Home

Tutoring

Subjects

Live Classes

Study Coach

Essay Review

On-Demand Courses

Colleges

Games

Opening subject page...

Loading your content

← Back to quizzes

Differential Equations

Differential Equations Quiz: Implicit Vs Explicit Solutions

Practice Implicit Vs Explicit Solutions in Differential Equations with focused quiz questions that help you check what you know, review explanations, and build confidence with test-style prompts.

What this quiz covers

This quiz focuses on Implicit Vs Explicit Solutions, 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.

Question 1

An implicit solution to a first-order differential equation is given by the relation arctan⁡(y/x)−ln⁡(x2+y2)=C\arctan(y/x) - \ln(\sqrt{x^2+y^2}) = Carctan(y/x)−ln(x2+y2​)=C. What is the differential equation?

  1. y′=x−yx+yy' = \frac{x-y}{x+y}y′=x+yx−y​
  2. y′=y−xx+yy' = \frac{y-x}{x+y}y′=x+yy−x​
  3. y′=x+yx−yy' = \frac{x+y}{x-y}y′=x−yx+y​
  4. y′=x+2yxy' = \frac{x+2y}{x}y′=xx+2y​
Explanation: We perform implicit differentiation on the given relation with respect to xxx. First, rewrite the relation as arctan⁡(y/x)−12ln⁡(x2+y2)=C\arctan(y/x) - \frac{1}{2}\ln(x^2+y^2) = Carctan(y/x)−21​ln(x2+y2)=C. Differentiating term by term: ddx(arctan⁡(y/x))=11+(y/x)2⋅xy′−yx2=x2x2+y2⋅xy′−yx2=xy′−yx2+y2\frac{d}{dx}(\arctan(y/x)) = \frac{1}{1+(y/x)^2} \cdot \frac{x y' - y}{x^2} = \frac{x^2}{x^2+y^2} \cdot \frac{x y' - y}{x^2} = \frac{x y' - y}{x^2+y^2}dxd​(arctan(y/x))=1+(y/x)21​⋅x2xy′−y​=x2+y2x2​⋅x2xy′−y​=x2+y2xy′−y​. And ddx(12ln⁡(x2+y2))=12⋅1x2+y2⋅(2x+2yy′)=x+yy′x2+y2\frac{d}{dx}(\frac{1}{2}\ln(x^2+y^2)) = \frac{1}{2} \cdot \frac{1}{x^2+y^2} \cdot (2x+2yy') = \frac{x+yy'}{x^2+y^2}dxd​(21​ln(x2+y2))=21​⋅x2+y21​⋅(2x+2yy′)=x2+y2x+yy′​. The derivative of the constant CCC is 000. So the equation becomes xy′−yx2+y2−x+yy′x2+y2=0\frac{x y' - y}{x^2+y^2} - \frac{x+yy'}{x^2+y^2} = 0x2+y2xy′−y​−x2+y2x+yy′​=0. Multiplying by x2+y2x^2+y^2x2+y2 gives xy′−y−(x+yy′)=0x y' - y - (x+yy') = 0xy′−y−(x+yy′)=0. Rearranging to solve for y′y'y′: xy′−yy′=x+yx y' - yy' = x+yxy′−yy′=x+y, so y′(x−y)=x+yy'(x-y) = x+yy′(x−y)=x+y. Finally, y′=x+yx−yy' = \frac{x+y}{x-y}y′=x−yx+y​.

Question 2

The implicit relation y2=sin⁡(x)+1y^2 = \sin(x) + 1y2=sin(x)+1 defines solutions to the differential equation 2yy′=cos⁡(x)2yy' = \cos(x)2yy′=cos(x). Which statement accurately describes the explicit solutions derived from this relation?

  1. There are two distinct explicit solutions, both of which are defined and differentiable for all real numbers xxx.
  2. The implicit relation defines two explicit solutions, but they are valid only on intervals where sin⁡(x)≥0\sin(x) \ge 0sin(x)≥0.
  3. There are two explicit solutions, but they are only valid as solutions to the differential equation on intervals where sin⁡(x)≠−1\sin(x) \neq -1sin(x)=−1.
  4. Only one continuous explicit solution can be defined from the relation, which must be y(x)=sin⁡(x)+1y(x) = \sqrt{\sin(x)+1}y(x)=sin(x)+1​.
Explanation: The implicit relation y2=sin⁡(x)+1y^2 = \sin(x) + 1y2=sin(x)+1 yields two explicit functions: y1(x)=sin⁡(x)+1y_1(x) = \sqrt{\sin(x)+1}y1​(x)=sin(x)+1​ and y2(x)=−sin⁡(x)+1y_2(x) = -\sqrt{\sin(x)+1}y2​(x)=−sin(x)+1​. Since −1≤sin⁡(x)≤1-1 \le \sin(x) \le 1−1≤sin(x)≤1, the term sin⁡(x)+1\sin(x)+1sin(x)+1 is always non-negative, so both functions are defined for all real xxx. To be a solution to the differential equation 2yy′=cos⁡(x)2yy' = \cos(x)2yy′=cos(x), or y′=cos⁡(x)2yy' = \frac{\cos(x)}{2y}y′=2ycos(x)​, the function must be differentiable and satisfy the equation. The derivative is undefined when y=0y=0y=0. This occurs when sin⁡(x)+1=0\sin(x)+1=0sin(x)+1=0, i.e., sin⁡(x)=−1\sin(x)=-1sin(x)=−1. This happens at x=3π2+2kπx = \frac{3\pi}{2} + 2k\pix=23π​+2kπ for any integer kkk. At these points, the graphs of y1(x)y_1(x)y1​(x) and y2(x)y_2(x)y2​(x) have cusps, and the functions are not differentiable. Therefore, they can only be considered solutions on open intervals that do not contain these points.

Question 3

The implicit relation x2+y24=1x^2 + \frac{y^2}{4} = 1x2+4y2​=1 defines solutions to the differential equation y′=−4x/yy' = -4x/yy′=−4x/y. Which function represents the explicit solution satisfying the initial condition y(1/2)=3y(1/2) = \sqrt{3}y(1/2)=3​?

  1. y(x)=21−x2y(x) = 2\sqrt{1-x^2}y(x)=21−x2​ on the interval (−1,1)(-1, 1)(−1,1)
  2. y(x)=−21−x2y(x) = -2\sqrt{1-x^2}y(x)=−21−x2​ on the interval (−1,1)(-1, 1)(−1,1)
  3. y(x)=21−x2y(x) = 2\sqrt{1-x^2}y(x)=21−x2​ on the interval (−∞,∞)(-\infty, \infty)(−∞,∞)
  4. y(x)=4−x2y(x) = \sqrt{4-x^2}y(x)=4−x2​ on the interval (−2,2)(-2, 2)(−2,2)
Explanation: First, solve the implicit relation for yyy: y24=1−x2  ⟹  y2=4(1−x2)  ⟹  y=±21−x2\frac{y^2}{4} = 1 - x^2 \implies y^2 = 4(1-x^2) \implies y = \pm 2\sqrt{1-x^2}4y2​=1−x2⟹y2=4(1−x2)⟹y=±21−x2​. This gives two possible explicit solutions. The initial condition is y(1/2)=3y(1/2) = \sqrt{3}y(1/2)=3​. Since 3\sqrt{3}3​ is positive, we must select the positive branch, y(x)=21−x2y(x) = 2\sqrt{1-x^2}y(x)=21−x2​. Let's verify the initial condition: y(1/2)=21−(1/2)2=23/4=2(32)=3y(1/2) = 2\sqrt{1-(1/2)^2} = 2\sqrt{3/4} = 2(\frac{\sqrt{3}}{2}) = \sqrt{3}y(1/2)=21−(1/2)2​=23/4​=2(23​​)=3​. The solution is valid. The interval of existence requires the argument of the square root to be positive, 1−x2>01-x^2 > 01−x2>0 (not equal to zero, because yyy is in the denominator of y′y'y′), which means x2<1x^2 < 1x2<1, or −1<x<1-1 < x < 1−1<x<1. So the interval of existence is (−1,1)(-1, 1)(−1,1).

Question 4

Consider a first-order differential equation y′=f(x,y)y' = f(x,y)y′=f(x,y) and a corresponding implicit solution F(x,y)=CF(x,y)=CF(x,y)=C. Which of the following statements is necessarily true?

  1. For any constant CCC, the relation F(x,y)=CF(x,y)=CF(x,y)=C defines a single, unique explicit solution y=g(x)y=g(x)y=g(x).
  2. If an explicit solution y=g(x)y=g(x)y=g(x) is derived from F(x,y)=CF(x,y)=CF(x,y)=C, its interval of existence is the set of all xxx for which g(x)g(x)g(x) is a real number.
  3. Any explicit solution y=g(x)y=g(x)y=g(x) derived from F(x,y)=CF(x,y)=CF(x,y)=C must satisfy the identity F(x,g(x))=CF(x, g(x)) = CF(x,g(x))=C for all xxx in its interval of existence.
  4. The implicit solution F(x,y)=CF(x,y)=CF(x,y)=C can always be obtained by separating variables and integrating the differential equation.
Explanation: By definition, an explicit solution y=g(x)y=g(x)y=g(x) derived from an implicit solution F(x,y)=CF(x,y)=CF(x,y)=C is a function that, when substituted back into the implicit relation, satisfies the relation for all xxx in its domain (interval of existence). Thus, F(x,g(x))=CF(x, g(x)) = CF(x,g(x))=C must hold true. Choice A is false; an implicit relation can define multiple explicit solutions (e.g., x2+y2=Cx^2+y^2=Cx2+y2=C gives y=±C−x2y=\pm\sqrt{C-x^2}y=±C−x2​) or no real solutions. Choice B is false; the interval of existence also requires that the solution be differentiable and that the original DE be defined, which may impose stricter constraints than just the function being real (e.g., denominators cannot be zero). Choice D is false; many differential equations are not separable, and their implicit solutions must be found by other methods like using integrating factors for exact equations.

Question 5

An implicit solution to a first-order ODE is given by the family sin⁡(x+y)=xy+C\sin(x+y) = xy + Csin(x+y)=xy+C. For the specific solution curve that passes through the point (0,π)(0, \pi)(0,π), what is the slope y′y'y′ at this point?

  1. −1/2-1/2−1/2
  2. π+1\pi+1π+1
  3. π−1\pi-1π−1
  4. −(π+1)-(\pi+1)−(π+1)
Explanation: When you encounter an implicit solution to a differential equation, you need to use implicit differentiation to find the slope at any given point. The key insight is that both the function and its derivative are embedded in the implicit equation. Starting with sin⁡(x+y)=xy+C\sin(x+y) = xy + Csin(x+y)=xy+C, first find the constant CCC using the given point (0,π)(0, \pi)(0,π). Substituting: sin⁡(0+π)=0⋅π+C\sin(0+\pi) = 0 \cdot \pi + Csin(0+π)=0⋅π+C, so sin⁡(π)=0=C\sin(\pi) = 0 = Csin(π)=0=C. Thus our specific solution is sin⁡(x+y)=xy\sin(x+y) = xysin(x+y)=xy. To find y′y'y′, differentiate both sides with respect to xxx. The left side gives cos⁡(x+y)⋅(1+y′)\cos(x+y) \cdot (1 + y')cos(x+y)⋅(1+y′) using the chain rule. The right side gives y+xy′y + xy'y+xy′ using the product rule. This yields: cos⁡(x+y)(1+y′)=y+xy′\cos(x+y)(1 + y') = y + xy'cos(x+y)(1+y′)=y+xy′ At point (0,π)(0, \pi)(0,π), we have cos⁡(0+π)(1+y′)=π+0⋅y′\cos(0+\pi)(1 + y') = \pi + 0 \cdot y'cos(0+π)(1+y′)=π+0⋅y′, which simplifies to −1(1+y′)=π-1(1 + y') = \pi−1(1+y′)=π. Solving: −1−y′=π-1 - y' = \pi−1−y′=π, so y′=−1−π=−(π+1)y' = -1 - \pi = -(\pi + 1)y′=−1−π=−(π+1). Choice A (−1/2-1/2−1/2) likely comes from incorrect differentiation or arithmetic errors. Choice B (π+1\pi + 1π+1) represents forgetting the negative sign from cos⁡(π)=−1\cos(\pi) = -1cos(π)=−1. Choice C (π−1\pi - 1π−1) involves sign errors in the algebraic manipulation. Remember: with implicit differentiation problems, always substitute the given point values after differentiating, and be extra careful with signs when evaluating trigonometric functions at special angles.

Question 6

The general implicit solution to the differential equation ey(y′+1)=2xe^y(y'+1) = 2xey(y′+1)=2x is ey=2x−2+Ce−xe^y = 2x-2+Ce^{-x}ey=2x−2+Ce−x. Which equation defines the specific solution satisfying the initial condition y(1)=0y(1)=0y(1)=0?

  1. ey=2x−2+e−x−1e^y = 2x - 2 + e^{-x-1}ey=2x−2+e−x−1
  2. ey=2x−2+e−xe^y = 2x - 2 + e^{-x}ey=2x−2+e−x
  3. ey=2x−2e^y = 2x - 2ey=2x−2
  4. ey=2x−2+e1−xe^y = 2x - 2 + e^{1-x}ey=2x−2+e1−x
Explanation: When you encounter a problem asking for a specific solution to a differential equation, you need to apply the given initial condition to the general solution to find the particular constant value. Given the general solution ey=2x−2+Ce−xe^y = 2x - 2 + Ce^{-x}ey=2x−2+Ce−x and the initial condition y(1)=0y(1) = 0y(1)=0, you substitute these values to find CCC. When x=1x = 1x=1 and y=0y = 0y=0: e0=2(1)−2+Ce−1e^0 = 2(1) - 2 + Ce^{-1}e0=2(1)−2+Ce−1 1=0+Ce−11 = 0 + Ce^{-1}1=0+Ce−1 1=Ce1 = \frac{C}{e}1=eC​ C=eC = eC=e Therefore, the specific solution is ey=2x−2+ee−x=2x−2+e1−xe^y = 2x - 2 + ee^{-x} = 2x - 2 + e^{1-x}ey=2x−2+ee−x=2x−2+e1−x, which matches answer choice D. Let's examine why the other options are incorrect: A) ey=2x−2+e−x−1e^y = 2x - 2 + e^{-x-1}ey=2x−2+e−x−1 represents C=e−1=1eC = e^{-1} = \frac{1}{e}C=e−1=e1​, which would satisfy e0=0+1e⋅e−1=1e2≠1e^0 = 0 + \frac{1}{e} \cdot e^{-1} = \frac{1}{e^2} \neq 1e0=0+e1​⋅e−1=e21​=1. B) ey=2x−2+e−xe^y = 2x - 2 + e^{-x}ey=2x−2+e−x corresponds to C=1C = 1C=1, giving us e0=0+1⋅e−1=1e≠1e^0 = 0 + 1 \cdot e^{-1} = \frac{1}{e} \neq 1e0=0+1⋅e−1=e1​=1. C) ey=2x−2e^y = 2x - 2ey=2x−2 implies C=0C = 0C=0, which would mean e0=0≠1e^0 = 0 \neq 1e0=0=1. Study tip: Always substitute your initial conditions directly into the general solution to solve for the arbitrary constant. Double-check your algebra, especially when working with exponential expressions, as small errors in exponent manipulation lead to incorrect constants.

Question 7

The relation x2+y2=Cyx^2+y^2 = Cyx2+y2=Cy represents a family of circles and is proposed as a family of implicit solutions for the differential equation y′=2xyx2−y2y' = \frac{2xy}{x^2-y^2}y′=x2−y22xy​. Which statement correctly assesses this proposal?

  1. The relation is not a solution because implicit differentiation yields y′=−xy−C/2y' = \frac{-x}{y-C/2}y′=y−C/2−x​.
  2. The relation is a correct family of solutions, as can be verified by implicit differentiation and substitution.
  3. The relation is not a solution because the correct differential equation it satisfies is y′=2xyy2−x2y' = \frac{2xy}{y^2-x^2}y′=y2−x22xy​.
  4. The relation is only a solution for C=1C=1C=1, as this is the only value allowing for a non-trivial solution.
Explanation: To verify if x2+y2=Cyx^2+y^2 = Cyx2+y2=Cy is a solution, we differentiate it implicitly with respect to xxx: 2x+2yy′=Cy′2x + 2yy' = Cy'2x+2yy′=Cy′. Our goal is to obtain an expression for y′y'y′ in terms of only xxx and yyy. First, solve for y′y'y′: 2x=y′(C−2y)2x = y'(C - 2y)2x=y′(C−2y), so y′=2xC−2yy' = \frac{2x}{C-2y}y′=C−2y2x​. This expression contains CCC. We can eliminate CCC by using the original relation, C=x2+y2yC = \frac{x^2+y^2}{y}C=yx2+y2​. Substituting this into the expression for y′y'y′: y′=2x(x2+y2y)−2yy' = \frac{2x}{(\frac{x^2+y^2}{y}) - 2y}y′=(yx2+y2​)−2y2x​. To simplify the denominator, find a common denominator: y′=2xx2+y2−2y2y=2xx2−y2yy' = \frac{2x}{\frac{x^2+y^2-2y^2}{y}} = \frac{2x}{\frac{x^2-y^2}{y}}y′=yx2+y2−2y2​2x​=yx2−y2​2x​. Finally, inverting and multiplying gives y′=2xyx2−y2y' = \frac{2xy}{x^2-y^2}y′=x2−y22xy​. This matches the given differential equation, so the proposal is correct.

Question 8

The differential equation (2xy+cos⁡(y))dx+(x2−xsin⁡(y))dy=0(2xy + \cos(y))dx + (x^2 - x\sin(y))dy = 0(2xy+cos(y))dx+(x2−xsin(y))dy=0 is exact and has an implicit solution of the form F(x,y)=CF(x,y)=CF(x,y)=C. If an explicit solution y(x)y(x)y(x) passes through the point (π,π/2)(\pi, \pi/2)(π,π/2), what is the value of the constant CCC?

  1. π32\frac{\pi^3}{2}2π3​
  2. π32+1\frac{\pi^3}{2} + 12π3​+1
  3. π2(π2−1)\pi^2(\frac{\pi}{2} - 1)π2(2π​−1)
  4. π2\pi^2π2
Explanation: Since the equation is exact, there is a potential function F(x,y)F(x,y)F(x,y) such that ∂F∂x=M=2xy+cos⁡(y)\frac{\partial F}{\partial x} = M = 2xy + \cos(y)∂x∂F​=M=2xy+cos(y) and ∂F∂y=N=x2−xsin⁡(y)\frac{\partial F}{\partial y} = N = x^2 - x\sin(y)∂y∂F​=N=x2−xsin(y). Integrating MMM with respect to xxx gives F(x,y)=∫(2xy+cos⁡(y))dx=x2y+xcos⁡(y)+g(y)F(x,y) = \int (2xy + \cos(y)) dx = x^2y + x\cos(y) + g(y)F(x,y)=∫(2xy+cos(y))dx=x2y+xcos(y)+g(y). To find g(y)g(y)g(y), we differentiate this expression with respect to yyy and set it equal to NNN: ∂F∂y=x2−xsin⁡(y)+g′(y)\frac{\partial F}{\partial y} = x^2 - x\sin(y) + g'(y)∂y∂F​=x2−xsin(y)+g′(y). Comparing this with N=x2−xsin⁡(y)N = x^2 - x\sin(y)N=x2−xsin(y), we see that g′(y)=0g'(y) = 0g′(y)=0, so g(y)g(y)g(y) is a constant. We can incorporate this into the constant of integration CCC. The family of implicit solutions is x2y+xcos⁡(y)=Cx^2y + x\cos(y) = Cx2y+xcos(y)=C. To find the value of CCC for the curve passing through (π,π/2)(\pi, \pi/2)(π,π/2), we substitute these values: C=(π)2(π2)+πcos⁡(π2)=π32+π(0)=π32C = (\pi)^2(\frac{\pi}{2}) + \pi\cos(\frac{\pi}{2}) = \frac{\pi^3}{2} + \pi(0) = \frac{\pi^3}{2}C=(π)2(2π​)+πcos(2π​)=2π3​+π(0)=2π3​.

Question 9

A first-order differential equation has a general implicit solution given by y2−x2=Cy^2 - x^2 = Cy2−x2=C. Which of the following represents the explicit solution to the initial value problem with condition y(3)=2y(3)=2y(3)=2 and its largest interval of existence?

  1. y(x)=x2−5y(x) = \sqrt{x^2-5}y(x)=x2−5​ on the interval (5,∞)(\sqrt{5}, \infty)(5​,∞)
  2. y(x)=−x2−5y(x) = -\sqrt{x^2-5}y(x)=−x2−5​ on the interval (5,∞)(\sqrt{5}, \infty)(5​,∞)
  3. y(x)=x2−5y(x) = \sqrt{x^2-5}y(x)=x2−5​ on the interval (−∞,−5)∪(5,∞)(-\infty, -\sqrt{5}) \cup (\sqrt{5}, \infty)(−∞,−5​)∪(5​,∞)
  4. y(x)=x2−5y(x) = \sqrt{x^2-5}y(x)=x2−5​ on the interval (−∞,∞)(-\infty, \infty)(−∞,∞)
Explanation: First, use the initial condition y(3)=2y(3)=2y(3)=2 to find the constant CCC. Substitute x=3x=3x=3 and y=2y=2y=2 into the implicit solution: 22−32=C2^2 - 3^2 = C22−32=C, which gives 4−9=−5=C4 - 9 = -5 = C4−9=−5=C. The particular implicit solution is y2−x2=−5y^2 - x^2 = -5y2−x2=−5, or y2=x2−5y^2 = x^2 - 5y2=x2−5. Solving for yyy yields two possible explicit solutions: y=±x2−5y = \pm\sqrt{x^2-5}y=±x2−5​. The initial condition y(3)=2y(3)=2y(3)=2 has a positive yyy-value, so we must choose the positive branch: y(x)=x2−5y(x) = \sqrt{x^2-5}y(x)=x2−5​. For this solution to be defined and real, the argument of the square root must be non-negative, x2−5≥0x^2-5 \ge 0x2−5≥0, which means ∣x∣≥5|x| \ge \sqrt{5}∣x∣≥5​. Additionally, the original differential equation, which can be found by differentiating the implicit solution (2yy′−2x=0  ⟹  y′=x/y2yy' - 2x = 0 \implies y' = x/y2yy′−2x=0⟹y′=x/y), is undefined when y=0y=0y=0. This occurs when x2−5=0x^2-5=0x2−5=0, or x=±5x=\pm\sqrt{5}x=±5​. Thus, the solution is valid for ∣x∣>5|x|>\sqrt{5}∣x∣>5​. The interval of existence for a solution to an IVP must be a single continuous interval containing the initial point x=3x=3x=3. The interval containing x=3x=3x=3 is (5,∞)(\sqrt{5}, \infty)(5​,∞).

Question 10

Given that y5+y+x−cos⁡(x)=0y^5 + y + x - \cos(x) = 0y5+y+x−cos(x)=0 is an implicit solution to a first-order ordinary differential equation, which of the following statements is true regarding its explicit solution y=g(x)y=g(x)y=g(x)?

  1. The explicit solution y=g(x)y=g(x)y=g(x) cannot be found, therefore the relation cannot be a solution to any differential equation.
  2. An explicit solution y=g(x)y=g(x)y=g(x) exists for any initial condition, but finding it requires solving a non-separable differential equation.
  3. An explicit solution y=g(x)y=g(x)y=g(x) cannot be expressed in terms of elementary functions, but its derivative y′y'y′ can be found in terms of xxx and yyy.
  4. The explicit solution can be written as y(x)=cos⁡(x)−x−y5y(x) = \sqrt[5]{\cos(x) - x - y}y(x)=5cos(x)−x−y​, which shows it is implicitly defined.
Explanation: The given relation is a quintic polynomial in yyy. According to the Abel-Ruffini theorem, there is no general algebraic formula for the roots of a polynomial of degree five or higher in terms of its coefficients. This means we cannot isolate yyy to find an explicit solution y=g(x)y=g(x)y=g(x) using elementary functions (algebraic operations, exponentials, logarithms, trigonometric functions). However, we can still find the differential equation it solves using implicit differentiation: 5y4y′+y′+1+sin⁡(x)=05y^4 y' + y' + 1 + \sin(x) = 05y4y′+y′+1+sin(x)=0. Solving for y′y'y′ gives y′(5y4+1)=−1−sin⁡(x)y'(5y^4+1) = -1-\sin(x)y′(5y4+1)=−1−sin(x), so y′=−1−sin⁡(x)5y4+1y' = \frac{-1-\sin(x)}{5y^4+1}y′=5y4+1−1−sin(x)​. This shows that while the explicit solution y(x)y(x)y(x) is not expressible in a simple closed form, its derivative y′y'y′ can be expressed in terms of xxx and yyy.

Question 11

Find the explicit solution to the initial value problem y′=1x(1−y)y' = \frac{1}{x(1-y)}y′=x(1−y)1​, with y(1)=3y(1) = 3y(1)=3, and determine its largest interval of existence.

  1. y(x)=1+4−2ln⁡(x)y(x) = 1 + \sqrt{4 - 2\ln(x)}y(x)=1+4−2ln(x)​ on the interval (0,∞)(0, \infty)(0,∞)
  2. y(x)=1−4−2ln⁡(x)y(x) = 1 - \sqrt{4 - 2\ln(x)}y(x)=1−4−2ln(x)​ on the interval (0,e2)(0, e^2)(0,e2)
  3. y(x)=1+4−2ln⁡(x)y(x) = 1 + \sqrt{4 - 2\ln(x)}y(x)=1+4−2ln(x)​ on the interval (−e2,0)∪(0,e2)(-e^2, 0) \cup (0, e^2)(−e2,0)∪(0,e2)
  4. y(x)=1+4−2ln⁡(x)y(x) = 1 + \sqrt{4 - 2\ln(x)}y(x)=1+4−2ln(x)​ on the interval (0,e2)(0, e^2)(0,e2)
Explanation: When you encounter a differential equation like y′=1x(1−y)y' = \frac{1}{x(1-y)}y′=x(1−y)1​, recognize this as a separable equation. You can rearrange it so all terms involving yyy are on one side and all terms involving xxx are on the other. Separating variables gives you (1−y)dy=1xdx(1-y)dy = \frac{1}{x}dx(1−y)dy=x1​dx. Integrating both sides: ∫(1−y)dy=∫1xdx\int(1-y)dy = \int\frac{1}{x}dx∫(1−y)dy=∫x1​dx, which yields y−y22=ln⁡∣x∣+Cy - \frac{y^2}{2} = \ln|x| + Cy−2y2​=ln∣x∣+C. Using the initial condition y(1)=3y(1) = 3y(1)=3: 3−92=ln⁡(1)+C3 - \frac{9}{2} = \ln(1) + C3−29​=ln(1)+C, so C=−32C = -\frac{3}{2}C=−23​. This gives us y−y22=ln⁡(x)−32y - \frac{y^2}{2} = \ln(x) - \frac{3}{2}y−2y2​=ln(x)−23​. Rearranging: y2−2y+(2ln⁡(x)−3)=0y^2 - 2y + (2\ln(x) - 3) = 0y2−2y+(2ln(x)−3)=0. Using the quadratic formula: y=2±4−4(2ln⁡(x)−3)2=1±4−2ln⁡(x)y = \frac{2 \pm \sqrt{4 - 4(2\ln(x) - 3)}}{2} = 1 \pm \sqrt{4 - 2\ln(x)}y=22±4−4(2ln(x)−3)​​=1±4−2ln(x)​. Since y(1)=3y(1) = 3y(1)=3 and 4−2ln⁡(1)=2\sqrt{4 - 2\ln(1)} = 24−2ln(1)​=2, we need y=1+4−2ln⁡(x)y = 1 + \sqrt{4 - 2\ln(x)}y=1+4−2ln(x)​. For the domain, the expression under the square root must be non-negative: 4−2ln⁡(x)≥04 - 2\ln(x) \geq 04−2ln(x)≥0, which means ln⁡(x)≤2\ln(x) \leq 2ln(x)≤2, so x≤e2x \leq e^2x≤e2. Combined with the requirement that x>0x > 0x>0 (from the original equation), the domain is (0,e2)(0, e^2)(0,e2). Choice A incorrectly extends the interval to infinity. Choice B has the wrong sign (minus instead of plus). Choice C includes negative values where ln⁡(x)\ln(x)ln(x) is undefined. Study tip: Always check your solution against the initial condition to determine the correct sign, and carefully analyze domain restrictions from both the original equation and your final solution.

Question 12

Given the implicit solution exy−x2+y=Ke^{xy} - x^2 + y = Kexy−x2+y=K to a first-order differential equation, suppose we want to find the explicit solution satisfying y(0)=2y(0) = 2y(0)=2. What is the primary challenge in converting this to explicit form?

  1. The exponential term prevents any algebraic manipulation to isolate yyy
  2. The initial condition y(0)=2y(0) = 2y(0)=2 leads to an inconsistent system with no solution
  3. The equation is not actually a valid implicit solution to any first-order differential equation
  4. The mixed xyxyxy term in the exponent creates a transcendental equation that generally requires numerical methods
Explanation: When working with implicit solutions to differential equations, you'll often encounter situations where converting to explicit form becomes mathematically challenging or impossible using elementary algebraic methods. Let's examine what happens when we try to solve exy−x2+y=Ke^{xy} - x^2 + y = Kexy−x2+y=K for yyy explicitly. Using the initial condition y(0)=2y(0) = 2y(0)=2, we first find KKK: e0⋅2−02+2=1+2=3e^{0 \cdot 2} - 0^2 + 2 = 1 + 2 = 3e0⋅2−02+2=1+2=3. So our equation becomes exy−x2+y=3e^{xy} - x^2 + y = 3exy−x2+y=3, or exy+y=x2+3e^{xy} + y = x^2 + 3exy+y=x2+3. The fundamental problem is that yyy appears both inside the exponential function (as part of xyxyxy) and as a separate linear term. This creates a transcendental equation — one that mixes algebraic and transcendental (exponential) functions in a way that cannot be solved using standard algebraic operations. The xyxyxy term in the exponent is the culprit, making this equation impossible to solve analytically for yyy in terms of xxx. This confirms answer D. Looking at the incorrect options: A is wrong because exponential terms can often be manipulated algebraically (using logarithms, for instance) — the issue is specifically the mixed xyxyxy term. B is incorrect since substituting y(0)=2y(0) = 2y(0)=2 gives us a consistent value K=3K = 3K=3. C is false because this type of implicit relation commonly arises from first-order differential equations. Study tip: When you see yyy appearing both inside a transcendental function and elsewhere in the equation, expect that numerical methods will be needed for explicit solutions.

Question 13

The implicit solution to a first-order differential equation is given by x3+3xy2−y3=8x^3 + 3xy^2 - y^3 = 8x3+3xy2−y3=8. To express yyy explicitly as a function of xxx, which approach would be most appropriate?

  1. Direct algebraic solving for yyy since this is a quadratic equation in yyy
  2. Using implicit differentiation to find dydx\frac{dy}{dx}dxdy​, then integrating to find y(x)y(x)y(x)
  3. Recognizing this as a cubic equation in yyy and applying the cubic formula or numerical methods
  4. Parametric representation since explicit form may not exist in elementary functions
Explanation: The equation x3+3xy2−y3=8x^3 + 3xy^2 - y^3 = 8x3+3xy2−y3=8 can be rearranged as −y3+3xy2+(x3−8)=0-y^3 + 3xy^2 + (x^3 - 8) = 0−y3+3xy2+(x3−8)=0, or y3−3xy2−(x3−8)=0y^3 - 3xy^2 - (x^3 - 8) = 0y3−3xy2−(x3−8)=0. This is indeed a cubic equation in yyy for any given value of xxx. While cubic equations can be solved using the cubic formula, the expressions are often complex. Choice A is wrong because this is cubic, not quadratic in yyy. Choice B is incorrect because implicit differentiation gives us the derivative, not the original function. Choice D is overly pessimistic - while the cubic formula yields complex expressions, explicit solutions do exist in elementary functions.

Question 14

Consider the implicit solution sin⁡(xy)+x2y=C\sin(xy) + x^2y = Csin(xy)+x2y=C where CCC is a constant. Near the point where x=π2x = \frac{\pi}{2}x=2π​ and y=1y = 1y=1, which statement about converting to explicit form is most accurate?

  1. An explicit solution y=f(x)y = f(x)y=f(x) exists and can be found using inverse trigonometric functions
  2. An explicit solution exists locally by the Implicit Function Theorem since ∂F∂y≠0\frac{\partial F}{\partial y} \neq 0∂y∂F​=0 at the given point
  3. No explicit solution exists because the equation involves both trigonometric and polynomial terms
  4. The explicit solution requires solving a transcendental equation that has no closed form
Explanation: Let F(x,y)=sin⁡(xy)+x2y−CF(x,y) = \sin(xy) + x^2y - CF(x,y)=sin(xy)+x2y−C. At the point (π2,1)(\frac{\pi}{2}, 1)(2π​,1), we have ∂F∂y=xcos⁡(xy)+x2=π2cos⁡(π2)+(π2)2=0+π24≠0\frac{\partial F}{\partial y} = x\cos(xy) + x^2 = \frac{\pi}{2}\cos(\frac{\pi}{2}) + (\frac{\pi}{2})^2 = 0 + \frac{\pi^2}{4} \neq 0∂y∂F​=xcos(xy)+x2=2π​cos(2π​)+(2π​)2=0+4π2​=0. Since the partial derivative with respect to yyy is non-zero, the Implicit Function Theorem guarantees that locally around this point, yyy can be expressed as an explicit function of xxx. Choice A is wrong because inverse trig functions alone won't solve this mixed equation. Choice C is incorrect - the combination of function types doesn't prevent explicit solutions from existing. Choice D confuses the difficulty of finding a closed form with the existence of an explicit function.

Question 15

The differential equation dydx=y−xy+x\frac{dy}{dx} = \frac{y-x}{y+x}dxdy​=y+xy−x​ has the implicit solution x2+2xy−y2=Cx^2 + 2xy - y^2 = Cx2+2xy−y2=C. If we attempt to solve for yyy explicitly, we obtain y=x±x2+Cy = x \pm \sqrt{x^2 + C}y=x±x2+C​. What is the significance of the ±\pm± sign in the context of differential equations?

  1. It represents two different arbitrary constants that should be written as C1C_1C1​ and C2C_2C2​
  2. It indicates two distinct solution branches that cannot cross each other due to uniqueness theorem
  3. It shows that the original differential equation has no unique solution for any initial condition
  4. It represents mathematical artifact with no physical meaning in differential equation solutions
Explanation: The ±\pm± sign represents two distinct solution branches: y=x+x2+Cy = x + \sqrt{x^2 + C}y=x+x2+C​ and y=x−x2+Cy = x - \sqrt{x^2 + C}y=x−x2+C​. By the uniqueness theorem for first-order ODEs, if the right-hand side and its partial derivative are continuous, then solution curves cannot intersect (except possibly at singular points). Each branch represents a different family of solution curves that cannot cross each other. Choice A is wrong because CCC is the same constant - the branches differ by which square root we choose. Choice C is incorrect because uniqueness still holds for each branch given an initial condition. Choice D is wrong because the branches have real geometric meaning as different solution families.

Question 16

The implicit solution arctan⁡(y)−arctan⁡(x)=C\arctan(y) - \arctan(x) = Carctan(y)−arctan(x)=C can be converted to explicit form. If C=π4C = \frac{\pi}{4}C=4π​, which of the following correctly represents yyy as an explicit function of xxx?

  1. y=tan⁡(arctan⁡(x)+π4)=1+x1−xy = \tan\left(\arctan(x) + \frac{\pi}{4}\right) = \frac{1+x}{1-x}y=tan(arctan(x)+4π​)=1−x1+x​ for x<1x < 1x<1
  2. y=tan⁡(arctan⁡(x)+π4)=x+11−xy = \tan\left(\arctan(x) + \frac{\pi}{4}\right) = \frac{x+1}{1-x}y=tan(arctan(x)+4π​)=1−xx+1​ for x<1x < 1x<1
  3. y=x+tan⁡(π4)=x+1y = x + \tan\left(\frac{\pi}{4}\right) = x + 1y=x+tan(4π​)=x+1 for all real xxx
  4. y=sin⁡(arctan⁡(x)+π4)cos⁡(arctan⁡(x)+π4)y = \frac{\sin(\arctan(x) + \frac{\pi}{4})}{\cos(\arctan(x) + \frac{\pi}{4})}y=cos(arctan(x)+4π​)sin(arctan(x)+4π​)​ which cannot be simplified further
Explanation: When you encounter an implicit solution involving inverse trigonometric functions, the key is systematically applying trigonometric identities to convert it to explicit form. Start by isolating one of the inverse trig terms. From arctan⁡(y)−arctan⁡(x)=π4\arctan(y) - \arctan(x) = \frac{\pi}{4}arctan(y)−arctan(x)=4π​, we get arctan⁡(y)=arctan⁡(x)+π4\arctan(y) = \arctan(x) + \frac{\pi}{4}arctan(y)=arctan(x)+4π​. Taking the tangent of both sides: y=tan⁡(arctan⁡(x)+π4)y = \tan\left(\arctan(x) + \frac{\pi}{4}\right)y=tan(arctan(x)+4π​). Now apply the tangent addition formula: tan⁡(A+B)=tan⁡A+tan⁡B1−tan⁡Atan⁡B\tan(A + B) = \frac{\tan A + \tan B}{1 - \tan A \tan B}tan(A+B)=1−tanAtanBtanA+tanB​. Here, tan⁡(arctan⁡(x))=x\tan(\arctan(x)) = xtan(arctan(x))=x and tan⁡(π4)=1\tan\left(\frac{\pi}{4}\right) = 1tan(4π​)=1, so: y=x+11−x⋅1=1+x1−xy = \frac{x + 1}{1 - x \cdot 1} = \frac{1 + x}{1 - x}y=1−x⋅1x+1​=1−x1+x​ The domain restriction x<1x < 1x<1 ensures the denominator doesn't equal zero. Looking at the wrong answers: Option B has the numerator terms in the wrong order (x+1x + 1x+1 instead of 1+x1 + x1+x), though mathematically these are equivalent - but the formatting doesn't match the systematic derivation. Option C incorrectly assumes you can separate the arctangent terms linearly, treating tan⁡(arctan⁡(x)+π4)\tan(\arctan(x) + \frac{\pi}{4})tan(arctan(x)+4π​) as x+1x + 1x+1, which ignores the tangent addition formula entirely. Option D stops at the sine/cosine form without recognizing this equals the tangent function, missing the simplification opportunity. Study tip: When converting implicit solutions with inverse trig functions, always use the appropriate addition formulas rather than trying to distribute operations linearly. The tangent addition formula is especially common in differential equations solutions.

Question 17

A first-order differential equation has the implicit general solution y3+3y2x+3yx2+x3=Cy^3 + 3y^2x + 3yx^2 + x^3 = Cy3+3y2x+3yx2+x3=C. When a student attempts to convert this to explicit form by recognizing it as (x+y)3=C(x+y)^3 = C(x+y)3=C, they conclude that y=C3−xy = \sqrt[3]{C} - xy=3C​−x. What is the most significant issue with this approach?

  1. The algebraic factoring (x+y)3=x3+3x2y+3xy2+y3(x+y)^3 = x^3 + 3x^2y + 3xy^2 + y^3(x+y)3=x3+3x2y+3xy2+y3 was applied incorrectly
  2. The cube root function is not defined for negative values of CCC
  3. The solution y=C3−xy = \sqrt[3]{C} - xy=3C​−x is incomplete because cube roots can have three complex values
  4. The approach loses generality by treating CCC as a specific value rather than an arbitrary constant
Explanation: The factoring is correct: x3+3x2y+3xy2+y3=(x+y)3x^3 + 3x^2y + 3xy^2 + y^3 = (x+y)^3x3+3x2y+3xy2+y3=(x+y)3. From (x+y)3=C(x+y)^3 = C(x+y)3=C, we get x+y=C3x+y = \sqrt[3]{C}x+y=3C​, so y=C3−xy = \sqrt[3]{C} - xy=3C​−x. However, the student has only considered the real cube root. In the complex plane, the equation w3=Cw^3 = Cw3=C has three solutions: w=C3,C3ω,C3ω2w = \sqrt[3]{C}, \sqrt[3]{C}\omega, \sqrt[3]{C}\omega^2w=3C​,3C​ω,3C​ω2 where ω=e2πi/3\omega = e^{2\pi i/3}ω=e2πi/3 is a primitive cube root of unity. This gives three solution branches: y=C3−xy = \sqrt[3]{C} - xy=3C​−x, y=C3ω−xy = \sqrt[3]{C}\omega - xy=3C​ω−x, and y=C3ω2−xy = \sqrt[3]{C}\omega^2 - xy=3C​ω2−x. In real differential equations, we typically focus on real solutions, but the student's approach misses the fact that there could be multiple real branches depending on the nature of CCC. Choice A is wrong - the factoring is correct. Choice B is incorrect - cube roots of negative numbers are well-defined real numbers. Choice D is not the main issue - CCC remains arbitrary in the final form.

Question 18

Consider the implicit relation ln⁡∣y∣−ln⁡∣x∣=t+K\ln|y| - \ln|x| = t + Kln∣y∣−ln∣x∣=t+K where ttt is the independent variable and KKK is a constant. To express yyy explicitly in terms of ttt, which form is most appropriate?

  1. y=Cety = Ce^ty=Cet where C=xeKC = xe^KC=xeK is redefined as the arbitrary constant
  2. y=xet+Ky = xe^{t+K}y=xet+K where xxx remains as a parameter in the solution
  3. y=±et+Ky = \pm e^{t+K}y=±et+K accounting for the absolute value signs in the logarithms
  4. y=et+K−ln⁡∣x∣y = e^{t+K-\ln|x|}y=et+K−ln∣x∣ maintaining the logarithmic form for generality
Explanation: When you encounter implicit relations involving logarithms in differential equations, your goal is to isolate the dependent variable while properly handling constants and parameters. Starting with ln⁡∣y∣−ln⁡∣x∣=t+K\ln|y| - \ln|x| = t + Kln∣y∣−ln∣x∣=t+K, you can use the logarithm property ln⁡a−ln⁡b=ln⁡(a/b)\ln a - \ln b = \ln(a/b)lna−lnb=ln(a/b) to rewrite this as ln⁡∣yx∣=t+K\ln\left|\frac{y}{x}\right| = t + Kln​xy​​=t+K. Taking the exponential of both sides gives ∣yx∣=et+K\left|\frac{y}{x}\right| = e^{t+K}​xy​​=et+K, which means yx=±et+K\frac{y}{x} = \pm e^{t+K}xy​=±et+K. Therefore, y=±xet+Ky = \pm x e^{t+K}y=±xet+K. Since xxx and the ±\pm± sign are both constants (not functions of ttt), you can combine them into a single arbitrary constant. Let C=±xeKC = \pm x e^KC=±xeK, giving you y=Cety = Ce^ty=Cet. This is answer choice A. Choice B incorrectly keeps xxx as a separate parameter rather than absorbing it into the constant. In differential equations solutions, you typically consolidate all constant terms. Choice C attempts to handle the absolute value but fails to account for xxx properly, and the exponential form doesn't match what you get from the algebraic manipulation. Choice D maintains an unnecessarily complex logarithmic form instead of simplifying to the standard exponential solution format. Study tip: In differential equations, always look to combine constants, parameters, and signs into a single arbitrary constant CCC when expressing your final solution. This creates the cleanest, most standard form that's typically expected.