Homogeneous First-Order Equations - Differential Equations

  1. A student is solving the equation xy′=2x+yx y' = 2x + y. They correctly identify it as a homogeneous equation and apply the substitution y=vxy=vx. However, they make a common error in the substitution for y′y', replacing it with xdvdxx\frac{dv}{dx} instead of the correct v+xdvdxv+x\frac{dv}{dx}. Following this incorrect procedure, what general solution do they obtain?
    Answer: y=Cx2−2xy = Cx^2 - 2x 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 + y and using the substitution y=vxy = vx, you need to find y′y'. The correct derivative is y′=v+xdvdxy' = v + x\frac{dv}{dx} using the product rule. However, the student incorrectly uses y′=xdvdxy' = x\frac{dv}{dx}, missing the vv term. With this incorrect substitution, the equation becomes: x⋅xdvdx=2x+vxx \cdot x\frac{dv}{dx} = 2x + vx x2dvdx=x(2+v)x^2\frac{dv}{dx} = x(2 + v) xdvdx=2+vx\frac{dv}{dx} = 2 + v dvdx=2+vx\frac{dv}{dx} = \frac{2 + v}{x} This separates to dv2+v=dxx\frac{dv}{2 + v} = \frac{dx}{x}. Integrating both sides gives ln⁡∣2+v∣=ln⁡∣x∣+C1\ln|2 + v| = \ln|x| + C_1, which leads to 2+v=Cx2 + v = Cx, so v=Cx−2v = Cx - 2. Since y=vxy = vx, the incorrect solution is y=Cx2−2xy = Cx^2 - 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 = vx substitution, always remember that y′=v+xdvdxy' = v + x\frac{dv}{dx} by the product rule—the vv term is crucial and easily forgotten under exam pressure.
  2. The general solution to the differential equation 2xyy′=y2−x22xy y' = y^2-x^2 represents a family of curves. Which of the following provides the best geometric description of this family for x>0x > 0?
    Answer: Circles passing through the origin with centers on the x-axis. 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^2 can be solved using substitution. Rearranging gives y′=y2−x22xyy' = \frac{y^2 - x^2}{2xy}. This suggests trying the substitution v=yxv = \frac{y}{x}, so y=vxy = vx and 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} 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} Separating variables and integrating leads to the general solution: x2+y2=2Cxx^2 + y^2 = 2Cx, where CC is an arbitrary constant. Completing the square gives (x−C)2+y2=C2(x - C)^2 + y^2 = C^2, which represents circles with centers at (C,0)(C, 0) and radius ∣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), not at the origin. Choice D places centers on the y-axis, but our centers are at (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.
  3. Consider the initial value problem dydx=x−yx+y\frac{dy}{dx} = \frac{x-y}{x+y}, with y(1)=1y(1)=1. What is the value of yy at x=2x=2?
    Answer: −2+10-2 + \sqrt{10} The equation is homogeneous. Let v=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}. Using dydx=v+xdvdx\frac{dy}{dx} = v+x\frac{dv}{dx}, we get v+xdvdx=1−v1+vv+x\frac{dv}{dx} = \frac{1-v}{1+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}. Separating variables: v+1v2+2v−1dv=−dxx\frac{v+1}{v^2+2v-1}dv = -\frac{dx}{x}. Integrating gives 12ln⁡∣v2+2v−1∣=−ln⁡∣x∣+C\frac{1}{2}\ln|v^2+2v-1| = -\ln|x|+C. Substituting back v=y/xv=y/x and multiplying by x2x^2 leads to the implicit solution y2+2xy−x2=ky^2+2xy-x^2=k. Using the initial condition y(1)=1y(1)=1, we find 12+2(1)(1)−12=k1^2+2(1)(1)-1^2 = k, so k=2k=2. The particular solution is y2+2xy−x2=2y^2+2xy-x^2=2. At x=2x=2, we have y2+4y−4=2y^2+4y-4=2, or y2+4y−6=0y^2+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}. Since the solution starts at y(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 1.16. - 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). - C is incorrect and could arise from an error in calculating the constant kk, for example, finding k=1k=1, which leads to the equation y2+4y−5=0y^2+4y-5=0 at x=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=k.
  4. Consider the differential equation dydx=x2+xyy2+xy\frac{dy}{dx} = \frac{x^2 + xy}{y^2 + xy}. After applying the substitution v=yxv = \frac{y}{x} and simplifying, which of the following represents the resulting separable equation in terms of vv and xx?
    Answer: dvdx=1+v−v2x(v2+v)\frac{dv}{dx} = \frac{1 + v - v^2}{x(v^2 + v)} Starting with dydx=x2+xyy2+xy\frac{dy}{dx} = \frac{x^2 + xy}{y^2 + xy}, divide numerator and denominator by x2x^2 to get dydx=1+yxy2x2+yx\frac{dy}{dx} = \frac{1 + \frac{y}{x}}{\frac{y^2}{x^2} + \frac{y}{x}}. With v=yxv = \frac{y}{x}, this becomes dydx=1+vv2+v\frac{dy}{dx} = \frac{1 + v}{v^2 + v}. Since y=vxy = vx, we have dydx=v+xdvdx\frac{dy}{dx} = v + x\frac{dv}{dx}. Setting equal: v+xdvdx=1+vv2+vv + x\frac{dv}{dx} = \frac{1 + v}{v^2 + v}. Solving for dvdx\frac{dv}{dx}: xdvdx=1+vv2+v−v=1+v−v(v2+v)v2+v=1+v−v3−v2v2+v=1+v−v2v2+vx\frac{dv}{dx} = \frac{1 + v}{v^2 + v} - v = \frac{1 + v - v(v^2 + v)}{v^2 + v} = \frac{1 + v - v^3 - v^2}{v^2 + v} = \frac{1 + v - v^2}{v^2 + v}. Therefore dvdx=1+v−v2x(v2+v)\frac{dv}{dx} = \frac{1 + v - v^2}{x(v^2 + v)}. Choice B omits the vv term, choice C incorrectly separates terms, and choice D has the wrong sign.
  5. Consider the differential equation dydx=x2−y2x2+xy\frac{dy}{dx} = \frac{x^2 - y^2}{x^2 + xy}. A student claims this equation is homogeneous and applies the substitution y=vxy = vx. After simplification, they obtain dvdx=1−3v2x(1+v)\frac{dv}{dx} = \frac{1 - 3v^2}{x(1 + v)}. What error, if any, did the student make?
    Answer: The student correctly identified the equation as homogeneous but made an algebraic error in the substitution First, check if the equation is homogeneous by dividing numerator and denominator by x2x^2: dydx=1−(yx)21+yx\frac{dy}{dx} = \frac{1 - \left(\frac{y}{x}\right)^2}{1 + \frac{y}{x}}. This is indeed a function of yx\frac{y}{x} only, so it's homogeneous. With v=yxv = \frac{y}{x}, we have dydx=1−v21+v\frac{dy}{dx} = \frac{1 - v^2}{1 + v} and y=vxy = vx gives dydx=v+xdvdx\frac{dy}{dx} = v + x\frac{dv}{dx}. Setting equal: v+xdvdx=1−v21+vv + x\frac{dv}{dx} = \frac{1 - v^2}{1 + v}. Solving for dvdx\frac{dv}{dx}: xdvdx=1−v21+v−v=1−v2−v(1+v)1+v=1−v2−v−v21+v=1−v−2v21+vx\frac{dv}{dx} = \frac{1 - v^2}{1 + v} - v = \frac{1 - v^2 - v(1 + v)}{1 + v} = \frac{1 - v^2 - v - v^2}{1 + v} = \frac{1 - v - 2v^2}{1 + v}. Therefore dvdx=1−v−2v2x(1+v)\frac{dv}{dx} = \frac{1 - v - 2v^2}{x(1 + v)}. The student wrote 1−3v2x(1+v)\frac{1 - 3v^2}{x(1 + v)}, missing the −v-v term in the numerator. Choice A is wrong because the equation is homogeneous. Choice C is unnecessary since y=vxy = vx is the standard substitution. Choice D is incorrect due to the algebraic error.
  6. The general solution to the homogeneous differential equation xdydx=y+y2−x2x \frac{dy}{dx} = y + \sqrt{y^2-x^2} for y>x>0y>x>0 is sought. Which of the following equations implicitly defines the solution family?
    Answer: y+y2−x2=Cx2y + \sqrt{y^2-x^2} = Cx^2 First, divide by xx to get dydx=yx+(yx)2−1\frac{dy}{dx} = \frac{y}{x} + \sqrt{(\frac{y}{x})^2-1}. Let v=y/xv=y/x, so dydx=v+xdvdx\frac{dy}{dx}=v+x\frac{dv}{dx}. The equation becomes v+xdvdx=v+v2−1v+x\frac{dv}{dx} = v + \sqrt{v^2-1}. This simplifies to xdvdx=v2−1x\frac{dv}{dx} = \sqrt{v^2-1}. Separating variables yields dvv2−1=dxx\frac{dv}{\sqrt{v^2-1}} = \frac{dx}{x}. Integrating both sides gives ln⁡∣v+v2−1∣=ln⁡∣x∣+C1\ln|v+\sqrt{v^2-1}| = \ln|x| + C_1. Let C1=ln⁡∣C∣C_1 = \ln|C|, so ln⁡∣v+v2−1∣=ln⁡∣Cx∣\ln|v+\sqrt{v^2-1}| = \ln|Cx|. This implies v+v2−1=Cxv+\sqrt{v^2-1} = Cx. Substituting v=y/xv=y/x back gives yx+(yx)2−1=Cx\frac{y}{x} + \sqrt{(\frac{y}{x})^2-1} = Cx, which simplifies to y+y2−x2x=Cx\frac{y+\sqrt{y^2-x^2}}{x} = Cx. Therefore, y+y2−x2=Cx2y+\sqrt{y^2-x^2} = Cx^2. - B is incorrect due to a common integration error, confusing the integral of 1/v2−11/\sqrt{v^2-1} with that of 1/1−v21/\sqrt{1-v^2}. - C is incorrect and would result from a sign error, for instance starting with xdvdx=−v2−1x\frac{dv}{dx} = -\sqrt{v^2-1}. - D is incorrect due to an algebraic error in the final step, failing to multiply CxCx by xx.
  7. The solution curve for the differential equation (x+yey/x)dx−xey/xdy=0(x+ye^{y/x})dx - xe^{y/x}dy=0 passes through the point (1,0)(1, 0). What is the value of y(e)y(e)?
    Answer: eln⁡(2)e\ln(2) This differential equation has the form M(x,y)dx+N(x,y)dy=0M(x,y)dx + N(x,y)dy = 0 where you need to check if it's exact or can be made exact through an integrating factor. Here, M=x+yey/xM = x + ye^{y/x} and N=−xey/xN = -xe^{y/x}. Testing for exactness: ∂M∂y=ey/x+yey/x⋅1x\frac{\partial M}{\partial y} = e^{y/x} + ye^{y/x} \cdot \frac{1}{x} and ∂N∂x=−ey/x−xey/x⋅(−y)x2=−ey/x+yxey/x\frac{\partial N}{\partial x} = -e^{y/x} - xe^{y/x} \cdot \frac{(-y)}{x^2} = -e^{y/x} + \frac{y}{x}e^{y/x}. Since these aren't equal, the equation isn't exact. However, this equation is homogeneous since both terms have the same degree. Use the substitution v=yxv = \frac{y}{x}, so y=vxy = vx and dy=vdx+xdvdy = v dx + x dv. Substituting: (x+vxev)dx−xev(vdx+xdv)=0(x + vxe^v)dx - xe^v(v dx + x dv) = 0 Simplifying: xdx+vxevdx−vxevdx−x2evdv=0x dx + vxe^v dx - vxe^v dx - x^2e^v dv = 0 This reduces to: xdx−x2evdv=0x dx - x^2e^v dv = 0 Dividing by xx: dx−xevdv=0dx - xe^v dv = 0, or dxx=evdv\frac{dx}{x} = e^v dv Integrating: ln⁡∣x∣=ev+C\ln|x| = e^v + C Since v=yxv = \frac{y}{x}: ln⁡∣x∣=ey/x+C\ln|x| = e^{y/x} + C Using the initial condition (1,0)(1,0): ln⁡(1)=e0/1+C\ln(1) = e^{0/1} + C, so 0=1+C0 = 1 + C, giving C=−1C = -1. The solution is ln⁡∣x∣=ey/x−1\ln|x| = e^{y/x} - 1. For x=ex = e: ln⁡(e)=ey/e−1\ln(e) = e^{y/e} - 1, so 1=ey/e−11 = e^{y/e} - 1, meaning ey/e=2e^{y/e} = 2. Taking the natural log: ye=ln⁡(2)\frac{y}{e} = \ln(2), so y=eln⁡(2)y = e\ln(2). Answer D is correct. Options A, B, and C result from algebraic errors in the integration process or incorrectly applying the initial condition. Strategy tip: For homogeneous differential equations, always try the substitution v=y/xv = y/x to separate variables effectively.
  8. The general solution to x dy−y dx=x2−y2 dxx\,dy - y\,dx = \sqrt{x^2-y^2}\,dx for x>0x>0 is found using a substitution y=vxy=vx. The resulting separated equation can be written as dvg(v)=dxx\frac{dv}{g(v)} = \frac{dx}{x}. What is the function g(v)g(v)?
    Answer: 1−v2\sqrt{1-v^2} When you encounter a differential equation with terms like x dy−y dxx\,dy - y\,dx alongside expressions involving x2−y2\sqrt{x^2-y^2}, this signals a homogeneous differential equation that's perfect for the substitution y=vxy = vx. Let's work through the substitution systematically. Starting with y=vxy = vx, we get dy=v dx+x dvdy = v\,dx + x\,dv. 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}\,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}\,dx The xv dxxv\,dx terms cancel, leaving: x2 dv=x2(1−v2) dxx^2\,dv = \sqrt{x^2(1-v^2)}\,dx Since x>0x > 0, we have x2(1−v2)=x1−v2\sqrt{x^2(1-v^2)} = x\sqrt{1-v^2}, so: x2 dv=x1−v2 dxx^2\,dv = x\sqrt{1-v^2}\,dx Dividing both sides by xx: x dv=1−v2 dxx\,dv = \sqrt{1-v^2}\,dx Separating variables: dv1−v2=dxx\frac{dv}{\sqrt{1-v^2}} = \frac{dx}{x} Therefore, g(v)=1−v2g(v) = \sqrt{1-v^2}, 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 vv term that doesn't appear in our derivation. D uses v2−1\sqrt{v^2-1} instead of 1−v2\sqrt{1-v^2}, which would only be valid if ∣v∣≥1|v| \geq 1, contradicting our domain requirements. Study tip: When using y=vxy = vx substitution, always remember that dy=v dx+x dvdy = v\,dx + x\,dv and carefully track sign changes during algebraic manipulation.
  9. A differential equation of the form dydx=ax+bycx+dy\frac{dy}{dx} = \frac{ax + by}{cx + dy} is homogeneous if and only if a certain condition is satisfied. Given the equation dydx=3x+2yx+ky\frac{dy}{dx} = \frac{3x + 2y}{x + ky} where kk is a parameter, for which value(s) of kk can this equation be solved using the substitution v=yxv = \frac{y}{x}?
    Answer: Any real value of kk including k=0k = 0 A differential equation dydx=ax+bycx+dy\frac{dy}{dx} = \frac{ax + by}{cx + dy} is homogeneous when both the numerator and denominator are homogeneous functions of the same degree. For dydx=3x+2yx+ky\frac{dy}{dx} = \frac{3x + 2y}{x + ky}, both the numerator 3x+2y3x + 2y and denominator x+kyx + ky are homogeneous functions of degree 1 (each term has total degree 1 in xx and yy). This is true regardless of the value of kk. We can verify by dividing numerator and denominator by xx: dydx=3+2yx1+kyx\frac{dy}{dx} = \frac{3 + 2\frac{y}{x}}{1 + k\frac{y}{x}}, which is a function of yx\frac{y}{x} alone for any value of kk, including k=0k = 0 (which gives dydx=3+2yx\frac{dy}{dx} = 3 + 2\frac{y}{x}). The substitution v=yxv = \frac{y}{x} will work for any value of kk. Some students might think k=0k = 0 causes problems because the denominator becomes just xx, but this doesn't prevent the homogeneous substitution from working. Others might think there's a specific relationship needed between the coefficients, but homogeneity only requires that all terms have the same degree, which is satisfied here for any kk.
  10. Consider a solution curve y=f(x)y=f(x) for a homogeneous first-order differential equation dydx=G(y/x)\frac{dy}{dx} = G(y/x). If this curve passes through the point (a,b)(a, b), which of the following statements about other points and curves must be true?
    Answer: The curve defined by yc(x)=cf(x/c)y_c(x) = c f(x/c) for any constant c>0c > 0 is also a solution curve. 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) plane is scaled by a factor cc, the solution curves are mapped onto other solution curves. If 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) 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). Since f(x)f(x) is a solution, 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)). 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)). So, dycdx=G(yc/x)\frac{dy_c}{dx} = G(y_c/x), and yc(x)y_c(x) is a solution. - A is incorrect. This is only true for the simple case y′=y/xy' = y/x. - C is incorrect. The slope depends only on the ratio y/xy/x. At (ka,kb)(ka, kb), the slope is G(kb/ka)=G(b/a)G(kb/ka) = G(b/a), which is the same as the slope at (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), not homogeneous equations.
  11. Given the initial value problem dydx=yx+tan⁡(yx)\frac{dy}{dx} = \frac{y}{x} + \tan(\frac{y}{x}) with y(1)=π/6y(1) = \pi/6, what is the value of y(3)y(\sqrt{3})?
    Answer: π3\frac{\pi}{\sqrt{3}} When you encounter a differential equation of the form dydx=f(yx)\frac{dy}{dx} = f(\frac{y}{x}), you're dealing with a homogeneous equation. The key strategy is to use the substitution v=yxv = \frac{y}{x}, which means y=vxy = vx and dydx=v+xdvdx\frac{dy}{dx} = v + x\frac{dv}{dx}. Applying this substitution to dydx=yx+tan⁡(yx)\frac{dy}{dx} = \frac{y}{x} + \tan(\frac{y}{x}), we get: v+xdvdx=v+tan⁡(v)v + x\frac{dv}{dx} = v + \tan(v) This simplifies to xdvdx=tan⁡(v)x\frac{dv}{dx} = \tan(v), or dvtan⁡(v)=dxx\frac{dv}{\tan(v)} = \frac{dx}{x}. Since 1tan⁡(v)=cot⁡(v)\frac{1}{\tan(v)} = \cot(v), we have cot⁡(v)dv=dxx\cot(v)dv = \frac{dx}{x}. Integrating both sides: ln⁡∣sin⁡(v)∣=ln⁡∣x∣+C\ln|\sin(v)| = \ln|x| + C. This gives us sin⁡(v)=Cx\sin(v) = Cx, or sin⁡(yx)=Cx\sin(\frac{y}{x}) = Cx. Using the initial condition y(1)=π6y(1) = \frac{\pi}{6}: sin⁡(π/61)=C⋅1\sin(\frac{\pi/6}{1}) = C \cdot 1, so C=sin⁡(π6)=12C = \sin(\frac{\pi}{6}) = \frac{1}{2}. Therefore, sin⁡(yx)=x2\sin(\frac{y}{x}) = \frac{x}{2}. At x=3x = \sqrt{3}: sin⁡(y3)=32\sin(\frac{y}{\sqrt{3}}) = \frac{\sqrt{3}}{2}. Since sin⁡(π3)=32\sin(\frac{\pi}{3}) = \frac{\sqrt{3}}{2}, we have y3=π3\frac{y}{\sqrt{3}} = \frac{\pi}{3}, giving us y=π3y = \frac{\pi}{\sqrt{3}}. Choice A incorrectly uses the original substitution without proper integration. Choice B forgets to multiply back by xx. 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} to separate variables effectively.
  12. Find the particular solution to the differential equation (x−y)dy=(x+y)dx(x - y) dy = (x + y) dx that satisfies the initial condition y(1)=1y(1) = 1.
    Answer: 2arctan⁡(y/x)−ln⁡(x2+y2)=π/2−ln⁡(2)2\arctan(y/x) - \ln(x^2+y^2) = \pi/2 - \ln(2) 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). Let y=vxy=vx, so y′=v+xv′y' = v+xv'. The equation becomes 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). Separate variables: ((1−v)/(1+v2))dv=dx/x((1-v)/(1+v^2)) 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. This gives arctan⁡(v)−(1/2)ln⁡(1+v2)=ln⁡∣x∣+C\arctan(v) - (1/2)\ln(1+v^2) = \ln|x| + C. Substitute back v=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| + C. This simplifies to arctan⁡(y/x)−(1/2)ln⁡(x2+y2)=C\arctan(y/x) - (1/2)\ln(x^2+y^2) = C. Using y(1)=1y(1)=1: arctan⁡(1)−(1/2)ln⁡(12+12)=C\arctan(1) - (1/2)\ln(1^2+1^2) = C, so C=π/4−(1/2)ln⁡(2)C = \pi/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). 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).
  13. A solution to the differential equation xdy=(y+x2+y2)dxx dy = (y + \sqrt{x^2+y^2}) dx for x>0x>0 passes through the point (1,0)(1, 0). What is the y-intercept of the line tangent to this solution curve at x=3x=\sqrt{3}?
    Answer: −2-2 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} is a key indicator that the substitution v=yxv = \frac{y}{x} (so y=vxy = vx) will simplify the equation. Making this substitution and using dydx=v+xdvdx\frac{dy}{dx} = v + x\frac{dv}{dx}, the equation becomes: x(v+xdvdx)=v+1+v2x(v + x\frac{dv}{dx}) = v + \sqrt{1+v^2} This simplifies to xdvdx=1+v2x\frac{dv}{dx} = \sqrt{1+v^2}, which separates as: dv1+v2=dxx\frac{dv}{\sqrt{1+v^2}} = \frac{dx}{x} Integrating both sides gives sinh⁡−1(v)=ln⁡∣x∣+C\sinh^{-1}(v) = \ln|x| + C. Using the initial condition (1,0)(1,0) where v=0v = 0, we find C=0C = 0. Therefore v=sinh⁡(ln⁡x)=x2−12xv = \sinh(\ln x) = \frac{x^2-1}{2x}, so y=x2−12y = \frac{x^2-1}{2}. At x=3x = \sqrt{3}, we have y=3−12=1y = \frac{3-1}{2} = 1 and dydx=x=3\frac{dy}{dx} = x = \sqrt{3}. The tangent line at (3,1)(\sqrt{3}, 1) with slope 3\sqrt{3} is: y−1=3(x−3)y - 1 = \sqrt{3}(x - \sqrt{3}) y=3x−2y = \sqrt{3}x - 2 The y-intercept is −2-2, which is choice C. Choice A (00) might come from incorrectly using the initial point. Choice B (−1-1) could result from calculation errors in finding the slope or intercept. Choice D (1−231-2\sqrt{3}) 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.
  14. The differential equation xdydx=y+x2+y2x\frac{dy}{dx} = y + \sqrt{x^2 + y^2} can be solved using a homogeneous substitution. After making the appropriate substitution and simplification, the resulting equation in terms of the new variable requires which integration technique?
    Answer: Trigonometric substitution using v=tan⁡(θ)v = \tan(\theta) to handle the square root Dividing by xx: dydx=yx+x2+y2x=yx+1+(yx)2\frac{dy}{dx} = \frac{y}{x} + \frac{\sqrt{x^2 + y^2}}{x} = \frac{y}{x} + \sqrt{1 + \left(\frac{y}{x}\right)^2}. With v=yxv = \frac{y}{x}, this becomes v+xdvdx=v+1+v2v + x\frac{dv}{dx} = v + \sqrt{1 + v^2}, so xdvdx=1+v2x\frac{dv}{dx} = \sqrt{1 + v^2}. Separating: dv1+v2=dxx\frac{dv}{\sqrt{1 + v^2}} = \frac{dx}{x}. The left side integral ∫dv1+v2\int \frac{dv}{\sqrt{1 + v^2}} is a standard form that requires the substitution v=tan⁡(θ)v = \tan(\theta), dv=sec⁡2(θ)dθdv = \sec^2(\theta)d\theta, and 1+v2=1+tan⁡2(θ)=sec⁡(θ)\sqrt{1 + v^2} = \sqrt{1 + \tan^2(\theta)} = \sec(\theta). This gives ∫sec⁡2(θ)dθsec⁡(θ)=∫sec⁡(θ)dθ=ln⁡∣sec⁡(θ)+tan⁡(θ)∣+C\int \frac{\sec^2(\theta)d\theta}{\sec(\theta)} = \int \sec(\theta)d\theta = \ln|\sec(\theta) + \tan(\theta)| + C. Choice A is incorrect because direct integration isn't possible with the square root. Choice C is wrong because integration by parts isn't needed. Choice D is incorrect because partial fractions don't apply to this radical expression.
  15. The differential equation dydx=2xyy2−x2\frac{dy}{dx} = \frac{2xy}{y^2-x^2} can be solved as a homogeneous equation. While both standard substitutions (y=vxy=vx and x=vyx=vy) are valid, one leads to a significantly simpler integration process. Why is the substitution x=vyx=vy preferable in this case?
    Answer: Because the resulting separable equation for vv can be solved with a basic uu-substitution, whereas the alternative requires partial fractions. Let's analyze both substitutions. With y=vxy=vx, the equation becomes v+xdvdx=2vv2−1v+x\frac{dv}{dx} = \frac{2v}{v^2-1}, which leads to xdvdx=3v−v3v2−1x\frac{dv}{dx} = \frac{3v-v^3}{v^2-1}. The separated form is v2−1v(3−v2)dv=dxx\frac{v^2-1}{v(3-v^2)}dv = \frac{dx}{x}, which requires integration using partial fractions. Now consider x=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)}. Let v=x/yv=x/y, so dxdy=v+ydvdy\frac{dx}{dy} = v+y\frac{dv}{dy}. The equation becomes v+ydvdy=1−v22vv+y\frac{dv}{dy} = \frac{1-v^2}{2v}, which leads to ydvdy=1−3v22vy\frac{dv}{dy} = \frac{1-3v^2}{2v}. The separated form is 2v1−3v2dv=dyy\frac{2v}{1-3v^2}dv = \frac{dy}{y}. The integral on the left can be solved with a simple uu-substitution (u=1−3v2u=1-3v^2). Thus, the substitution x=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.
  16. The general solution to the homogeneous differential equation xdydx=y+xey/xx \frac{dy}{dx} = y + x e^{y/x} can be written in the implicit form f(x,y)=Cf(x, y) = C. Which of the following is a valid expression for f(x,y)f(x, y)?
    Answer: ln∣x∣+e−y/xln|x| + e^{-y/x} First, rewrite the equation as dydx=yx+ey/x\frac{dy}{dx} = \frac{y}{x} + e^{y/x}. This is a homogeneous equation. Use the substitution y=vxy = vx, which implies dydx=v+xdvdx\frac{dy}{dx} = v + x \frac{dv}{dx}. The equation becomes v+xdvdx=v+evv + x \frac{dv}{dx} = v + e^v. This simplifies to xdvdx=evx \frac{dv}{dx} = e^v. Separating variables, we get e−vdv=dxxe^{-v} dv = \frac{dx}{x}. Integrating both sides yields ∫e−vdv=∫dxx\int e^{-v} dv = \int \frac{dx}{x}, which gives −e−v=ln∣x∣+C1-e^{-v} = ln|x| + C_1. Substituting back v=y/xv = y/x, we have −e−y/x=ln∣x∣+C1-e^{-y/x} = ln|x| + C_1. Rearranging to the form f(x,y)=Cf(x, y) = C, we get ln∣x∣+e−y/x=−C1ln|x| + e^{-y/x} = -C_1. Letting C=−C1C = -C_1, the solution is ln∣x∣+e−y/x=Cln|x| + e^{-y/x} = C.
  17. A homogeneous differential equation of the form dydx=F(yx)\frac{dy}{dx} = F\left(\frac{y}{x}\right) is given by dydx=y2−x22xy\frac{dy}{dx} = \frac{y^2 - x^2}{2xy}. After applying the substitution v=yxv = \frac{y}{x} and reaching the separated form, the student obtains ∫2vv2−1dv=∫dxx\int \frac{2v}{v^2 - 1} dv = \int \frac{dx}{x}. Which of the following represents the correct evaluation of the left-hand integral?
    Answer: ln⁡∣v2−1∣+C\ln|v^2 - 1| + C When you encounter a homogeneous differential equation and need to evaluate an integral after substitution, the key is recognizing the correct integration technique and applying it carefully. To evaluate ∫2vv2−1dv\int \frac{2v}{v^2 - 1} dv, you should use substitution. Let u=v2−1u = v^2 - 1, so du=2v dvdu = 2v \, dv. This transforms the integral to ∫1udu=ln⁡∣u∣+C\int \frac{1}{u} du = \ln|u| + C. Substituting back gives ln⁡∣v2−1∣+C\ln|v^2 - 1| + C. Answer C is correct because it represents the proper application of the natural logarithm integration rule after the appropriate substitution. Answer A, ln⁡∣v2−1∣1/2+C\ln|v^2 - 1|^{1/2} + C, incorrectly applies logarithm properties. While ln⁡∣v2−1∣1/2=12ln⁡∣v2−1∣\ln|v^2 - 1|^{1/2} = \frac{1}{2}\ln|v^2 - 1|, this suggests the student might have confused the coefficient placement. Answer B, 12ln⁡∣v2−1∣+C\frac{1}{2}\ln|v^2 - 1| + C, represents a common error where students incorrectly handle the coefficient 2 in the numerator. This would be the result if you mistakenly treated the integral as 12∫2vv2−1dv\frac{1}{2} \int \frac{2v}{v^2 - 1} dv instead of recognizing the perfect substitution. Answer D uses partial fraction decomposition, which is unnecessary here. While 2vv2−1\frac{2v}{v^2 - 1} could theoretically be decomposed, the direct substitution method is more efficient and less error-prone. Study tip: When you see a rational function where the numerator is the derivative (or a constant multiple) of the denominator, always try uu-substitution first before attempting partial fractions. This pattern appears frequently in differential equations.
  18. A particular solution to the differential equation (x2+3y2)dx−2xydy=0(x^2 + 3y^2) dx - 2xy dy = 0 passes through the point (1,1)(1, 1). What is the value of yy when x=2x=2?
    Answer: 232\sqrt{3} The equation can be rewritten as dy/dx=(x2+3y2)/(2xy)dy/dx = (x^2 + 3y^2) / (2xy). Dividing the numerator and denominator by x2x^2 gives 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/x, so y=vxy = vx and 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). Rearranging gives x(dv/dx)=(1+3v2)/(2v)−v=(1+v2)/(2v)x(dv/dx) = (1 + 3v^2)/(2v) - v = (1 + v^2)/(2v). Separating variables yields (2v/(1+v2))dv=dx/x(2v / (1 + v^2)) dv = dx/x. Integrating both sides gives ln(1+v2)=ln∣x∣+Cln(1 + v^2) = ln|x| + C. Using the initial condition y(1)=1y(1)=1, we have x=1x=1 and v=y/x=1v=y/x=1. So, ln(1+12)=ln(1)+Cln(1+1^2) = ln(1) + C, which implies 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|). For x>0x>0, this is 1+v2=2x1+v^2 = 2x. Substituting back v=y/xv=y/x, we get 1+(y/x)2=2x1 + (y/x)^2 = 2x, which simplifies to x2+y2=2x3x^2 + y^2 = 2x^3. To find yy when x=2x=2, we substitute x=2x=2 into the solution: 22+y2=2(23)2^2 + y^2 = 2(2^3), which is 4+y2=164 + y^2 = 16. Thus, y2=12y^2 = 12, and since the initial condition has y>0y>0, we take the positive root, y=12=23y = \sqrt{12} = 2\sqrt{3}.
  19. Find the explicit solution to the initial value problem y′=yx+cos⁡2(yx)y' = \frac{y}{x} + \cos^2(\frac{y}{x}), with y(1)=π/4y(1) = \pi/4.
    Answer: y=xarctan⁡(ln⁡x+1)y = x \arctan(\ln x + 1) When you encounter a differential equation of the form y′=f(yx)y' = f\left(\frac{y}{x}\right), this signals a homogeneous equation that requires the substitution v=yxv = \frac{y}{x}, making y=vxy = vx and y′=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): v′x+v=v+cos⁡2(v)v'x + v = v + \cos^2(v) v′x=cos⁡2(v)v'x = \cos^2(v) dvcos⁡2(v)=dxx\frac{dv}{\cos^2(v)} = \frac{dx}{x} Integrating both sides: ∫sec⁡2(v) dv=∫dxx\int \sec^2(v) \, dv = \int \frac{dx}{x} This gives us tan⁡(v)=ln⁡∣x∣+C\tan(v) = \ln|x| + C, so v=arctan⁡(ln⁡∣x∣+C)v = \arctan(\ln|x| + C). Since y=vxy = vx, we have y=xarctan⁡(ln⁡∣x∣+C)y = x \arctan(\ln|x| + C). Using the initial condition y(1)=π/4y(1) = \pi/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) Therefore C=tan⁡(π/4)=1C = \tan(\pi/4) = 1, giving us y=xarctan⁡(ln⁡x+1)y = x \arctan(\ln x + 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} and don't forget to apply your initial conditions to find the integration constant.
  20. A homogeneous differential equation has the form dy/dx=F(y/x)dy/dx = F(y/x). When the substitution y=vxy=vx is made, the equation transforms into a separable equation of the form xdvdx=f(v)x \frac{dv}{dx} = f(v). If F(v)=1−v1+vF(v) = \frac{1-v}{1+v}, which of the following expressions represents the integral ∫1f(v)dv\int \frac{1}{f(v)} dv?
    Answer: −12ln⁡∣1−2v−v2∣+C-\frac{1}{2}\ln|1-2v-v^2| + C When you encounter a homogeneous differential equation problem involving the substitution y=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} where v=y/xv = y/x, the substitution y=vxy = vx gives us dydx=v+xdvdx\frac{dy}{dx} = v + x\frac{dv}{dx}. Setting this equal to F(v)F(v): v+xdvdx=1−v1+vv + x\frac{dv}{dx} = \frac{1-v}{1+v} Solving for xdvdxx\frac{dv}{dx}: 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} Therefore, f(v)=1−2v−v21+vf(v) = \frac{1-2v-v^2}{1+v}, 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. To evaluate this integral, notice that the derivative of the denominator is −2−2v-2-2v, which is −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 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) - v, as small errors here cascade through the entire solution.

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