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Differential Equations Quiz

Differential Equations Quiz: Integrating Factor Method

Practice Integrating Factor Method 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 / 15

0 of 15 answered

The differential equation (x2+1)y′+2xy=cos⁡(x)(x^2 + 1)y' + 2xy = \cos(x)(x2+1)y′+2xy=cos(x) is a first-order linear equation. What is its general solution for y(x)y(x)y(x)?

Select an answer to continue

What this quiz covers

This quiz focuses on Integrating Factor Method, 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

The differential equation (x2+1)y′+2xy=cos⁡(x)(x^2 + 1)y' + 2xy = \cos(x)(x2+1)y′+2xy=cos(x) is a first-order linear equation. What is its general solution for y(x)y(x)y(x)?

  1. y=−sin⁡(x)+Cx2+1y = \frac{-\sin(x) + C}{x^2 + 1}y=x2+1−sin(x)+C​
  2. y=sin⁡(x)x2+1+Cy = \frac{\sin(x)}{x^2 + 1} + Cy=x2+1sin(x)​+C
  3. y=sin⁡(x)+Cx2+1y = \sin(x) + \frac{C}{x^2+1}y=sin(x)+x2+1C​
  4. y=sin⁡(x)+Cx2+1y = \frac{\sin(x) + C}{x^2 + 1}y=x2+1sin(x)+C​ (correct answer)

Explanation: First, put the equation in standard form y′+P(x)y=Q(x)y' + P(x)y = Q(x)y′+P(x)y=Q(x) by dividing by (x2+1)(x^2 + 1)(x2+1): y′+2xx2+1y=cos⁡(x)x2+1y' + \frac{2x}{x^2+1}y = \frac{\cos(x)}{x^2+1}y′+x2+12x​y=x2+1cos(x)​. The integrating factor is μ(x)=e∫2xx2+1dx=eln⁡(x2+1)=x2+1\mu(x) = e^{\int \frac{2x}{x^2+1} dx} = e^{\ln(x^2+1)} = x^2+1μ(x)=e∫x2+12x​dx=eln(x2+1)=x2+1. Multiplying the standard form equation by μ(x)\mu(x)μ(x) gives d/dx((x2+1)y)=cos⁡(x)d/dx((x^2+1)y) = \cos(x)d/dx((x2+1)y)=cos(x). Integrating both sides yields (x2+1)y=∫cos⁡(x)dx=sin⁡(x)+C(x^2+1)y = \int \cos(x) dx = \sin(x) + C(x2+1)y=∫cos(x)dx=sin(x)+C. Finally, solving for yyy gives y=sin⁡(x)+Cx2+1y = \frac{\sin(x) + C}{x^2 + 1}y=x2+1sin(x)+C​.

Question 2

Consider the initial value problem y′−y=xexy' - y = xe^xy′−y=xex with the initial condition y(0)=2y(0) = 2y(0)=2. What is the value of y(2)y(2)y(2)?

  1. 2e22e^22e2
  2. 6e26e^26e2
  3. 34e2+94e−2\frac{3}{4}e^2 + \frac{9}{4}e^{-2}43​e2+49​e−2
  4. 4e24e^24e2 (correct answer)

Explanation: The equation is in standard form with P(x)=−1P(x) = -1P(x)=−1 and Q(x)=xexQ(x) = xe^xQ(x)=xex. The integrating factor is μ(x)=e∫−1dx=e−x\mu(x) = e^{\int -1 dx} = e^{-x}μ(x)=e∫−1dx=e−x. Multiplying the equation by μ(x)\mu(x)μ(x) gives d/dx(e−xy)=e−x(xex)=xd/dx(e^{-x}y) = e^{-x}(xe^x) = xd/dx(e−xy)=e−x(xex)=x. Integrating both sides, we get e−xy=∫xdx=x22+Ce^{-x}y = \int x dx = \frac{x^2}{2} + Ce−xy=∫xdx=2x2​+C. The general solution is y(x)=(x22+C)exy(x) = (\frac{x^2}{2} + C)e^xy(x)=(2x2​+C)ex. Using the initial condition y(0)=2y(0)=2y(0)=2, we find 2=(0+C)e02 = (0 + C)e^02=(0+C)e0, so C=2C=2C=2. The particular solution is y(x)=(x22+2)exy(x) = (\frac{x^2}{2} + 2)e^xy(x)=(2x2​+2)ex. Evaluating at x=2x=2x=2 gives y(2)=(222+2)e2=(2+2)e2=4e2y(2) = (\frac{2^2}{2} + 2)e^2 = (2+2)e^2 = 4e^2y(2)=(222​+2)e2=(2+2)e2=4e2.

Question 3

To solve y′+P(x)y=Q(x)y' + P(x)y = Q(x)y′+P(x)y=Q(x), the integrating factor is typically chosen as μ(x)=e∫P(x)dx\mu(x) = e^{\int P(x)dx}μ(x)=e∫P(x)dx. Suppose instead, an integrating factor μ∗(x)=A⋅e∫P(x)dx\mu^*(x) = A \cdot e^{\int P(x)dx}μ∗(x)=A⋅e∫P(x)dx is used, where AAA is a positive constant other than 1. How does the resulting family of solutions y∗(x)y^*(x)y∗(x) relate to the family of solutions y(x)y(x)y(x) obtained using μ(x)\mu(x)μ(x)?

  1. The family of solutions y∗(x)y^*(x)y∗(x) is identical to the family of solutions y(x)y(x)y(x). (correct answer)
  2. y∗(x)y^*(x)y∗(x) is a vertical translation of y(x)y(x)y(x), i.e., y∗(x)=y(x)+Ay^*(x) = y(x) + Ay∗(x)=y(x)+A.
  3. y∗(x)y^*(x)y∗(x) is a scaling of y(x)y(x)y(x), i.e., y∗(x)=A⋅y(x)y^*(x) = A \cdot y(x)y∗(x)=A⋅y(x).
  4. The method fails because the left-hand side is no longer an exact derivative.

Explanation: Using μ∗(x)=Aμ(x)\mu^*(x) = A\mu(x)μ∗(x)=Aμ(x), the differential equation becomes d/dx(μ∗(x)y)=μ∗(x)Q(x)d/dx(\mu^*(x)y) = \mu^*(x)Q(x)d/dx(μ∗(x)y)=μ∗(x)Q(x). Integrating gives μ∗(x)y=∫μ∗(x)Q(x)dx+C∗\mu^*(x)y = \int \mu^*(x)Q(x)dx + C^*μ∗(x)y=∫μ∗(x)Q(x)dx+C∗, where C∗C^*C∗ is an arbitrary constant. Substituting μ∗(x)=Aμ(x)\mu^*(x) = A\mu(x)μ∗(x)=Aμ(x) gives Aμ(x)y=∫Aμ(x)Q(x)dx+C∗=A∫μ(x)Q(x)dx+C∗A\mu(x)y = \int A\mu(x)Q(x)dx + C^* = A\int \mu(x)Q(x)dx + C^*Aμ(x)y=∫Aμ(x)Q(x)dx+C∗=A∫μ(x)Q(x)dx+C∗. Dividing by Aμ(x)A\mu(x)Aμ(x) yields y∗(x)=1μ(x)(∫μ(x)Q(x)dx+C∗A)y^*(x) = \frac{1}{\mu(x)}(\int \mu(x)Q(x)dx + \frac{C^*}{A})y∗(x)=μ(x)1​(∫μ(x)Q(x)dx+AC∗​). Since C∗C^*C∗ is an arbitrary constant, C=C∗/AC = C^*/AC=C∗/A is also an arbitrary constant. Thus, y∗(x)=1μ(x)(∫μ(x)Q(x)dx+C)y^*(x) = \frac{1}{\mu(x)}(\int \mu(x)Q(x)dx + C)y∗(x)=μ(x)1​(∫μ(x)Q(x)dx+C), which represents the exact same family of solutions as y(x)y(x)y(x).

Question 4

Find the general solution for x(y)x(y)x(y) for the differential equation dxdy+1yx=y2\frac{dx}{dy} + \frac{1}{y}x = y^2dydx​+y1​x=y2, assuming y>0y>0y>0.

  1. x(y)=y32+Cyx(y) = \frac{y^3}{2} + Cyx(y)=2y3​+Cy
  2. x(y)=3y+Cyx(y) = 3y + \frac{C}{y}x(y)=3y+yC​
  3. y(x)=x34+Cxy(x) = \frac{x^3}{4} + \frac{C}{x}y(x)=4x3​+xC​
  4. x(y)=y34+Cyx(y) = \frac{y^3}{4} + \frac{C}{y}x(y)=4y3​+yC​ (correct answer)

Explanation: This is a first-order linear differential equation for xxx as a function of yyy. The equation is already in standard form dx/dy+P(y)x=Q(y)dx/dy + P(y)x = Q(y)dx/dy+P(y)x=Q(y), with P(y)=1/yP(y) = 1/yP(y)=1/y and Q(y)=y2Q(y) = y^2Q(y)=y2. The integrating factor is μ(y)=e∫(1/y)dy=eln⁡y=y\mu(y) = e^{\int (1/y) dy} = e^{\ln y} = yμ(y)=e∫(1/y)dy=elny=y. Multiplying the equation by μ(y)\mu(y)μ(y) gives d/dy(y⋅x)=y⋅y2=y3d/dy(y \cdot x) = y \cdot y^2 = y^3d/dy(y⋅x)=y⋅y2=y3. Integrating both sides with respect to yyy gives yx=∫y3dy=y44+Cyx = \int y^3 dy = \frac{y^4}{4} + Cyx=∫y3dy=4y4​+C. Solving for xxx yields x(y)=y34+Cyx(y) = \frac{y^3}{4} + \frac{C}{y}x(y)=4y3​+yC​.

Question 5

A student attempts to solve the initial value problem xy′+y=4x3xy' + y = 4x^3xy′+y=4x3 with y(1)=5y(1)=5y(1)=5. Their work is shown below: Step 1: Rearrange to y′+(1/x)y=4x2y' + (1/x)y = 4x^2y′+(1/x)y=4x2. Step 2: The integrating factor is μ(x)=e∫(1/x)dx=eln⁡x=x\mu(x) = e^{\int(1/x)dx} = e^{\ln x} = xμ(x)=e∫(1/x)dx=elnx=x. Step 3: Multiply by μ(x)\mu(x)μ(x): x(y′+(1/x)y)=x(4x2)x(y' + (1/x)y) = x(4x^2)x(y′+(1/x)y)=x(4x2), which simplifies to d/dx(xy)=4x3d/dx(xy) = 4x^3d/dx(xy)=4x3. Step 4: Integrate both sides: xy=∫4x3dx=x4xy = \int 4x^3 dx = x^4xy=∫4x3dx=x4. Step 5: Solve for yyy: y=x3y = x^3y=x3. Step 6: Apply initial condition: y(1)=13=1y(1) = 1^3 = 1y(1)=13=1. Since this does not match y(1)=5y(1)=5y(1)=5, the student concludes there is no solution. In which step did the first error occur?

  1. Step 1
  2. Step 3
  3. Step 4 (correct answer)
  4. Step 6

Explanation: When solving first-order linear differential equations using integrating factors, you must carefully track each algebraic step, especially during integration where constants of integration are crucial. Let's trace through the student's work to find where things went wrong. Steps 1-3 are executed correctly: the equation is properly rearranged into standard form y′+1xy=4x2y' + \frac{1}{x}y = 4x^2y′+x1​y=4x2, the integrating factor μ(x)=x\mu(x) = xμ(x)=x is computed correctly, and multiplying through gives ddx(xy)=4x3\frac{d}{dx}(xy) = 4x^3dxd​(xy)=4x3. The error occurs in Step 4 during integration. When integrating 4x34x^34x3, the student gets x4x^4x4, but this is missing the constant of integration. The correct integration should yield xy=∫4x3dx=x4+Cxy = \int 4x^3 dx = x^4 + Cxy=∫4x3dx=x4+C, giving y=x3+Cxy = x^3 + \frac{C}{x}y=x3+xC​. Applying the initial condition y(1)=5y(1) = 5y(1)=5 allows us to solve for CCC: 5=1+C5 = 1 + C5=1+C, so C=4C = 4C=4. The complete solution is y=x3+4xy = x^3 + \frac{4}{x}y=x3+x4​. Choice A is wrong because Step 1 correctly rearranges to standard form. Choice B is wrong because Step 3 properly applies the integrating factor. Choice D is wrong because Step 6 correctly applies the initial condition to the (incomplete) solution from Step 5. Study tip: Always include the constant of integration when solving differential equations, even if it seems obvious. The initial conditions exist specifically to determine this constant, and forgetting it will lead to incorrect solutions that don't satisfy the given conditions.

Question 6

What is the general solution to the differential equation y′+ycot⁡(x)=2cos⁡(x)y' + y \cot(x) = 2 \cos(x)y′+ycot(x)=2cos(x) for 0<x<π0 < x < \pi0<x<π?

  1. y=2sin⁡(x)ln⁡∣sin⁡x∣+Csin⁡(x)y = 2\sin(x)\ln|\sin x| + C\sin(x)y=2sin(x)ln∣sinx∣+Csin(x)
  2. y=sin⁡(x)+Ccsc⁡(x)y = \sin(x) + C\csc(x)y=sin(x)+Ccsc(x) (correct answer)
  3. y=12cos⁡(2x)+Csin⁡(x)y = \frac{\frac{1}{2}\cos(2x) + C}{\sin(x)}y=sin(x)21​cos(2x)+C​
  4. y=(x+12sin⁡(2x)+C)sec⁡(x)y = (x + \frac{1}{2}\sin(2x) + C)\sec(x)y=(x+21​sin(2x)+C)sec(x)

Explanation: When you encounter a first-order linear differential equation like this one, recognize the standard form y′+P(x)y=Q(x)y' + P(x)y = Q(x)y′+P(x)y=Q(x) where P(x)=cot⁡(x)P(x) = \cot(x)P(x)=cot(x) and Q(x)=2cos⁡(x)Q(x) = 2\cos(x)Q(x)=2cos(x). The solution method requires finding an integrating factor μ(x)=e∫P(x)dx\mu(x) = e^{\int P(x)dx}μ(x)=e∫P(x)dx. First, calculate the integrating factor: μ(x)=e∫cot⁡(x)dx=eln⁡∣sin⁡(x)∣=sin⁡(x)\mu(x) = e^{\int \cot(x)dx} = e^{\ln|\sin(x)|} = \sin(x)μ(x)=e∫cot(x)dx=eln∣sin(x)∣=sin(x) (for 0<x<π0 < x < \pi0<x<π where sin⁡(x)>0\sin(x) > 0sin(x)>0). Multiply the entire equation by sin⁡(x)\sin(x)sin(x): sin⁡(x)y′+sin⁡(x)ycot⁡(x)=2sin⁡(x)cos⁡(x)\sin(x)y' + \sin(x)y\cot(x) = 2\sin(x)\cos(x)sin(x)y′+sin(x)ycot(x)=2sin(x)cos(x) This simplifies to: sin⁡(x)y′+ycos⁡(x)=sin⁡(2x)\sin(x)y' + y\cos(x) = \sin(2x)sin(x)y′+ycos(x)=sin(2x) The left side is the derivative of sin⁡(x)y\sin(x)ysin(x)y, so: ddx[sin⁡(x)y]=sin⁡(2x)\frac{d}{dx}[\sin(x)y] = \sin(2x)dxd​[sin(x)y]=sin(2x) Integrating both sides: sin⁡(x)y=∫sin⁡(2x)dx=−12cos⁡(2x)+C\sin(x)y = \int \sin(2x)dx = -\frac{1}{2}\cos(2x) + Csin(x)y=∫sin(2x)dx=−21​cos(2x)+C Therefore: y=−12cos⁡(2x)+Csin⁡(x)=−12cos⁡(2x)csc⁡(x)+Ccsc⁡(x)y = \frac{-\frac{1}{2}\cos(2x) + C}{\sin(x)} = -\frac{1}{2}\cos(2x)\csc(x) + C\csc(x)y=sin(x)−21​cos(2x)+C​=−21​cos(2x)csc(x)+Ccsc(x) Using the identity cos⁡(2x)=1−2sin⁡2(x)\cos(2x) = 1 - 2\sin^2(x)cos(2x)=1−2sin2(x), this becomes y=sin⁡(x)+Ccsc⁡(x)y = \sin(x) + C\csc(x)y=sin(x)+Ccsc(x), which is answer B. Answer A incorrectly involves a logarithmic term not present in this solution. Answer C has the wrong sign and coefficient for the cosine term. Answer D incorrectly uses secant instead of cosecant and includes terms that don't arise from this differential equation. Strategy tip: For first-order linear equations, always identify P(x)P(x)P(x) correctly and remember that ∫cot⁡(x)dx=ln⁡∣sin⁡(x)∣\int \cot(x)dx = \ln|\sin(x)|∫cot(x)dx=ln∣sin(x)∣, making μ(x)=sin⁡(x)\mu(x) = \sin(x)μ(x)=sin(x).

Question 7

A mixing tank initially contains 100 L of pure water. A salt solution with a concentration of 0.2 kg/L enters the tank at a rate of 5 L/min. The well-mixed solution is drained from the tank at the same rate. Let A(t)A(t)A(t) be the amount of salt (in kg) in the tank at time ttt (in minutes). What is the limiting amount of salt in the tank as t→∞t \to \inftyt→∞?

  1. 0 kg
  2. 100 kg
  3. The amount of salt increases without bound.
  4. 20 kg (correct answer)

Explanation: The rate of change of salt is dA/dt=rate in−rate outdA/dt = \text{rate in} - \text{rate out}dA/dt=rate in−rate out. The rate in is (0.2 kg/L)×(5 L/min)=1 kg/min(0.2 \text{ kg/L}) \times (5 \text{ L/min}) = 1 \text{ kg/min}(0.2 kg/L)×(5 L/min)=1 kg/min. The concentration in the tank is A(t)/100A(t)/100A(t)/100 kg/L, so the rate out is (A(t)/100 kg/L)×(5 L/min)=A(t)/20 kg/min(A(t)/100 \text{ kg/L}) \times (5 \text{ L/min}) = A(t)/20 \text{ kg/min}(A(t)/100 kg/L)×(5 L/min)=A(t)/20 kg/min. The DE is dA/dt=1−A/20dA/dt = 1 - A/20dA/dt=1−A/20, or A′+(1/20)A=1A' + (1/20)A = 1A′+(1/20)A=1. This is a linear equation. The integrating factor is μ(t)=e∫(1/20)dt=et/20\mu(t) = e^{\int(1/20)dt} = e^{t/20}μ(t)=e∫(1/20)dt=et/20. The solution is A(t)=20+Ce−t/20A(t) = 20 + Ce^{-t/20}A(t)=20+Ce−t/20. With A(0)=0A(0)=0A(0)=0, we find C=−20C=-20C=−20. So, A(t)=20−20e−t/20A(t) = 20 - 20e^{-t/20}A(t)=20−20e−t/20. As t→∞t \to \inftyt→∞, the term e−t/20→0e^{-t/20} \to 0e−t/20→0, so lim⁡t→∞A(t)=20\lim_{t\to\infty} A(t) = 20limt→∞​A(t)=20. Alternatively, at equilibrium, dA/dt=0dA/dt=0dA/dt=0, so 1−A/20=01 - A/20 = 01−A/20=0, which gives A=20A=20A=20.

Question 8

For what value of the constant kkk does the solution to the initial value problem y′+2y=ekty' + 2y = e^{kt}y′+2y=ekt with y(0)=3y(0)=3y(0)=3 have a finite, non-zero limit as x→∞x \to \inftyx→∞?

  1. k=−2k = -2k=−2
  2. k=2k = 2k=2
  3. k=0k = 0k=0 (correct answer)
  4. No such value of kkk exists.

Explanation: When analyzing the long-term behavior of solutions to first-order linear differential equations, you need to consider how each term in the solution behaves as the independent variable approaches infinity. To solve y′+2y=ekty' + 2y = e^{kt}y′+2y=ekt, you'll use an integrating factor. The integrating factor is μ(t)=e2t\mu(t) = e^{2t}μ(t)=e2t. Multiplying through and integrating gives you the general solution: y=Ce−2t+ektk+2y = Ce^{-2t} + \frac{e^{kt}}{k+2}y=Ce−2t+k+2ekt​ (when k≠−2k \neq -2k=−2). Applying the initial condition y(0)=3y(0) = 3y(0)=3: 3=C+1k+23 = C + \frac{1}{k+2}3=C+k+21​, so C=3−1k+2C = 3 - \frac{1}{k+2}C=3−k+21​. For the solution to have a finite, non-zero limit as t→∞t \to \inftyt→∞, the exponential terms must behave appropriately. The term Ce−2tCe^{-2t}Ce−2t always approaches zero since the exponent is negative. The term ektk+2\frac{e^{kt}}{k+2}k+2ekt​ determines the limit behavior. When k=0k = 0k=0, this term becomes 12\frac{1}{2}21​, which is constant. Therefore, lim⁡t→∞y(t)=0+12=12\lim_{t \to \infty} y(t) = 0 + \frac{1}{2} = \frac{1}{2}limt→∞​y(t)=0+21​=21​, giving us a finite, non-zero limit. This makes (C) correct. (A) k=−2k = -2k=−2 creates division by zero in our solution formula, requiring special handling and ultimately leading to unbounded growth. (B) k=2k = 2k=2 makes e2te^{2t}e2t grow exponentially, so the limit is infinite. (D) is incorrect since we found that k=0k = 0k=0 works. Study tip: For linear differential equations with exponential forcing functions, the key to finite limits is matching the forcing function's growth rate to the natural decay rate of the homogeneous solution.

Question 9

Consider the differential equation t2dydt+3ty=ln⁡(t)t^2\frac{dy}{dt} + 3ty = \ln(t)t2dtdy​+3ty=ln(t). If the integrating factor method is applied, the equation can be written in the form ddt(μ(t)y)=F(t)\frac{d}{dt}(\mu(t)y) = F(t)dtd​(μ(t)y)=F(t). What is the function F(t)F(t)F(t)?

  1. tln⁡(t)t \ln(t)tln(t) (correct answer)
  2. t3ln⁡(t)t^3 \ln(t)t3ln(t)
  3. ln⁡(t)t2\frac{\ln(t)}{t^2}t2ln(t)​
  4. ln⁡(t)\ln(t)ln(t)

Explanation: When you encounter a first-order linear differential equation, the integrating factor method transforms it into a form where the left side becomes the derivative of a product. This question tests whether you can correctly identify what appears on the right side after this transformation. Starting with t2dydt+3ty=ln⁡(t)t^2\frac{dy}{dt} + 3ty = \ln(t)t2dtdy​+3ty=ln(t), first divide by t2t^2t2 to get standard form: dydt+3ty=ln⁡(t)t2\frac{dy}{dt} + \frac{3}{t}y = \frac{\ln(t)}{t^2}dtdy​+t3​y=t2ln(t)​ The integrating factor is μ(t)=e∫3tdt=e3ln⁡(t)=t3\mu(t) = e^{\int \frac{3}{t}dt} = e^{3\ln(t)} = t^3μ(t)=e∫t3​dt=e3ln(t)=t3 Multiplying the standard form by t3t^3t3: t3dydt+3t2y=t3⋅ln⁡(t)t2=tln⁡(t)t^3\frac{dy}{dt} + 3t^2y = t^3 \cdot \frac{\ln(t)}{t^2} = t\ln(t)t3dtdy​+3t2y=t3⋅t2ln(t)​=tln(t) The left side is indeed ddt(t3y)\frac{d}{dt}(t^3y)dtd​(t3y), so F(t)=tln⁡(t)F(t) = t\ln(t)F(t)=tln(t). Choice A is correct: tln⁡(t)t\ln(t)tln(t) is exactly what we get when multiplying the original right side by the integrating factor. Choice B (t3ln⁡(t)t^3\ln(t)t3ln(t)) represents a common error where students forget to divide by t2t^2t2 before applying the integrating factor, essentially multiplying ln⁡(t)\ln(t)ln(t) directly by t3t^3t3. Choice C (ln⁡(t)t2\frac{\ln(t)}{t^2}t2ln(t)​) is the right side of the equation in standard form before multiplying by the integrating factor. Choice D (ln⁡(t)\ln(t)ln(t)) is simply the original right side, showing no transformation was applied. Study tip: Always convert to standard form first, then find the integrating factor. The function F(t)F(t)F(t) equals the integrating factor times the right side of the standard form equation.

Question 10

Let y(x)y(x)y(x) be the solution to the initial value problem y′+2xy=x2y' + \frac{2}{x}y = x^2y′+x2​y=x2 with the initial condition y(1)=1y(1)=1y(1)=1. What is the value of y(2)y(2)y(2)?

  1. 8/58/58/5
  2. 9/59/59/5 (correct answer)
  3. 888
  4. 12/512/512/5

Explanation: When you encounter a first-order linear differential equation like y′+2xy=x2y' + \frac{2}{x}y = x^2y′+x2​y=x2, recognize this as the standard form y′+P(x)y=Q(x)y' + P(x)y = Q(x)y′+P(x)y=Q(x) where P(x)=2xP(x) = \frac{2}{x}P(x)=x2​ and Q(x)=x2Q(x) = x^2Q(x)=x2. The solution method requires finding an integrating factor. The integrating factor is μ(x)=e∫P(x)dx=e∫2xdx=e2ln⁡∣x∣=x2\mu(x) = e^{\int P(x)dx} = e^{\int \frac{2}{x}dx} = e^{2\ln|x|} = x^2μ(x)=e∫P(x)dx=e∫x2​dx=e2ln∣x∣=x2. Multiplying the entire equation by x2x^2x2 gives: x2y′+2xy=x4x^2y' + 2xy = x^4x2y′+2xy=x4. The left side is the derivative of x2yx^2yx2y, so we have ddx(x2y)=x4\frac{d}{dx}(x^2y) = x^4dxd​(x2y)=x4. Integrating both sides: x2y=∫x4dx=x55+Cx^2y = \int x^4 dx = \frac{x^5}{5} + Cx2y=∫x4dx=5x5​+C, which gives us y=x35+Cx2y = \frac{x^3}{5} + \frac{C}{x^2}y=5x3​+x2C​. Using the initial condition y(1)=1y(1) = 1y(1)=1: 1=15+C1 = \frac{1}{5} + C1=51​+C, so C=45C = \frac{4}{5}C=54​. Therefore, y(x)=x35+45x2y(x) = \frac{x^3}{5} + \frac{4}{5x^2}y(x)=5x3​+5x24​. At x=2x = 2x=2: y(2)=85+45⋅4=85+15=95y(2) = \frac{8}{5} + \frac{4}{5 \cdot 4} = \frac{8}{5} + \frac{1}{5} = \frac{9}{5}y(2)=58​+5⋅44​=58​+51​=59​, confirming answer B. Answer A (8/58/58/5) would result from forgetting the constant term. Answer C (888) likely comes from computational errors or misapplying the integrating factor. Answer D (12/512/512/5) might arise from incorrectly computing the constant or making integration mistakes. Remember: first-order linear equations always follow this integrating factor pattern. Practice identifying P(x)P(x)P(x) and computing e∫P(x)dxe^{\int P(x)dx}e∫P(x)dx accurately—it's the foundation of the entire solution process.

Question 11

The differential equation dydx−yx=exx2\frac{dy}{dx} - \frac{y}{x} = \frac{e^x}{x^2}dxdy​−xy​=x2ex​ has solution y=ex+Cxy = \frac{e^x + C}{x}y=xex+C​ for x>0x > 0x>0. If we extend this solution to x<0x < 0x<0, which statement about the general solution is correct?

  1. The solution remains y=ex+Cxy = \frac{e^x + C}{x}y=xex+C​ with the same constant CCC for all x≠0x \neq 0x=0
  2. The solution requires modification to y=ex+C∣x∣y = \frac{e^x + C}{|x|}y=∣x∣ex+C​ for x<0x < 0x<0
  3. The solution is undefined for x<0x < 0x<0 due to the integrating factor
  4. The solution becomes y=ex+C1xy = \frac{e^x + C_1}{x}y=xex+C1​​ for x>0x > 0x>0 and y=ex+C2xy = \frac{e^x + C_2}{x}y=xex+C2​​ for x<0x < 0x<0 (correct answer)

Explanation: When solving linear first-order differential equations across domains that include singular points (like x=0x = 0x=0 here), you need to consider each connected domain separately. The point x=0x = 0x=0 creates a discontinuity that prevents solutions from being extended across it. To understand why, let's examine the integrating factor method. For this equation dydx−yx=exx2\frac{dy}{dx} - \frac{y}{x} = \frac{e^x}{x^2}dxdy​−xy​=x2ex​, the integrating factor is μ(x)=e−∫1xdx=e−ln⁡∣x∣=1∣x∣\mu(x) = e^{-\int \frac{1}{x}dx} = e^{-\ln|x|} = \frac{1}{|x|}μ(x)=e−∫x1​dx=e−ln∣x∣=∣x∣1​. When you multiply through and integrate, you get different constants of integration for x>0x > 0x>0 and x<0x < 0x<0 because these are separate integration processes over disconnected intervals. The correct answer is (D) because the general solution must allow for different constants C1C_1C1​ and C2C_2C2​ on each side of the singular point. Each domain (x>0(x > 0(x>0 and x<0)x < 0)x<0) represents a separate initial value problem with its own arbitrary constant. (A) is wrong because it assumes continuity across x=0x = 0x=0, which isn't possible given the singular behavior of the coefficients. (B) incorrectly modifies the solution form rather than recognizing the need for separate constants. (C) is incorrect because the integrating factor 1∣x∣\frac{1}{|x|}∣x∣1​ works perfectly well for x<0x < 0x<0; the issue isn't undefined behavior but rather separate domains. Study tip: When differential equations have singular points, always solve on each connected domain separately. The constants of integration are independent across these domains.

Question 12

A tank contains 100 gallons of brine with 10 pounds of salt. Pure water flows in at 5 gal/min and the mixture flows out at the same rate. The differential equation dSdt+S20=0\frac{dS}{dt} + \frac{S}{20} = 0dtdS​+20S​=0 models the salt content S(t)S(t)S(t). If someone claims the integrating factor approach gives S(t)=10e−t/20S(t) = 10e^{-t/20}S(t)=10e−t/20, what verification step would confirm this is correct?

  1. Substitute into the original equation and verify both sides are equal (correct answer)
  2. Check that S(0)=10S(0) = 10S(0)=10 and lim⁡t→∞S(t)=0\lim_{t \to \infty} S(t) = 0limt→∞​S(t)=0
  3. Verify that the integrating factor et/20e^{t/20}et/20 was computed correctly
  4. Check that the rate of salt decrease matches the outflow concentration

Explanation: When you're given a proposed solution to a differential equation, the most reliable way to verify its correctness is to substitute it back into the original equation and check that both sides are equal. This is the fundamental verification method in differential equations. Let's see why option A is correct. If S(t)=10e−t/20S(t) = 10e^{-t/20}S(t)=10e−t/20, then dSdt=10⋅(−120)e−t/20=−12e−t/20\frac{dS}{dt} = 10 \cdot (-\frac{1}{20})e^{-t/20} = -\frac{1}{2}e^{-t/20}dtdS​=10⋅(−201​)e−t/20=−21​e−t/20. Substituting into the original equation: −12e−t/20+10e−t/2020=−12e−t/20+12e−t/20=0-\frac{1}{2}e^{-t/20} + \frac{10e^{-t/20}}{20} = -\frac{1}{2}e^{-t/20} + \frac{1}{2}e^{-t/20} = 0−21​e−t/20+2010e−t/20​=−21​e−t/20+21​e−t/20=0. Since both sides equal zero, the solution is verified. Option B checks boundary conditions and limiting behavior, which are important for physical reasonableness but don't prove the solution satisfies the differential equation itself. A function could have the right initial value and limit but still not solve the equation. Option C focuses on verifying the integrating factor computation, but even if the integrating factor is correct, errors could occur in subsequent steps. This doesn't verify the final answer. Option D examines physical interpretation, which is valuable for understanding but insufficient for mathematical verification. The solution could make physical sense yet still be mathematically incorrect. Remember: when verifying any proposed solution to a differential equation, always substitute back into the original equation first. This direct substitution is your most powerful and definitive verification tool.

Question 13

For the differential equation dydx+ytan⁡x=sec⁡x\frac{dy}{dx} + y\tan x = \sec xdxdy​+ytanx=secx, which of the following represents the correct integrating factor and the form of the general solution?

  1. Integrating factor: sec⁡x\sec xsecx; Solution: y=x+Ccos⁡xy = x + C\cos xy=x+Ccosx
  2. Integrating factor: cos⁡x\cos xcosx; Solution: y=sin⁡x+Csec⁡xy = \sin x + C\sec xy=sinx+Csecx
  3. Integrating factor: sec⁡x\sec xsecx; Solution: y=sin⁡x+Ccos⁡xy = \sin x + C\cos xy=sinx+Ccosx (correct answer)
  4. Integrating factor: cos⁡x\cos xcosx; Solution: y=x+Csec⁡xy = x + C\sec xy=x+Csecx

Explanation: The integrating factor is μ(x)=e∫tan⁡xdx=eln⁡∣sec⁡x∣=sec⁡x\mu(x) = e^{\int \tan x dx} = e^{\ln|\sec x|} = \sec xμ(x)=e∫tanxdx=eln∣secx∣=secx. Multiplying the equation: sec⁡xdydx+ysec⁡xtan⁡x=sec⁡2x\sec x \frac{dy}{dx} + y\sec x \tan x = \sec^2 xsecxdxdy​+ysecxtanx=sec2x. The left side is ddx[ysec⁡x]\frac{d}{dx}[y\sec x]dxd​[ysecx]. Integrating: ysec⁡x=∫sec⁡2xdx=tan⁡x+Cy\sec x = \int \sec^2 x dx = \tan x + Cysecx=∫sec2xdx=tanx+C. Therefore y=(tan⁡x+C)cos⁡x=sin⁡x+Ccos⁡xy = (\tan x + C)\cos x = \sin x + C\cos xy=(tanx+C)cosx=sinx+Ccosx. Choice A has wrong solution form, Choice B has wrong integrating factor, Choice D has both wrong integrating factor and solution.

Question 14

For the differential equation dydx+ycot⁡x=csc⁡x\frac{dy}{dx} + y\cot x = \csc xdxdy​+ycotx=cscx, a student finds the integrating factor to be sin⁡x\sin xsinx and obtains ysin⁡x=−cos⁡x+Cy\sin x = -\cos x + Cysinx=−cosx+C. However, the final answer y=−cot⁡x+Ccsc⁡xy = -\cot x + C\csc xy=−cotx+Ccscx fails verification. What went wrong?

  1. The integrating factor should be csc⁡x\csc xcscx, not sin⁡x\sin xsinx
  2. The integration of the right-hand side was performed incorrectly (correct answer)
  3. The student forgot to apply the product rule when verifying
  4. The sign error occurred when computing ∫cot⁡xdx\int \cot x dx∫cotxdx

Explanation: The integrating factor μ(x)=e∫cot⁡xdx=eln⁡∣sin⁡x∣=sin⁡x\mu(x) = e^{\int \cot x dx} = e^{\ln|\sin x|} = \sin xμ(x)=e∫cotxdx=eln∣sinx∣=sinx is correct. Multiplying: sin⁡xdydx+ysin⁡xcot⁡x=sin⁡xcsc⁡x=1\sin x \frac{dy}{dx} + y\sin x \cot x = \sin x \csc x = 1sinxdxdy​+ysinxcotx=sinxcscx=1. The left side is ddx[ysin⁡x]\frac{d}{dx}[y\sin x]dxd​[ysinx]. Integrating: ysin⁡x=∫1dx=x+Cy\sin x = \int 1 dx = x + Cysinx=∫1dx=x+C, not −cos⁡x+C-\cos x + C−cosx+C. The student incorrectly integrated the right-hand side. The correct solution is y=x+Csin⁡x=(x+C)csc⁡xy = \frac{x + C}{\sin x} = (x + C)\csc xy=sinxx+C​=(x+C)cscx. Choices A and D are incorrect about the integrating factor and integration respectively, while C is wrong because the issue isn't with verification technique.

Question 15

The equation xdydx+2y=x3sin⁡xx\frac{dy}{dx} + 2y = x^3\sin xxdxdy​+2y=x3sinx can be solved using an integrating factor method after a preliminary step. What is the correct sequence of operations?

  1. Divide by xxx, then use integrating factor e2∫1xdx=x2e^{2\int \frac{1}{x} dx} = x^2e2∫x1​dx=x2
  2. Multiply by xxx, then use integrating factor e∫2xdx=ex2e^{\int 2x dx} = e^{x^2}e∫2xdx=ex2
  3. Divide by xxx, then use integrating factor e∫2xdx=x2e^{\int \frac{2}{x} dx} = x^2e∫x2​dx=x2 (correct answer)
  4. Use substitution u=x2u = x^2u=x2, then apply standard integrating factor eue^ueu

Explanation: First, we need the equation in standard form dydx+P(x)y=Q(x)\frac{dy}{dx} + P(x)y = Q(x)dxdy​+P(x)y=Q(x). Dividing by xxx: dydx+2xy=x2sin⁡x\frac{dy}{dx} + \frac{2}{x}y = x^2\sin xdxdy​+x2​y=x2sinx. Now P(x)=2xP(x) = \frac{2}{x}P(x)=x2​, so the integrating factor is μ(x)=e∫2xdx=e2ln⁡∣x∣=x2\mu(x) = e^{\int \frac{2}{x} dx} = e^{2\ln|x|} = x^2μ(x)=e∫x2​dx=e2ln∣x∣=x2. Choice A has the wrong exponent (should be ∫2xdx\int \frac{2}{x} dx∫x2​dx, not 2∫1xdx2\int \frac{1}{x} dx2∫x1​dx), Choice B incorrectly multiplies by xxx, and Choice D suggests an inappropriate substitution method.