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Differential Equations Quiz

Differential Equations Quiz: Homogeneous First Order Equations

Practice Homogeneous First Order 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 / 20

0 of 20 answered

A particular solution to the differential equation (x2+3y2)dx−2xydy=0(x^2 + 3y^2) dx - 2xy dy = 0(x2+3y2)dx−2xydy=0 passes through the point (1,1)(1, 1)(1,1). What is the value of yyy when x=2x=2x=2?

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What this quiz covers

This quiz focuses on Homogeneous First Order 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 particular solution to the differential equation (x2+3y2)dx−2xydy=0(x^2 + 3y^2) dx - 2xy dy = 0(x2+3y2)dx−2xydy=0 passes through the point (1,1)(1, 1)(1,1). What is the value of yyy when x=2x=2x=2?

  1. 232\sqrt{3}23​ (correct answer)
  2. 222\sqrt{2}22​
  3. 14\sqrt{14}14​
  4. 444

Explanation: The equation can be rewritten as dy/dx=(x2+3y2)/(2xy)dy/dx = (x^2 + 3y^2) / (2xy)dy/dx=(x2+3y2)/(2xy). Dividing the numerator and denominator by x2x^2x2 gives dy/dx=(1+3(y/x)2)/(2(y/x))dy/dx = (1 + 3(y/x)^2) / (2(y/x))dy/dx=(1+3(y/x)2)/(2(y/x)), which is a homogeneous equation. Let v=y/xv = y/xv=y/x, so y=vxy = vxy=vx and dy/dx=v+x(dv/dx)dy/dx = v + x(dv/dx)dy/dx=v+x(dv/dx). The equation becomes v+x(dv/dx)=(1+3v2)/(2v)v + x(dv/dx) = (1 + 3v^2)/(2v)v+x(dv/dx)=(1+3v2)/(2v). Rearranging gives x(dv/dx)=(1+3v2)/(2v)−v=(1+v2)/(2v)x(dv/dx) = (1 + 3v^2)/(2v) - v = (1 + v^2)/(2v)x(dv/dx)=(1+3v2)/(2v)−v=(1+v2)/(2v). Separating variables yields (2v/(1+v2))dv=dx/x(2v / (1 + v^2)) dv = dx/x(2v/(1+v2))dv=dx/x. Integrating both sides gives ln(1+v2)=ln∣x∣+Cln(1 + v^2) = ln|x| + Cln(1+v2)=ln∣x∣+C. Using the initial condition y(1)=1y(1)=1y(1)=1, we have x=1x=1x=1 and v=y/x=1v=y/x=1v=y/x=1. So, ln(1+12)=ln(1)+Cln(1+1^2) = ln(1) + Cln(1+12)=ln(1)+C, which implies C=ln(2)C = ln(2)C=ln(2). The solution is ln(1+v2)=ln∣x∣+ln(2)=ln(2∣x∣)ln(1+v^2) = ln|x| + ln(2) = ln(2|x|)ln(1+v2)=ln∣x∣+ln(2)=ln(2∣x∣). For x>0x>0x>0, this is 1+v2=2x1+v^2 = 2x1+v2=2x. Substituting back v=y/xv=y/xv=y/x, we get 1+(y/x)2=2x1 + (y/x)^2 = 2x1+(y/x)2=2x, which simplifies to x2+y2=2x3x^2 + y^2 = 2x^3x2+y2=2x3. To find yyy when x=2x=2x=2, we substitute x=2x=2x=2 into the solution: 22+y2=2(23)2^2 + y^2 = 2(2^3)22+y2=2(23), which is 4+y2=164 + y^2 = 164+y2=16. Thus, y2=12y^2 = 12y2=12, and since the initial condition has y>0y>0y>0, we take the positive root, y=12=23y = \sqrt{12} = 2\sqrt{3}y=12​=23​.

Question 2

Find the particular solution to the differential equation (x−y)dy=(x+y)dx(x - y) dy = (x + y) dx(x−y)dy=(x+y)dx that satisfies the initial condition y(1)=1y(1) = 1y(1)=1.

  1. 2arctan⁡(y/x)−ln⁡(x2+y2)=π/2−ln⁡(2)2\arctan(y/x) - \ln(x^2+y^2) = \pi/2 - \ln(2)2arctan(y/x)−ln(x2+y2)=π/2−ln(2) (correct answer)
  2. 2arctan⁡(y/x)+ln⁡(x2+y2)=π/2+ln⁡(2)2\arctan(y/x) + \ln(x^2+y^2) = \pi/2 + \ln(2)2arctan(y/x)+ln(x2+y2)=π/2+ln(2)
  3. ln⁡(x2+y2)−2arctan⁡(y/x)=ln⁡(2)−π/2\ln(x^2+y^2) - 2\arctan(y/x) = \ln(2) - \pi/2ln(x2+y2)−2arctan(y/x)=ln(2)−π/2
  4. y=xy=xy=x

Explanation: Rewrite as dy/dx=(x+y)/(x−y)=(1+y/x)/(1−y/x)dy/dx = (x+y)/(x-y) = (1+y/x)/(1-y/x)dy/dx=(x+y)/(x−y)=(1+y/x)/(1−y/x). Let y=vxy=vxy=vx, so y′=v+xv′y' = v+xv'y′=v+xv′. The equation becomes v+xv′=(1+v)/(1−v)v+xv' = (1+v)/(1-v)v+xv′=(1+v)/(1−v). Then xv′=(1+v)/(1−v)−v=(1+v−v+v2)/(1−v)=(1+v2)/(1−v)xv' = (1+v)/(1-v) - v = (1+v - v + v^2)/(1-v) = (1+v^2)/(1-v)xv′=(1+v)/(1−v)−v=(1+v−v+v2)/(1−v)=(1+v2)/(1−v). Separate variables: ((1−v)/(1+v2))dv=dx/x((1-v)/(1+v^2)) dv = dx/x((1−v)/(1+v2))dv=dx/x. Integrate: ∫(1/(1+v2)−v/(1+v2))dv=∫dx/x\int (1/(1+v^2) - v/(1+v^2)) dv = \int dx/x∫(1/(1+v2)−v/(1+v2))dv=∫dx/x. This gives arctan⁡(v)−(1/2)ln⁡(1+v2)=ln⁡∣x∣+C\arctan(v) - (1/2)\ln(1+v^2) = \ln|x| + Carctan(v)−(1/2)ln(1+v2)=ln∣x∣+C. Substitute back v=y/xv=y/xv=y/x: arctan⁡(y/x)−(1/2)ln⁡(1+(y/x)2)=ln⁡∣x∣+C\arctan(y/x) - (1/2)\ln(1+(y/x)^2) = \ln|x| + Carctan(y/x)−(1/2)ln(1+(y/x)2)=ln∣x∣+C. This simplifies to arctan⁡(y/x)−(1/2)ln⁡(x2+y2)=C\arctan(y/x) - (1/2)\ln(x^2+y^2) = Carctan(y/x)−(1/2)ln(x2+y2)=C. Using y(1)=1y(1)=1y(1)=1: arctan⁡(1)−(1/2)ln⁡(12+12)=C\arctan(1) - (1/2)\ln(1^2+1^2) = Carctan(1)−(1/2)ln(12+12)=C, so C=π/4−(1/2)ln⁡(2)C = \pi/4 - (1/2)\ln(2)C=π/4−(1/2)ln(2). The solution is arctan⁡(y/x)−(1/2)ln⁡(x2+y2)=π/4−(1/2)ln⁡(2)\arctan(y/x) - (1/2)\ln(x^2+y^2) = \pi/4 - (1/2)\ln(2)arctan(y/x)−(1/2)ln(x2+y2)=π/4−(1/2)ln(2). Multiplying by 2 gives 2arctan⁡(y/x)−ln⁡(x2+y2)=π/2−ln⁡(2)2\arctan(y/x) - \ln(x^2+y^2) = \pi/2 - \ln(2)2arctan(y/x)−ln(x2+y2)=π/2−ln(2).

Question 3

The differential equation (2x2y+y3)dx+(xy2−2x3)dy=0(2x^2y + y^3)dx + (xy^2 - 2x^3)dy = 0(2x2y+y3)dx+(xy2−2x3)dy=0 is homogeneous. After applying the substitution v=y/xv = y/xv=y/x, the equation can be written in the separable form g(v)dv=dx/xg(v)dv = dx/xg(v)dv=dx/x. What is the expression for g(v)g(v)g(v)?

  1. 2v32−v2\frac{2v^3}{2-v^2}2−v22v3​
  2. v2−24v\frac{v^2-2}{4v}4vv2−2​
  3. 2−v22v+v3\frac{2-v^2}{2v+v^3}2v+v32−v2​
  4. 2−v22v3\frac{2-v^2}{2v^3}2v32−v2​ (correct answer)

Explanation: When you encounter a homogeneous differential equation, the key strategy is using the substitution v=y/xv = y/xv=y/x (so y=vxy = vxy=vx) to transform it into a separable equation. This technique works because homogeneous equations have terms where all variables have the same total degree. Starting with (2x2y+y3)dx+(xy2−2x3)dy=0(2x^2y + y^3)dx + (xy^2 - 2x^3)dy = 0(2x2y+y3)dx+(xy2−2x3)dy=0, substitute y=vxy = vxy=vx and dy=vdx+xdvdy = v dx + x dvdy=vdx+xdv: (2x2(vx)+(vx)3)dx+(x(vx)2−2x3)(vdx+xdv)=0(2x^2(vx) + (vx)^3)dx + (x(vx)^2 - 2x^3)(v dx + x dv) = 0(2x2(vx)+(vx)3)dx+(x(vx)2−2x3)(vdx+xdv)=0 Simplifying: (2x3v+v3x3)dx+(xv2x2−2x3)(vdx+xdv)=0(2x^3v + v^3x^3)dx + (xv^2x^2 - 2x^3)(v dx + x dv) = 0(2x3v+v3x3)dx+(xv2x2−2x3)(vdx+xdv)=0 This becomes: (2x3v+v3x3)dx+(x3v2−2x3)vdx+(x3v2−2x3)xdv=0(2x^3v + v^3x^3)dx + (x^3v^2 - 2x^3)v dx + (x^3v^2 - 2x^3)x dv = 0(2x3v+v3x3)dx+(x3v2−2x3)vdx+(x3v2−2x3)xdv=0 Collecting dxdxdx terms: [2x3v+v3x3+x3v3−2x3v]dx+x4(v2−2)dv=0[2x^3v + v^3x^3 + x^3v^3 - 2x^3v]dx + x^4(v^2 - 2)dv = 0[2x3v+v3x3+x3v3−2x3v]dx+x4(v2−2)dv=0 The dxdxdx terms cancel to give 2v3x3dx2v^3x^3dx2v3x3dx, so: 2v3x3dx+x4(v2−2)dv=02v^3x^3dx + x^4(v^2 - 2)dv = 02v3x3dx+x4(v2−2)dv=0 Dividing by x3x^3x3: 2v3dx+x(v2−2)dv=02v^3dx + x(v^2 - 2)dv = 02v3dx+x(v2−2)dv=0 Rearranging: dvv2−2=−2v3xdx\frac{dv}{v^2 - 2} = -\frac{2v^3}{x}dxv2−2dv​=−x2v3​dx, which gives us g(v)=2−v22v3g(v) = \frac{2-v^2}{2v^3}g(v)=2v32−v2​ when written as g(v)dv=dxxg(v)dv = \frac{dx}{x}g(v)dv=xdx​. Answer D is correct. Answer A has the wrong sign in the numerator. Answer B has incorrect powers and missing factors. Answer C has the denominator wrong and doesn't match the algebraic manipulation. Remember: when applying the homogeneous substitution, carefully track all terms through the algebra—small errors in sign or powers will lead you to incorrect separable forms.

Question 4

Given the initial value problem dydx=yx+tan⁡(yx)\frac{dy}{dx} = \frac{y}{x} + \tan(\frac{y}{x})dxdy​=xy​+tan(xy​) with y(1)=π/6y(1) = \pi/6y(1)=π/6, what is the value of y(3)y(\sqrt{3})y(3​)?

  1. π36\frac{\pi\sqrt{3}}{6}6π3​​
  2. π3\frac{\pi}{3}3π​
  3. 2π33\frac{2\pi\sqrt{3}}{3}32π3​​
  4. π3\frac{\pi}{\sqrt{3}}3​π​ (correct answer)

Explanation: When you encounter a differential equation of the form dydx=f(yx)\frac{dy}{dx} = f(\frac{y}{x})dxdy​=f(xy​), you're dealing with a homogeneous equation. The key strategy is to use the substitution v=yxv = \frac{y}{x}v=xy​, which means y=vxy = vxy=vx and dydx=v+xdvdx\frac{dy}{dx} = v + x\frac{dv}{dx}dxdy​=v+xdxdv​. Applying this substitution to dydx=yx+tan⁡(yx)\frac{dy}{dx} = \frac{y}{x} + \tan(\frac{y}{x})dxdy​=xy​+tan(xy​), we get: v+xdvdx=v+tan⁡(v)v + x\frac{dv}{dx} = v + \tan(v)v+xdxdv​=v+tan(v) This simplifies to xdvdx=tan⁡(v)x\frac{dv}{dx} = \tan(v)xdxdv​=tan(v), or dvtan⁡(v)=dxx\frac{dv}{\tan(v)} = \frac{dx}{x}tan(v)dv​=xdx​. Since 1tan⁡(v)=cot⁡(v)\frac{1}{\tan(v)} = \cot(v)tan(v)1​=cot(v), we have cot⁡(v)dv=dxx\cot(v)dv = \frac{dx}{x}cot(v)dv=xdx​. Integrating both sides: ln⁡∣sin⁡(v)∣=ln⁡∣x∣+C\ln|\sin(v)| = \ln|x| + Cln∣sin(v)∣=ln∣x∣+C. This gives us sin⁡(v)=Cx\sin(v) = Cxsin(v)=Cx, or sin⁡(yx)=Cx\sin(\frac{y}{x}) = Cxsin(xy​)=Cx. Using the initial condition y(1)=π6y(1) = \frac{\pi}{6}y(1)=6π​: sin⁡(π/61)=C⋅1\sin(\frac{\pi/6}{1}) = C \cdot 1sin(1π/6​)=C⋅1, so C=sin⁡(π6)=12C = \sin(\frac{\pi}{6}) = \frac{1}{2}C=sin(6π​)=21​. Therefore, sin⁡(yx)=x2\sin(\frac{y}{x}) = \frac{x}{2}sin(xy​)=2x​. At x=3x = \sqrt{3}x=3​: sin⁡(y3)=32\sin(\frac{y}{\sqrt{3}}) = \frac{\sqrt{3}}{2}sin(3​y​)=23​​. Since sin⁡(π3)=32\sin(\frac{\pi}{3}) = \frac{\sqrt{3}}{2}sin(3π​)=23​​, we have y3=π3\frac{y}{\sqrt{3}} = \frac{\pi}{3}3​y​=3π​, giving us y=π3y = \frac{\pi}{\sqrt{3}}y=3​π​. Choice A incorrectly uses the original substitution without proper integration. Choice B forgets to multiply back by xxx. Choice C appears to involve computational errors in the trigonometric evaluation. Remember: homogeneous differential equations always call for the substitution v=yxv = \frac{y}{x}v=xy​ to separate variables effectively.

Question 5

A homogeneous differential equation has the form dy/dx=F(y/x)dy/dx = F(y/x)dy/dx=F(y/x). When the substitution y=vxy=vxy=vx is made, the equation transforms into a separable equation of the form xdvdx=f(v)x \frac{dv}{dx} = f(v)xdxdv​=f(v). If F(v)=1−v1+vF(v) = \frac{1-v}{1+v}F(v)=1+v1−v​, which of the following expressions represents the integral ∫1f(v)dv\int \frac{1}{f(v)} dv∫f(v)1​dv?

  1. 12ln⁡∣1−2v−v2∣+C\frac{1}{2}\ln|1-2v-v^2| + C21​ln∣1−2v−v2∣+C
  2. −12ln⁡∣1−2v−v2∣+C-\frac{1}{2}\ln|1-2v-v^2| + C−21​ln∣1−2v−v2∣+C (correct answer)
  3. −v−2ln⁡∣1−v∣+C-v - 2\ln|1-v| + C−v−2ln∣1−v∣+C
  4. −ln⁡∣1−v∣+C-\ln|1-v| + C−ln∣1−v∣+C

Explanation: When you encounter a homogeneous differential equation problem involving the substitution y=vxy = vxy=vx, you need to carefully track how the transformation affects the equation structure. Starting with dydx=F(y/x)=1−v1+v\frac{dy}{dx} = F(y/x) = \frac{1-v}{1+v}dxdy​=F(y/x)=1+v1−v​ where v=y/xv = y/xv=y/x, the substitution y=vxy = vxy=vx gives us dydx=v+xdvdx\frac{dy}{dx} = v + x\frac{dv}{dx}dxdy​=v+xdxdv​. Setting this equal to F(v)F(v)F(v): v+xdvdx=1−v1+vv + x\frac{dv}{dx} = \frac{1-v}{1+v}v+xdxdv​=1+v1−v​ Solving for xdvdxx\frac{dv}{dx}xdxdv​: xdvdx=1−v1+v−v=1−v−v(1+v)1+v=1−v−v−v21+v=1−2v−v21+vx\frac{dv}{dx} = \frac{1-v}{1+v} - v = \frac{1-v-v(1+v)}{1+v} = \frac{1-v-v-v^2}{1+v} = \frac{1-2v-v^2}{1+v}xdxdv​=1+v1−v​−v=1+v1−v−v(1+v)​=1+v1−v−v−v2​=1+v1−2v−v2​ Therefore, f(v)=1−2v−v21+vf(v) = \frac{1-2v-v^2}{1+v}f(v)=1+v1−2v−v2​, and we need ∫1f(v)dv=∫1+v1−2v−v2dv\int \frac{1}{f(v)} dv = \int \frac{1+v}{1-2v-v^2} dv∫f(v)1​dv=∫1−2v−v21+v​dv. To evaluate this integral, notice that the derivative of the denominator is −2−2v-2-2v−2−2v, which is −2(1+v)-2(1+v)−2(1+v). This means: ∫1+v1−2v−v2dv=−12∫−2(1+v)1−2v−v2dv=−12ln⁡∣1−2v−v2∣+C\int \frac{1+v}{1-2v-v^2} dv = -\frac{1}{2}\int \frac{-2(1+v)}{1-2v-v^2} dv = -\frac{1}{2}\ln|1-2v-v^2| + C∫1−2v−v21+v​dv=−21​∫1−2v−v2−2(1+v)​dv=−21​ln∣1−2v−v2∣+C This confirms answer B is correct. Answer A has the wrong sign on the coefficient. Answer C appears to come from incorrectly attempting partial fractions or making algebraic errors in the substitution. Answer D oversimplifies the denominator structure. Remember: in homogeneous equation problems, always double-check your algebra when computing f(v)=F(v)−vf(v) = F(v) - vf(v)=F(v)−v, as small errors here cascade through the entire solution.

Question 6

The general solution to the differential equation (xcos⁡(y/x)+ysin⁡(y/x))y=(ysin⁡(y/x)−xcos⁡(y/x))xy′(x \cos(y/x) + y \sin(y/x))y = (y \sin(y/x) - x \cos(y/x))x y'(xcos(y/x)+ysin(y/x))y=(ysin(y/x)−xcos(y/x))xy′ is given by which of the following implicit relations?

  1. xysin⁡(y/x)=Cxy \sin(y/x) = Cxysin(y/x)=C
  2. xycos⁡(y/x)=Cxy \cos(y/x) = Cxycos(y/x)=C (correct answer)
  3. ycos⁡(y/x)=Cy\cos(y/x) = Cycos(y/x)=C
  4. cos⁡(y/x)+(y/x)sin⁡(y/x)=C\cos(y/x) + (y/x)\sin(y/x) = Ccos(y/x)+(y/x)sin(y/x)=C

Explanation: When you encounter a differential equation with expressions involving ratios like y/xy/xy/x, this signals a homogeneous differential equation that often benefits from substitution methods or recognizing it as an exact equation. Let's rearrange this equation into standard form. Moving terms around, we get: (xcos⁡(y/x)+ysin⁡(y/x))dy−(ysin⁡(y/x)−xcos⁡(y/x))dx=0(x \cos(y/x) + y \sin(y/x))dy - (y \sin(y/x) - x \cos(y/x))dx = 0(xcos(y/x)+ysin(y/x))dy−(ysin(y/x)−xcos(y/x))dx=0 This has the form M(x,y)dx+N(x,y)dy=0M(x,y)dx + N(x,y)dy = 0M(x,y)dx+N(x,y)dy=0 where:

  • M=−(ysin⁡(y/x)−xcos⁡(y/x))=xcos⁡(y/x)−ysin⁡(y/x)M = -(y \sin(y/x) - x \cos(y/x)) = x \cos(y/x) - y \sin(y/x)M=−(ysin(y/x)−xcos(y/x))=xcos(y/x)−ysin(y/x)
  • N=xcos⁡(y/x)+ysin⁡(y/x)N = x \cos(y/x) + y \sin(y/x)N=xcos(y/x)+ysin(y/x)
For an exact equation, we need ∂M∂y=∂N∂x\frac{\partial M}{\partial y} = \frac{\partial N}{\partial x}∂y∂M​=∂x∂N​. You can verify this condition holds here, making this an exact differential equation. The solution comes from finding a function F(x,y)F(x,y)F(x,y) such that ∂F∂x=M\frac{\partial F}{\partial x} = M∂x∂F​=M and ∂F∂y=N\frac{\partial F}{\partial y} = N∂y∂F​=N. By inspection or integration, F(x,y)=xycos⁡(y/x)F(x,y) = xy\cos(y/x)F(x,y)=xycos(y/x), so the general solution is xycos⁡(y/x)=Cxy\cos(y/x) = Cxycos(y/x)=C. Choice A gives xysin⁡(y/x)=Cxy \sin(y/x) = Cxysin(y/x)=C, which would correspond to a different differential equation. Choice C, ycos⁡(y/x)=Cy\cos(y/x) = Cycos(y/x)=C, is missing the crucial xxx factor. Choice D represents a more complex expression that doesn't match our integrating function. Study tip: For homogeneous differential equations involving y/xy/xy/x ratios, always check if the equation is exact first—it's often faster than substitution methods.

Question 7

Find the particular solution to x2dydx=y2−xyx^2 \frac{dy}{dx} = y^2 - xyx2dxdy​=y2−xy that satisfies the initial condition y(1)=−1y(1)=-1y(1)=−1, and express yyy as an explicit function of xxx.

  1. y=2x1+x2y = \frac{2x}{1+x^2}y=1+x22x​
  2. y=2x3x2−3y = \frac{2x^3}{x^2-3}y=x2−32x3​
  3. y=2x1−3x2y = \frac{2x}{1-3x^2}y=1−3x22x​ (correct answer)
  4. y=2x(1−3x2)y = 2x(1-3x^2)y=2x(1−3x2)

Explanation: When you encounter a differential equation like x2dydx=y2−xyx^2 \frac{dy}{dx} = y^2 - xyx2dxdy​=y2−xy, look for opportunities to use separation of variables or recognize it as a specific type like Bernoulli or homogeneous. Let's rearrange this equation: x2dydx=y(y−x)x^2 \frac{dy}{dx} = y(y - x)x2dxdy​=y(y−x), so dydx=y(y−x)x2\frac{dy}{dx} = \frac{y(y-x)}{x^2}dxdy​=x2y(y−x)​. This is a homogeneous differential equation since we can write it as dydx=yx⋅y/x−1x/x=yx⋅(y/x−1)\frac{dy}{dx} = \frac{y}{x} \cdot \frac{y/x - 1}{x/x} = \frac{y}{x} \cdot (y/x - 1)dxdy​=xy​⋅x/xy/x−1​=xy​⋅(y/x−1). For homogeneous equations, substitute v=yxv = \frac{y}{x}v=xy​, so y=vxy = vxy=vx and dydx=v+xdvdx\frac{dy}{dx} = v + x\frac{dv}{dx}dxdy​=v+xdxdv​. Substituting: v+xdvdx=v(v−1)=v2−vv + x\frac{dv}{dx} = v(v-1) = v^2 - vv+xdxdv​=v(v−1)=v2−v. This simplifies to xdvdx=v2−2v=v(v−2)x\frac{dv}{dx} = v^2 - 2v = v(v-2)xdxdv​=v2−2v=v(v−2). Separating variables: dvv(v−2)=dxx\frac{dv}{v(v-2)} = \frac{dx}{x}v(v−2)dv​=xdx​. Using partial fractions: 1v(v−2)=1/2v−2−1/2v\frac{1}{v(v-2)} = \frac{1/2}{v-2} - \frac{1/2}{v}v(v−2)1​=v−21/2​−v1/2​. Integrating both sides and applying the initial condition y(1)=−1y(1) = -1y(1)=−1 (so v=−1v = -1v=−1 when x=1x = 1x=1), we get v=21−3x2v = \frac{2}{1-3x^2}v=1−3x22​. Since y=vxy = vxy=vx, we have y=2x1−3x2y = \frac{2x}{1-3x^2}y=1−3x22x​. Answer C is correct. Answer A has the wrong denominator form. Answer B incorrectly includes x3x^3x3 in the numerator and has a different denominator structure. Answer D isn't even a rational function. Strategy tip: For homogeneous differential equations, always try the substitution v=y/xv = y/xv=y/x to convert them into separable equations.

Question 8

The general solution to the differential equation 2xyy′=y2−x22xy y' = y^2-x^22xyy′=y2−x2 represents a family of curves. Which of the following provides the best geometric description of this family for x>0x > 0x>0?

  1. Parabolas with vertices at the origin.
  2. Circles centered at the origin.
  3. Circles passing through the origin with centers on the x-axis. (correct answer)
  4. Circles passing through the origin with centers on the y-axis.

Explanation: When you encounter a differential equation that asks about the geometric description of its solution family, your goal is to solve the equation and identify the resulting curve type. This differential equation 2xyy′=y2−x22xy y' = y^2 - x^22xyy′=y2−x2 can be solved using substitution. Rearranging gives y′=y2−x22xyy' = \frac{y^2 - x^2}{2xy}y′=2xyy2−x2​. This suggests trying the substitution v=yxv = \frac{y}{x}v=xy​, so y=vxy = vxy=vx and y′=v+xv′y' = v + xv'y′=v+xv′. Substituting: v+xv′=(vx)2−x22x(vx)=x2(v2−1)2x2v=v2−12vv + xv' = \frac{(vx)^2 - x^2}{2x(vx)} = \frac{x^2(v^2 - 1)}{2x^2v} = \frac{v^2 - 1}{2v}v+xv′=2x(vx)(vx)2−x2​=2x2vx2(v2−1)​=2vv2−1​ This simplifies to xv′=v2−12v−v=v2−1−2v22v=−v2−12vxv' = \frac{v^2 - 1}{2v} - v = \frac{v^2 - 1 - 2v^2}{2v} = \frac{-v^2 - 1}{2v}xv′=2vv2−1​−v=2vv2−1−2v2​=2v−v2−1​ Separating variables and integrating leads to the general solution: x2+y2=2Cxx^2 + y^2 = 2Cxx2+y2=2Cx, where CCC is an arbitrary constant. Completing the square gives (x−C)2+y2=C2(x - C)^2 + y^2 = C^2(x−C)2+y2=C2, which represents circles with centers at (C,0)(C, 0)(C,0) and radius ∣C∣|C|∣C∣. Since the radius equals the x-coordinate of the center, these circles all pass through the origin. Choice A is wrong because these aren't parabolas—they're clearly circular equations. Choice B is incorrect because the centers are at (C,0)(C, 0)(C,0), not at the origin. Choice D places centers on the y-axis, but our centers are at (C,0)(C, 0)(C,0) on the x-axis. Study tip: When solving differential equations geometrically, always complete the square on the final implicit equation to identify the standard form and geometric properties of the curve family.

Question 9

The non-homogeneous differential equation dydx=y−x+1y+x+5\frac{dy}{dx} = \frac{y-x+1}{y+x+5}dxdy​=y+x+5y−x+1​ can be transformed into a homogeneous equation in variables uuu and vvv by a substitution of the form x=u+h,y=v+kx=u+h, y=v+kx=u+h,y=v+k. What are the required constant values for hhh and kkk?

  1. h=2,k=3h = 2, k = 3h=2,k=3
  2. h=−2,k=−3h = -2, k = -3h=−2,k=−3 (correct answer)
  3. h=−3,k=−2h = -3, k = -2h=−3,k=−2
  4. h=1,k=5h = 1, k = 5h=1,k=5

Explanation: When you encounter a differential equation like dydx=y−x+1y+x+5\frac{dy}{dx} = \frac{y-x+1}{y+x+5}dxdy​=y+x+5y−x+1​, you should recognize this as a non-homogeneous equation that can be made homogeneous through translation. A homogeneous differential equation has the form dydx=f(yx)\frac{dy}{dx} = f\left(\frac{y}{x}\right)dxdy​=f(xy​), but here we have linear terms with constants that prevent this structure. To transform this equation using substitutions x=u+hx = u + hx=u+h and y=v+ky = v + ky=v+k, we need the constant terms to vanish. Substituting these expressions gives us: dvdu=(v+k)−(u+h)+1(v+k)+(u+h)+5=v−u+(k−h+1)v+u+(k+h+5)\frac{dv}{du} = \frac{(v+k)-(u+h)+1}{(v+k)+(u+h)+5} = \frac{v-u+(k-h+1)}{v+u+(k+h+5)}dudv​=(v+k)+(u+h)+5(v+k)−(u+h)+1​=v+u+(k+h+5)v−u+(k−h+1)​ For this to become homogeneous, both constant terms in the parentheses must equal zero:

  • k−h+1=0k - h + 1 = 0k−h+1=0
  • k+h+5=0k + h + 5 = 0k+h+5=0
Solving this system: From the second equation, k=−h−5k = -h - 5k=−h−5. Substituting into the first: (−h−5)−h+1=0(-h - 5) - h + 1 = 0(−h−5)−h+1=0, which gives −2h−4=0-2h - 4 = 0−2h−4=0, so h=−2h = -2h=−2. Therefore, k=−(−2)−5=−3k = -(-2) - 5 = -3k=−(−2)−5=−3. Choice A gives h=2,k=3h = 2, k = 3h=2,k=3, which would leave non-zero constant terms. Choice C reverses the values (h=−3,k=−2h = -3, k = -2h=−3,k=−2), failing to satisfy our system. Choice D (h=1,k=5h = 1, k = 5h=1,k=5) also produces non-zero constants when substituted. The answer is B: h=−2,k=−3h = -2, k = -3h=−2,k=−3. Study tip: Always set up the system by requiring both constant terms to vanish simultaneously—this is the key to transforming non-homogeneous equations into homogeneous ones.

Question 10

A solution to the differential equation xdy=(y+x2+y2)dxx dy = (y + \sqrt{x^2+y^2}) dxxdy=(y+x2+y2​)dx for x>0x>0x>0 passes through the point (1,0)(1, 0)(1,0). What is the y-intercept of the line tangent to this solution curve at x=3x=\sqrt{3}x=3​?

  1. 000
  2. −1-1−1
  3. −2-2−2 (correct answer)
  4. 1−231-2\sqrt{3}1−23​

Explanation: When you encounter a differential equation like this one, recognize it as a homogeneous equation that can be solved using the substitution method. The presence of x2+y2\sqrt{x^2+y^2}x2+y2​ is a key indicator that the substitution v=yxv = \frac{y}{x}v=xy​ (so y=vxy = vxy=vx) will simplify the equation. Making this substitution and using dydx=v+xdvdx\frac{dy}{dx} = v + x\frac{dv}{dx}dxdy​=v+xdxdv​, the equation becomes: x(v+xdvdx)=v+1+v2x(v + x\frac{dv}{dx}) = v + \sqrt{1+v^2}x(v+xdxdv​)=v+1+v2​ This simplifies to xdvdx=1+v2x\frac{dv}{dx} = \sqrt{1+v^2}xdxdv​=1+v2​, which separates as: dv1+v2=dxx\frac{dv}{\sqrt{1+v^2}} = \frac{dx}{x}1+v2​dv​=xdx​ Integrating both sides gives sinh⁡−1(v)=ln⁡∣x∣+C\sinh^{-1}(v) = \ln|x| + Csinh−1(v)=ln∣x∣+C. Using the initial condition (1,0)(1,0)(1,0) where v=0v = 0v=0, we find C=0C = 0C=0. Therefore v=sinh⁡(ln⁡x)=x2−12xv = \sinh(\ln x) = \frac{x^2-1}{2x}v=sinh(lnx)=2xx2−1​, so y=x2−12y = \frac{x^2-1}{2}y=2x2−1​. At x=3x = \sqrt{3}x=3​, we have y=3−12=1y = \frac{3-1}{2} = 1y=23−1​=1 and dydx=x=3\frac{dy}{dx} = x = \sqrt{3}dxdy​=x=3​. The tangent line at (3,1)(\sqrt{3}, 1)(3​,1) with slope 3\sqrt{3}3​ is: y−1=3(x−3)y - 1 = \sqrt{3}(x - \sqrt{3})y−1=3​(x−3​) y=3x−2y = \sqrt{3}x - 2y=3​x−2 The y-intercept is −2-2−2, which is choice C. Choice A (000) might come from incorrectly using the initial point. Choice B (−1-1−1) could result from calculation errors in finding the slope or intercept. Choice D (1−231-2\sqrt{3}1−23​) might arise from sign errors or incorrect substitution of the point coordinates. Always verify your solution satisfies both the differential equation and initial condition before finding tangent lines.

Question 11

The general solution to the homogeneous differential equation xdydx=y+xey/xx \frac{dy}{dx} = y + x e^{y/x}xdxdy​=y+xey/x can be written in the implicit form f(x,y)=Cf(x, y) = Cf(x,y)=C. Which of the following is a valid expression for f(x,y)f(x, y)f(x,y)?

  1. ln∣x∣+e−y/xln|x| + e^{-y/x}ln∣x∣+e−y/x (correct answer)
  2. ln∣x∣−e−y/xln|x| - e^{-y/x}ln∣x∣−e−y/x
  3. ey/x−ln∣x∣e^{y/x} - ln|x|ey/x−ln∣x∣
  4. e−y/x+xe^{-y/x} + xe−y/x+x

Explanation: First, rewrite the equation as dydx=yx+ey/x\frac{dy}{dx} = \frac{y}{x} + e^{y/x}dxdy​=xy​+ey/x. This is a homogeneous equation. Use the substitution y=vxy = vxy=vx, which implies dydx=v+xdvdx\frac{dy}{dx} = v + x \frac{dv}{dx}dxdy​=v+xdxdv​. The equation becomes v+xdvdx=v+evv + x \frac{dv}{dx} = v + e^vv+xdxdv​=v+ev. This simplifies to xdvdx=evx \frac{dv}{dx} = e^vxdxdv​=ev. Separating variables, we get e−vdv=dxxe^{-v} dv = \frac{dx}{x}e−vdv=xdx​. Integrating both sides yields ∫e−vdv=∫dxx\int e^{-v} dv = \int \frac{dx}{x}∫e−vdv=∫xdx​, which gives −e−v=ln∣x∣+C1-e^{-v} = ln|x| + C_1−e−v=ln∣x∣+C1​. Substituting back v=y/xv = y/xv=y/x, we have −e−y/x=ln∣x∣+C1-e^{-y/x} = ln|x| + C_1−e−y/x=ln∣x∣+C1​. Rearranging to the form f(x,y)=Cf(x, y) = Cf(x,y)=C, we get ln∣x∣+e−y/x=−C1ln|x| + e^{-y/x} = -C_1ln∣x∣+e−y/x=−C1​. Letting C=−C1C = -C_1C=−C1​, the solution is ln∣x∣+e−y/x=Cln|x| + e^{-y/x} = Cln∣x∣+e−y/x=C.

Question 12

Find the particular solution to the initial value problem x2dydx=y2+xyx^2 \frac{dy}{dx} = y^2 + xyx2dxdy​=y2+xy, with y(1)=−2y(1) = -2y(1)=−2.

  1. y=−2x2ln⁡x+1y = \frac{-2x}{2\ln x + 1}y=2lnx+1−2x​ (correct answer)
  2. y=2x21−2xy = \frac{2x^2}{1-2x}y=1−2x2x2​
  3. y=2x1−2ln⁡xy = \frac{2x}{1 - 2\ln x}y=1−2lnx2x​
  4. y=−2x3/2y = -2x^{3/2}y=−2x3/2

Explanation: The equation can be rewritten as dydx=(yx)2+yx\frac{dy}{dx} = (\frac{y}{x})^2 + \frac{y}{x}dxdy​=(xy​)2+xy​, which is a homogeneous equation. Let v=y/xv = y/xv=y/x, so y=vxy=vxy=vx and dydx=v+xdvdx\frac{dy}{dx} = v + x\frac{dv}{dx}dxdy​=v+xdxdv​. Substituting gives v+xdvdx=v2+vv + x\frac{dv}{dx} = v^2 + vv+xdxdv​=v2+v, which simplifies to xdvdx=v2x\frac{dv}{dx} = v^2xdxdv​=v2. This is a separable equation: dvv2=dxx\frac{dv}{v^2} = \frac{dx}{x}v2dv​=xdx​. Integrating both sides gives −1v=ln⁡∣x∣+C-\frac{1}{v} = \ln|x| + C−v1​=ln∣x∣+C. Substituting back v=y/xv=y/xv=y/x gives −xy=ln⁡∣x∣+C-\frac{x}{y} = \ln|x| + C−yx​=ln∣x∣+C. Using the initial condition y(1)=−2y(1)=-2y(1)=−2: −1−2=ln⁡∣1∣+C-\frac{1}{-2} = \ln|1| + C−−21​=ln∣1∣+C, which implies C=1/2C = 1/2C=1/2. The implicit solution is −xy=ln⁡x+12-\frac{x}{y} = \ln x + \frac{1}{2}−yx​=lnx+21​ for x>0x>0x>0. Solving for yyy gives y=−xln⁡x+1/2=−2x2ln⁡x+1y = \frac{-x}{\ln x + 1/2} = \frac{-2x}{2\ln x + 1}y=lnx+1/2−x​=2lnx+1−2x​.

  • B is incorrect because it results from the common error of replacing dydx\frac{dy}{dx}dxdy​ with just xdvdxx\frac{dv}{dx}xdxdv​ instead of v+xdvdxv+x\frac{dv}{dx}v+xdxdv​.
  • C is incorrect due to a sign error when solving for the constant of integration or manipulating the final equation.
  • D is incorrect due to a fundamental error in integration, such as treating ∫v−2dv\int v^{-2}dv∫v−2dv as ln⁡(v2)\ln(v^2)ln(v2).

Question 13

The differential equation (x2+3y2)dx−2xy dy=0(x^2+3y^2)dx - 2xy\,dy = 0(x2+3y2)dx−2xydy=0 is homogeneous. After applying the substitution y=vxy=vxy=vx, which of the following separable differential equations in terms of vvv and xxx is obtained?

  1. 2v1+v2dv=dxx\frac{2v}{1+v^2} dv = \frac{dx}{x}1+v22v​dv=xdx​ (correct answer)
  2. 2v1+5v2dv=dxx\frac{2v}{1+5v^2} dv = \frac{dx}{x}1+5v22v​dv=xdx​
  3. 2v1+3v2dv=dxx\frac{2v}{1+3v^2} dv = \frac{dx}{x}1+3v22v​dv=xdx​
  4. 1+3v2v(1−3v2)dv=dxx\frac{1+3v^2}{v(1-3v^2)}dv = \frac{dx}{x}v(1−3v2)1+3v2​dv=xdx​

Explanation: First, rewrite the equation in the form dydx=f(x,y)\frac{dy}{dx} = f(x,y)dxdy​=f(x,y): dydx=x2+3y22xy\frac{dy}{dx} = \frac{x^2+3y^2}{2xy}dxdy​=2xyx2+3y2​. Dividing the numerator and denominator by x2x^2x2 gives dydx=1+3(y/x)22(y/x)\frac{dy}{dx} = \frac{1+3(y/x)^2}{2(y/x)}dxdy​=2(y/x)1+3(y/x)2​. Now, let v=y/xv = y/xv=y/x, so dydx=v+xdvdx\frac{dy}{dx} = v + x\frac{dv}{dx}dxdy​=v+xdxdv​. The equation becomes v+xdvdx=1+3v22vv + x\frac{dv}{dx} = \frac{1+3v^2}{2v}v+xdxdv​=2v1+3v2​. To separate the variables, we isolate xdvdxx\frac{dv}{dx}xdxdv​: xdvdx=1+3v22v−v=1+3v2−2v22v=1+v22vx\frac{dv}{dx} = \frac{1+3v^2}{2v} - v = \frac{1+3v^2 - 2v^2}{2v} = \frac{1+v^2}{2v}xdxdv​=2v1+3v2​−v=2v1+3v2−2v2​=2v1+v2​. Finally, separating the variables gives 2v1+v2dv=dxx\frac{2v}{1+v^2} dv = \frac{dx}{x}1+v22v​dv=xdx​.

  • B is incorrect because it results from adding vvv to the right side instead of subtracting it.
  • C is incorrect because it comes from forgetting the vvv term in the product rule substitution for dydx\frac{dy}{dx}dxdy​, i.e., using dydx=xdvdx\frac{dy}{dx} = x\frac{dv}{dx}dxdy​=xdxdv​.
  • D is incorrect because it would arise from incorrectly setting up the initial derivative as dydx=2xyx2+3y2\frac{dy}{dx} = \frac{2xy}{x^2+3y^2}dxdy​=x2+3y22xy​.

Question 14

The general solution to the homogeneous differential equation xdydx=y+y2−x2x \frac{dy}{dx} = y + \sqrt{y^2-x^2}xdxdy​=y+y2−x2​ for y>x>0y>x>0y>x>0 is sought. Which of the following equations implicitly defines the solution family?

  1. y+y2−x2=Cx2y + \sqrt{y^2-x^2} = Cx^2y+y2−x2​=Cx2 (correct answer)
  2. arcsin⁡(y/x)=ln⁡∣x∣+C\arcsin(y/x) = \ln|x| + Carcsin(y/x)=ln∣x∣+C
  3. y−y2−x2=Cx2y - \sqrt{y^2-x^2} = Cx^2y−y2−x2​=Cx2
  4. y+y2−x2=Cxy + \sqrt{y^2-x^2} = Cxy+y2−x2​=Cx

Explanation: First, divide by xxx to get dydx=yx+(yx)2−1\frac{dy}{dx} = \frac{y}{x} + \sqrt{(\frac{y}{x})^2-1}dxdy​=xy​+(xy​)2−1​. Let v=y/xv=y/xv=y/x, so dydx=v+xdvdx\frac{dy}{dx}=v+x\frac{dv}{dx}dxdy​=v+xdxdv​. The equation becomes v+xdvdx=v+v2−1v+x\frac{dv}{dx} = v + \sqrt{v^2-1}v+xdxdv​=v+v2−1​. This simplifies to xdvdx=v2−1x\frac{dv}{dx} = \sqrt{v^2-1}xdxdv​=v2−1​. Separating variables yields dvv2−1=dxx\frac{dv}{\sqrt{v^2-1}} = \frac{dx}{x}v2−1​dv​=xdx​. Integrating both sides gives ln⁡∣v+v2−1∣=ln⁡∣x∣+C1\ln|v+\sqrt{v^2-1}| = \ln|x| + C_1ln∣v+v2−1​∣=ln∣x∣+C1​. Let C1=ln⁡∣C∣C_1 = \ln|C|C1​=ln∣C∣, so ln⁡∣v+v2−1∣=ln⁡∣Cx∣\ln|v+\sqrt{v^2-1}| = \ln|Cx|ln∣v+v2−1​∣=ln∣Cx∣. This implies v+v2−1=Cxv+\sqrt{v^2-1} = Cxv+v2−1​=Cx. Substituting v=y/xv=y/xv=y/x back gives yx+(yx)2−1=Cx\frac{y}{x} + \sqrt{(\frac{y}{x})^2-1} = Cxxy​+(xy​)2−1​=Cx, which simplifies to y+y2−x2x=Cx\frac{y+\sqrt{y^2-x^2}}{x} = Cxxy+y2−x2​​=Cx. Therefore, y+y2−x2=Cx2y+\sqrt{y^2-x^2} = Cx^2y+y2−x2​=Cx2.

  • B is incorrect due to a common integration error, confusing the integral of 1/v2−11/\sqrt{v^2-1}1/v2−1​ with that of 1/1−v21/\sqrt{1-v^2}1/1−v2​.
  • C is incorrect and would result from a sign error, for instance starting with xdvdx=−v2−1x\frac{dv}{dx} = -\sqrt{v^2-1}xdxdv​=−v2−1​.
  • D is incorrect due to an algebraic error in the final step, failing to multiply CxCxCx by xxx.

Question 15

The general solution to x dy−y dx=x2−y2 dxx\,dy - y\,dx = \sqrt{x^2-y^2}\,dxxdy−ydx=x2−y2​dx for x>0x>0x>0 is found using a substitution y=vxy=vxy=vx. The resulting separated equation can be written as dvg(v)=dxx\frac{dv}{g(v)} = \frac{dx}{x}g(v)dv​=xdx​. What is the function g(v)g(v)g(v)?

  1. −1−v2-\sqrt{1-v^2}−1−v2​
  2. v+1−v2v+\sqrt{1-v^2}v+1−v2​
  3. 1−v2\sqrt{1-v^2}1−v2​ (correct answer)
  4. v2−1\sqrt{v^2-1}v2−1​

Explanation: When you encounter a differential equation with terms like x dy−y dxx\,dy - y\,dxxdy−ydx alongside expressions involving x2−y2\sqrt{x^2-y^2}x2−y2​, this signals a homogeneous differential equation that's perfect for the substitution y=vxy = vxy=vx. Let's work through the substitution systematically. Starting with y=vxy = vxy=vx, we get dy=v dx+x dvdy = v\,dx + x\,dvdy=vdx+xdv. Substituting into the original equation: x(v dx+x dv)−vx dx=x2−(vx)2 dxx(v\,dx + x\,dv) - vx\,dx = \sqrt{x^2-(vx)^2}\,dxx(vdx+xdv)−vxdx=x2−(vx)2​dx Expanding the left side: xv dx+x2 dv−vx dx=x2−v2x2 dxxv\,dx + x^2\,dv - vx\,dx = \sqrt{x^2-v^2x^2}\,dxxvdx+x2dv−vxdx=x2−v2x2​dx The xv dxxv\,dxxvdx terms cancel, leaving: x2 dv=x2(1−v2) dxx^2\,dv = \sqrt{x^2(1-v^2)}\,dxx2dv=x2(1−v2)​dx Since x>0x > 0x>0, we have x2(1−v2)=x1−v2\sqrt{x^2(1-v^2)} = x\sqrt{1-v^2}x2(1−v2)​=x1−v2​, so: x2 dv=x1−v2 dxx^2\,dv = x\sqrt{1-v^2}\,dxx2dv=x1−v2​dx Dividing both sides by xxx: x dv=1−v2 dxx\,dv = \sqrt{1-v^2}\,dxxdv=1−v2​dx Separating variables: dv1−v2=dxx\frac{dv}{\sqrt{1-v^2}} = \frac{dx}{x}1−v2​dv​=xdx​ Therefore, g(v)=1−v2g(v) = \sqrt{1-v^2}g(v)=1−v2​, which is choice C. Looking at the wrong answers: A has an incorrect negative sign that would flip the direction of integration. B adds an extra vvv term that doesn't appear in our derivation. D uses v2−1\sqrt{v^2-1}v2−1​ instead of 1−v2\sqrt{1-v^2}1−v2​, which would only be valid if ∣v∣≥1|v| \geq 1∣v∣≥1, contradicting our domain requirements. Study tip: When using y=vxy = vxy=vx substitution, always remember that dy=v dx+x dvdy = v\,dx + x\,dvdy=vdx+xdv and carefully track sign changes during algebraic manipulation.

Question 16

The differential equation dydx=2xyy2−x2\frac{dy}{dx} = \frac{2xy}{y^2-x^2}dxdy​=y2−x22xy​ can be solved as a homogeneous equation. While both standard substitutions (y=vxy=vxy=vx and x=vyx=vyx=vy) are valid, one leads to a significantly simpler integration process. Why is the substitution x=vyx=vyx=vy preferable in this case?

  1. Because the term y2−x2y^2-x^2y2−x2 in the denominator suggests expressing xxx in terms of yyy.
  2. Because it transforms the equation into a first-order linear equation in vvv and yyy.
  3. Because the resulting separable equation for vvv can be solved with a basic uuu-substitution, whereas the alternative requires partial fractions. (correct answer)
  4. Because the substitution y=vxy=vxy=vx fails, as it would lead to division by zero for any solution passing through the line y=xy=xy=x.

Explanation: Let's analyze both substitutions. With y=vxy=vxy=vx, the equation becomes v+xdvdx=2vv2−1v+x\frac{dv}{dx} = \frac{2v}{v^2-1}v+xdxdv​=v2−12v​, which leads to xdvdx=3v−v3v2−1x\frac{dv}{dx} = \frac{3v-v^3}{v^2-1}xdxdv​=v2−13v−v3​. The separated form is v2−1v(3−v2)dv=dxx\frac{v^2-1}{v(3-v^2)}dv = \frac{dx}{x}v(3−v2)v2−1​dv=xdx​, which requires integration using partial fractions. Now consider x=vyx=vyx=vy. This implies dxdy=y2−x22xy=1−(x/y)22(x/y)\frac{dx}{dy} = \frac{y^2-x^2}{2xy} = \frac{1-(x/y)^2}{2(x/y)}dydx​=2xyy2−x2​=2(x/y)1−(x/y)2​. Let v=x/yv=x/yv=x/y, so dxdy=v+ydvdy\frac{dx}{dy} = v+y\frac{dv}{dy}dydx​=v+ydydv​. The equation becomes v+ydvdy=1−v22vv+y\frac{dv}{dy} = \frac{1-v^2}{2v}v+ydydv​=2v1−v2​, which leads to ydvdy=1−3v22vy\frac{dv}{dy} = \frac{1-3v^2}{2v}ydydv​=2v1−3v2​. The separated form is 2v1−3v2dv=dyy\frac{2v}{1-3v^2}dv = \frac{dy}{y}1−3v22v​dv=ydy​. The integral on the left can be solved with a simple uuu-substitution (u=1−3v2u=1-3v^2u=1−3v2). Thus, the substitution x=vyx=vyx=vy is preferable because it leads to a much simpler integral.

  • A is incorrect as this reasoning is heuristic and not mathematically precise.
  • B is incorrect because the substitution leads to a separable equation, not a linear one.
  • D is incorrect because while domain issues can be a concern, they are not the primary reason for preferring one substitution over the other based on computational efficiency.

Question 17

Consider a solution curve y=f(x)y=f(x)y=f(x) for a homogeneous first-order differential equation dydx=G(y/x)\frac{dy}{dx} = G(y/x)dxdy​=G(y/x). If this curve passes through the point (a,b)(a, b)(a,b), which of the following statements about other points and curves must be true?

  1. All solution curves are straight lines passing through the origin.
  2. The curve defined by yc(x)=cf(x/c)y_c(x) = c f(x/c)yc​(x)=cf(x/c) for any constant c>0c > 0c>0 is also a solution curve. (correct answer)
  3. The slope of the tangent to any solution curve at (ka,kb)(ka, kb)(ka,kb) is kkk times the slope at (a,b)(a,b)(a,b) for any k>0k > 0k>0.
  4. The function y=f(x)+Cy = f(x) + Cy=f(x)+C for any constant CCC represents the family of all solution curves.

Explanation: A key geometric property of homogeneous equations is that their direction fields are constant along any ray from the origin. This means that if the (x,y)(x,y)(x,y) plane is scaled by a factor ccc, the solution curves are mapped onto other solution curves. If y=f(x)y=f(x)y=f(x) is a solution, then the scaled function yc(x)=cf(x/c)y_c(x) = c f(x/c)yc​(x)=cf(x/c) is also a solution. This can be verified by differentiation: dycdx=cf′(x/c)⋅(1/c)=f′(x/c)\frac{dy_c}{dx} = c f'(x/c) \cdot (1/c) = f'(x/c)dxdyc​​=cf′(x/c)⋅(1/c)=f′(x/c). Since f(x)f(x)f(x) is a solution, f′(x)=G(f(x)/x)f'(x) = G(f(x)/x)f′(x)=G(f(x)/x). Thus, dycdx=G(f(x/c)/(x/c))\frac{dy_c}{dx} = G(f(x/c)/(x/c))dxdyc​​=G(f(x/c)/(x/c)). Also, G(yc/x)=G(cf(x/c)/x)=G(f(x/c)/(x/c))G(y_c/x) = G(cf(x/c)/x) = G(f(x/c)/(x/c))G(yc​/x)=G(cf(x/c)/x)=G(f(x/c)/(x/c)). So, dycdx=G(yc/x)\frac{dy_c}{dx} = G(y_c/x)dxdyc​​=G(yc​/x), and yc(x)y_c(x)yc​(x) is a solution.

  • A is incorrect. This is only true for the simple case y′=y/xy' = y/xy′=y/x.
  • C is incorrect. The slope depends only on the ratio y/xy/xy/x. At (ka,kb)(ka, kb)(ka,kb), the slope is G(kb/ka)=G(b/a)G(kb/ka) = G(b/a)G(kb/ka)=G(b/a), which is the same as the slope at (a,b)(a,b)(a,b).
  • D is incorrect. This describes vertical shifting, which is a property of solutions to equations of the form y′=h(x)y' = h(x)y′=h(x), not homogeneous equations.

Question 18

A student is solving the equation xy′=2x+yx y' = 2x + yxy′=2x+y. They correctly identify it as a homogeneous equation and apply the substitution y=vxy=vxy=vx. However, they make a common error in the substitution for y′y'y′, replacing it with xdvdxx\frac{dv}{dx}xdxdv​ instead of the correct v+xdvdxv+x\frac{dv}{dx}v+xdxdv​. Following this incorrect procedure, what general solution do they obtain?

  1. y=Cx−2xln⁡∣x∣y = Cx - 2x\ln|x|y=Cx−2xln∣x∣
  2. y=2xln⁡∣x∣+Cxy = 2x\ln|x| + Cxy=2xln∣x∣+Cx
  3. y=Cex−2x−2y = Ce^x - 2x - 2y=Cex−2x−2
  4. y=Cx2−2xy = Cx^2 - 2xy=Cx2−2x (correct answer)

Explanation: This problem tests your understanding of the substitution method for homogeneous differential equations, specifically what happens when you make a common algebraic error during the substitution process. Starting with xy′=2x+yxy' = 2x + yxy′=2x+y and using the substitution y=vxy = vxy=vx, you need to find y′y'y′. The correct derivative is y′=v+xdvdxy' = v + x\frac{dv}{dx}y′=v+xdxdv​ using the product rule. However, the student incorrectly uses y′=xdvdxy' = x\frac{dv}{dx}y′=xdxdv​, missing the vvv term. With this incorrect substitution, the equation becomes: x⋅xdvdx=2x+vxx \cdot x\frac{dv}{dx} = 2x + vxx⋅xdxdv​=2x+vx x2dvdx=x(2+v)x^2\frac{dv}{dx} = x(2 + v)x2dxdv​=x(2+v) xdvdx=2+vx\frac{dv}{dx} = 2 + vxdxdv​=2+v dvdx=2+vx\frac{dv}{dx} = \frac{2 + v}{x}dxdv​=x2+v​ This separates to dv2+v=dxx\frac{dv}{2 + v} = \frac{dx}{x}2+vdv​=xdx​. Integrating both sides gives ln⁡∣2+v∣=ln⁡∣x∣+C1\ln|2 + v| = \ln|x| + C_1ln∣2+v∣=ln∣x∣+C1​, which leads to 2+v=Cx2 + v = Cx2+v=Cx, so v=Cx−2v = Cx - 2v=Cx−2. Since y=vxy = vxy=vx, the incorrect solution is y=Cx2−2xy = Cx^2 - 2xy=Cx2−2x. Answer D matches this flawed derivation. Answer A represents the correct solution to the original equation. Answer B looks similar to A but with terms reversed. Answer C suggests an exponential solution, which would arise from a completely different type of equation. Study tip: When using y=vxy = vxy=vx substitution, always remember that y′=v+xdvdxy' = v + x\frac{dv}{dx}y′=v+xdxdv​ by the product rule—the vvv term is crucial and easily forgotten under exam pressure.

Question 19

Find the explicit solution to the initial value problem y′=yx+cos⁡2(yx)y' = \frac{y}{x} + \cos^2(\frac{y}{x})y′=xy​+cos2(xy​), with y(1)=π/4y(1) = \pi/4y(1)=π/4.

  1. y=xarctan⁡(ln⁡x)y = x \arctan(\ln x)y=xarctan(lnx)
  2. y=xarctan⁡(ln⁡x+1)y = x \arctan(\ln x + 1)y=xarctan(lnx+1) (correct answer)
  3. y=x(ln⁡x+π/4)y = x (\ln x + \pi/4)y=x(lnx+π/4)
  4. y=x arccot(1−ln⁡x)y = x \,\mathrm{arccot}(1-\ln x)y=xarccot(1−lnx)

Explanation: When you encounter a differential equation of the form y′=f(yx)y' = f\left(\frac{y}{x}\right)y′=f(xy​), this signals a homogeneous equation that requires the substitution v=yxv = \frac{y}{x}v=xy​, making y=vxy = vxy=vx and y′=v′x+vy' = v'x + vy′=v′x+v. Applying this substitution to y′=yx+cos⁡2(yx)y' = \frac{y}{x} + \cos^2\left(\frac{y}{x}\right)y′=xy​+cos2(xy​): v′x+v=v+cos⁡2(v)v'x + v = v + \cos^2(v)v′x+v=v+cos2(v) v′x=cos⁡2(v)v'x = \cos^2(v)v′x=cos2(v) dvcos⁡2(v)=dxx\frac{dv}{\cos^2(v)} = \frac{dx}{x}cos2(v)dv​=xdx​ Integrating both sides: ∫sec⁡2(v) dv=∫dxx\int \sec^2(v) \, dv = \int \frac{dx}{x}∫sec2(v)dv=∫xdx​ This gives us tan⁡(v)=ln⁡∣x∣+C\tan(v) = \ln|x| + Ctan(v)=ln∣x∣+C, so v=arctan⁡(ln⁡∣x∣+C)v = \arctan(\ln|x| + C)v=arctan(ln∣x∣+C). Since y=vxy = vxy=vx, we have y=xarctan⁡(ln⁡∣x∣+C)y = x \arctan(\ln|x| + C)y=xarctan(ln∣x∣+C). Using the initial condition y(1)=π/4y(1) = \pi/4y(1)=π/4: π4=1⋅arctan⁡(ln⁡(1)+C)=arctan⁡(0+C)=arctan⁡(C)\frac{\pi}{4} = 1 \cdot \arctan(\ln(1) + C) = \arctan(0 + C) = \arctan(C)4π​=1⋅arctan(ln(1)+C)=arctan(0+C)=arctan(C) Therefore C=tan⁡(π/4)=1C = \tan(\pi/4) = 1C=tan(π/4)=1, giving us y=xarctan⁡(ln⁡x+1)y = x \arctan(\ln x + 1)y=xarctan(lnx+1), which is choice B. Choice A omits the constant of integration. Choice C incorrectly assumes a linear relationship without proper integration of the trigonometric term. Choice D uses arccotangent instead of arctangent and has the wrong sign pattern. For homogeneous differential equations, always remember the key substitution v=yxv = \frac{y}{x}v=xy​ and don't forget to apply your initial conditions to find the integration constant.

Question 20

Consider the initial value problem dydx=x−yx+y\frac{dy}{dx} = \frac{x-y}{x+y}dxdy​=x+yx−y​, with y(1)=1y(1)=1y(1)=1. What is the value of yyy at x=2x=2x=2?

  1. −2+10-2 + \sqrt{10}−2+10​ (correct answer)
  2. −2−10-2 - \sqrt{10}−2−10​
  3. 111
  4. 000

Explanation: The equation is homogeneous. Let v=y/xv=y/xv=y/x. Then dydx=1−y/x1+y/x=1−v1+v\frac{dy}{dx} = \frac{1-y/x}{1+y/x} = \frac{1-v}{1+v}dxdy​=1+y/x1−y/x​=1+v1−v​. Using dydx=v+xdvdx\frac{dy}{dx} = v+x\frac{dv}{dx}dxdy​=v+xdxdv​, we get v+xdvdx=1−v1+vv+x\frac{dv}{dx} = \frac{1-v}{1+v}v+xdxdv​=1+v1−v​. This leads to xdvdx=1−v1+v−v=1−v−v−v21+v=−v2+2v−1v+1x\frac{dv}{dx} = \frac{1-v}{1+v} - v = \frac{1-v-v-v^2}{1+v} = -\frac{v^2+2v-1}{v+1}xdxdv​=1+v1−v​−v=1+v1−v−v−v2​=−v+1v2+2v−1​. Separating variables: v+1v2+2v−1dv=−dxx\frac{v+1}{v^2+2v-1}dv = -\frac{dx}{x}v2+2v−1v+1​dv=−xdx​. Integrating gives 12ln⁡∣v2+2v−1∣=−ln⁡∣x∣+C\frac{1}{2}\ln|v^2+2v-1| = -\ln|x|+C21​ln∣v2+2v−1∣=−ln∣x∣+C. Substituting back v=y/xv=y/xv=y/x and multiplying by x2x^2x2 leads to the implicit solution y2+2xy−x2=ky^2+2xy-x^2=ky2+2xy−x2=k. Using the initial condition y(1)=1y(1)=1y(1)=1, we find 12+2(1)(1)−12=k1^2+2(1)(1)-1^2 = k12+2(1)(1)−12=k, so k=2k=2k=2. The particular solution is y2+2xy−x2=2y^2+2xy-x^2=2y2+2xy−x2=2. At x=2x=2x=2, we have y2+4y−4=2y^2+4y-4=2y2+4y−4=2, or y2+4y−6=0y^2+4y-6=0y2+4y−6=0. Using the quadratic formula, y=−4±16−4(−6)2=−2±10y = \frac{-4 \pm \sqrt{16-4(-6)}}{2} = -2 \pm \sqrt{10}y=2−4±16−4(−6)​​=−2±10​. Since the solution starts at y(1)=1y(1)=1y(1)=1 (positive), and the function is continuous, we choose the positive root, y(2)=−2+10≈1.16y(2) = -2+\sqrt{10} \approx 1.16y(2)=−2+10​≈1.16.

  • B is incorrect as it is the other root from the quadratic formula, which does not match the trajectory of the solution curve starting at (1,1)(1,1)(1,1).
  • C is incorrect and could arise from an error in calculating the constant kkk, for example, finding k=1k=1k=1, which leads to the equation y2+4y−5=0y^2+4y-5=0y2+4y−5=0 at x=2x=2x=2.
  • D is incorrect and would result from a sign error during separation leading to the implicit solution y2+2xy+x2=ky^2+2xy+x^2=ky2+2xy+x2=k.