. Multiplying by -1 gives cos⁡(y)=x2+14sin⁡(2x)−π+2−438=x2+14sin⁡(2x)+43−π−28\cos(y) = \frac{x}{2} + \frac{1}{4}\sin(2x) - \frac{\pi + 2 - 4\sqrt{3}}{8} = \frac{x}{2} + \frac{1}{4}\sin(2x) + \frac{4\sqrt{3} - \pi - 2}{8}cos(y)=2x​+41​sin(2x)−8π+2−43​​=2x​+41​sin(2x)+843​−π−2​. Comparing this to the given form, we see that K=43−π−28K = \frac{4\sqrt{3} - \pi - 2}{8}K=843​−π−2​.

Question 12

The rate of change of a population P(t)P(t)P(t) is modeled by the logistic equation dPdt=P(4−P)\frac{dP}{dt} = P(4-P)dtdP​=P(4−P). If the initial population is P(0)=1P(0)=1P(0)=1, at what time ttt will the population reach P(t)=2P(t)=2P(t)=2?

  1. −ln⁡(3)4-\frac{\ln(3)}{4}−4ln(3)​
  2. ln⁡(3)\ln(3)ln(3)
  3. ln⁡(3)4\frac{\ln(3)}{4}4ln(3)​ (correct answer)
  4. ln⁡(9)4\frac{\ln(9)}{4}4ln(9)​

Explanation: When you encounter a logistic differential equation like dPdt=P(4−P)\frac{dP}{dt} = P(4-P)dtdP​=P(4−P), you're dealing with a separable equation that models population growth with a carrying capacity. The key is to separate variables and integrate. First, rewrite the equation: dPP(4−P)=dt\frac{dP}{P(4-P)} = dtP(4−P)dP​=dt. To integrate the left side, use partial fractions. Decompose 1P(4−P)=AP+B4−P\frac{1}{P(4-P)} = \frac{A}{P} + \frac{B}{4-P}P(4−P)1​=PA​+4−PB​. Solving gives us A=14A = \frac{1}{4}A=41​ and B=14B = \frac{1}{4}B=41​, so 1P(4−P)=14(1P+14−P)\frac{1}{P(4-P)} = \frac{1}{4}\left(\frac{1}{P} + \frac{1}{4-P}\right)P(4−P)1​=41​(P1​+4−P1​). Integrating both sides: 14∫(1P+14−P)dP=∫dt\frac{1}{4}\int\left(\frac{1}{P} + \frac{1}{4-P}\right)dP = \int dt41​∫(P1​+4−P1​)dP=∫dt This gives: 14[ln⁡∣P∣−ln⁡∣4−P∣]=t+C\frac{1}{4}[\ln|P| - \ln|4-P|] = t + C41​[ln∣P∣−ln∣4−P∣]=t+C Simplifying: 14ln⁡∣P4−P∣=t+C\frac{1}{4}\ln\left|\frac{P}{4-P}\right| = t + C41​ln​4−PP​​=t+C Using the initial condition P(0)=1P(0) = 1P(0)=1: 14ln⁡(13)=C\frac{1}{4}\ln\left(\frac{1}{3}\right) = C41​ln(31​)=C, so C=−ln⁡(3)4C = -\frac{\ln(3)}{4}C=−4ln(3)​. The solution becomes: 14ln⁡(P4−P)=t−ln⁡(3)4\frac{1}{4}\ln\left(\frac{P}{4-P}\right) = t - \frac{\ln(3)}{4}41​ln(4−PP​)=t−4ln(3)​ When P(t)=2P(t) = 2P(t)=2: 14ln⁡(22)=14ln⁡(1)=0=t−ln⁡(3)4\frac{1}{4}\ln\left(\frac{2}{2}\right) = \frac{1}{4}\ln(1) = 0 = t - \frac{\ln(3)}{4}41​ln(22​)=41​ln(1)=0=t−4ln(3)​ Therefore, t=ln⁡(3)4t = \frac{\ln(3)}{4}t=4ln(3)​, which is answer C. Answer A gives the negative value (incorrect sign). Answer B omits the factor of 14\frac{1}{4}41​. Answer D results from incorrectly calculating ln⁡(32)\ln(3^2)ln(32) instead of the proper partial fraction integration. Remember: logistic equations always require partial fractions for integration, and careful attention to initial conditions determines the integration constant.

Question 13

Consider the equation dydx=2x3y2+1\frac{dy}{dx} = \frac{2x}{3y^2 + 1}dxdy​=3y2+12x​ with initial condition y(0)=1y(0) = 1y(0)=1. After applying the initial condition, the coefficient of x2x^2x2 in the implicit solution is:

  1. 12\frac{1}{2}21​
  2. 111 (correct answer)
  3. 32\frac{3}{2}23​
  4. 222

Explanation: Separating variables: (3y2+1)dy=2xdx(3y^2 + 1)dy = 2x dx(3y2+1)dy=2xdx. Integrating both sides: ∫(3y2+1)dy=∫2xdx\int (3y^2 + 1)dy = \int 2x dx∫(3y2+1)dy=∫2xdx gives y3+y=x2+Cy^3 + y = x^2 + Cy3+y=x2+C. Using initial condition y(0)=1y(0) = 1y(0)=1: 13+1=02+C1^3 + 1 = 0^2 + C13+1=02+C, so C=2C = 2C=2. The solution is y3+y=x2+2y^3 + y = x^2 + 2y3+y=x2+2. The coefficient of x2x^2x2 is 111. Choice A would result from incorrectly integrating 2x2x2x as x2x^2x2 instead of x2x^2x2. Choice C might come from confusion with the coefficient 3 in the original equation. Choice D would result from incorrectly keeping the factor of 2 from the integration of 2x2x2x.

Question 14

Consider the separable differential equation dydx=2xyx2+1\frac{dy}{dx} = \frac{2xy}{x^2 + 1}dxdy​=x2+12xy​ with initial condition y(2)=4y(2) = 4y(2)=4. If the solution is written in the form y=f(x)y = f(x)y=f(x), what is the value of y(0)y(0)y(0)?

  1. 45\frac{4}{5}54​ (correct answer)
  2. 165\frac{16}{5}516​
  3. 444
  4. 204=5\frac{20}{4} = 5420​=5

Explanation: Separating variables: dyy=2xx2+1dx\frac{dy}{y} = \frac{2x}{x^2 + 1}dxydy​=x2+12x​dx. Integrating: ln⁡∣y∣=ln⁡(x2+1)+C\ln|y| = \ln(x^2 + 1) + Cln∣y∣=ln(x2+1)+C, so y=K(x2+1)y = K(x^2 + 1)y=K(x2+1) where K=eCK = e^CK=eC. Using y(2)=4y(2) = 4y(2)=4: 4=K(4+1)=5K4 = K(4 + 1) = 5K4=K(4+1)=5K, so K=45K = \frac{4}{5}K=54​. Therefore y=45(x2+1)y = \frac{4}{5}(x^2 + 1)y=54​(x2+1). At x=0x = 0x=0: y(0)=45(0+1)=45y(0) = \frac{4}{5}(0 + 1) = \frac{4}{5}y(0)=54​(0+1)=54​. Choice B incorrectly uses K=45K = \frac{4}{5}K=54​ but calculates y(0)=45⋅4=165y(0) = \frac{4}{5} \cdot 4 = \frac{16}{5}y(0)=54​⋅4=516​. Choice C assumes the solution is constant. Choice D makes an arithmetic error in finding K.

Question 15

The separable equation dydx=yln⁡yx\frac{dy}{dx} = \frac{y \ln y}{x}dxdy​=xylny​ has initial condition y(1)=ey(1) = ey(1)=e. Which of the following best describes a potential issue when solving this initial value problem?

  1. The equation is undefined when x=0x = 0x=0, creating a vertical asymptote in the solution
  2. The separation process fails because ln⁡y\ln ylny is undefined when y≤0y \leq 0y≤0, restricting the domain (correct answer)
  3. The initial condition y(1)=ey(1) = ey(1)=e leads to ln⁡y=1\ln y = 1lny=1, causing integration difficulties
  4. Multiple solutions exist due to the nonlinear nature of the logarithmic function in the equation

Explanation: When separating variables, we get dyyln⁡y=dxx\frac{dy}{y \ln y} = \frac{dx}{x}ylnydy​=xdx​. The left side requires y>0y > 0y>0 and y≠1y \neq 1y=1 (since ln⁡1=0\ln 1 = 0ln1=0). The function ln⁡y\ln ylny is only defined for y>0y > 0y>0, and the denominator yln⁡y=0y \ln y = 0ylny=0 when y=1y = 1y=1. This creates a restriction on the domain of the solution that must be carefully considered. Choice A incorrectly focuses only on x=0x = 0x=0. Choice C misunderstands that ln⁡e=1\ln e = 1lne=1 is actually convenient for calculations. Choice D incorrectly suggests multiple solutions when the initial value problem has a unique solution in appropriate domains.

Question 16

The differential equation dydx=ycos⁡xsin⁡x+2\frac{dy}{dx} = \frac{y\cos x}{\sin x + 2}dxdy​=sinx+2ycosx​ satisfies y(π)=e2y(\pi) = e^2y(π)=e2. What constraint must be placed on the domain of the solution to ensure continuity?

  1. x≠0x \neq 0x=0 and x≠πx \neq \pix=π for all integer multiples
  2. sin⁡x+2>0\sin x + 2 > 0sinx+2>0, which is satisfied for all real xxx
  3. x≠π2+nπx \neq \frac{\pi}{2} + n\pix=2π​+nπ for integer nnn, where cos⁡x=0\cos x = 0cosx=0
  4. sin⁡x≠−2\sin x \neq -2sinx=−2, but since −1≤sin⁡x≤1-1 \leq \sin x \leq 1−1≤sinx≤1, no restriction needed (correct answer)

Explanation: Separating variables: dyy=cos⁡xsin⁡x+2dx\frac{dy}{y} = \frac{\cos x}{\sin x + 2}dxydy​=sinx+2cosx​dx. The denominator sin⁡x+2\sin x + 2sinx+2 in the original equation could potentially cause issues if it equals zero. However, since −1≤sin⁡x≤1-1 \leq \sin x \leq 1−1≤sinx≤1 for all real xxx, we have 1≤sin⁡x+2≤31 \leq \sin x + 2 \leq 31≤sinx+2≤3, so sin⁡x+2>0\sin x + 2 > 0sinx+2>0 always. Therefore, no domain restrictions are needed for continuity. Choice A incorrectly identifies zeros of sine and cosine. Choice B correctly notes sin⁡x+2>0\sin x + 2 > 0sinx+2>0 but incorrectly presents this as a constraint rather than noting it's automatically satisfied. Choice C incorrectly focuses on where cosine equals zero.

Question 17

A differential equation dydx=f(x)g(y)\frac{dy}{dx} = f(x)g(y)dxdy​=f(x)g(y) satisfies the initial condition y(x0)=y0y(x_0) = y_0y(x0​)=y0​. If G(y)=∫1g(y)dyG(y) = \int \frac{1}{g(y)} dyG(y)=∫g(y)1​dy and F(x)=∫f(x)dxF(x) = \int f(x) dxF(x)=∫f(x)dx, then the particular solution can be written as:

  1. G(y)=F(x)+G(y0)−F(x0)G(y) = F(x) + G(y_0) - F(x_0)G(y)=F(x)+G(y0​)−F(x0​)
  2. G(y)−G(y0)=F(x)−F(x0)G(y) - G(y_0) = F(x) - F(x_0)G(y)−G(y0​)=F(x)−F(x0​) (correct answer)
  3. G(y)+F(x)=G(y0)+F(x0)G(y) + F(x) = G(y_0) + F(x_0)G(y)+F(x)=G(y0​)+F(x0​)
  4. G(y)=F(x)−G(y0)+F(x0)G(y) = F(x) - G(y_0) + F(x_0)G(y)=F(x)−G(y0​)+F(x0​)

Explanation: For the separable equation dydx=f(x)g(y)\frac{dy}{dx} = f(x)g(y)dxdy​=f(x)g(y), we separate to get dyg(y)=f(x)dx\frac{dy}{g(y)} = f(x)dxg(y)dy​=f(x)dx. Integrating both sides from the initial condition: ∫y0y1g(t)dt=∫x0xf(s)ds\int_{y_0}^y \frac{1}{g(t)} dt = \int_{x_0}^x f(s) ds∫y0​y​g(t)1​dt=∫x0​x​f(s)ds. This gives us G(y)−G(y0)=F(x)−F(x0)G(y) - G(y_0) = F(x) - F(x_0)G(y)−G(y0​)=F(x)−F(x0​), where the definite integrals are expressed as differences of antiderivatives. Choice A incorrectly adds G(y0)G(y_0)G(y0​) instead of subtracting. Choice C incorrectly suggests the sum is constant. Choice D has incorrect signs for the terms involving the initial conditions.