General Solutions: Separation of Variables - Calculus 1

  1. Solve the differential equation y′=y2sin⁡(x)y' = y^2 \sin(x).
    Answer: y=1cos⁡(x)+Cy = \frac{1}{\cos(x)+C} This is a separable differential equation, which means you can separate the variables and integrate both sides. When you see an equation of the form y′=f(x)g(y)y' = f(x)g(y), your strategy is to rewrite it as dydx=f(x)g(y)\frac{dy}{dx} = f(x)g(y) and then separate variables. Starting with y′=y2sin⁡(x)y' = y^2 \sin(x), rewrite as dydx=y2sin⁡(x)\frac{dy}{dx} = y^2 \sin(x). Separate variables by dividing both sides by y2y^2 and multiplying by dxdx: dyy2=sin⁡(x)dx\frac{dy}{y^2} = \sin(x) dx. Now integrate both sides: ∫y−2dy=∫sin⁡(x)dx\int y^{-2} dy = \int \sin(x) dx. The left side gives y−1−1=−1y\frac{y^{-1}}{-1} = -\frac{1}{y}, and the right side gives −cos⁡(x)-\cos(x). So you have −1y=−cos⁡(x)+C-\frac{1}{y} = -\cos(x) + C. Solving for yy: 1y=cos⁡(x)−C\frac{1}{y} = \cos(x) - C, which means y=1cos⁡(x)−Cy = \frac{1}{\cos(x) - C}. Since CC is an arbitrary constant, −C-C is also arbitrary, so we can write this as y=1cos⁡(x)+Cy = \frac{1}{\cos(x) + C}. Choice A gives y=−1cos⁡(x)+Cy = \frac{-1}{\cos(x)} + C, which has the wrong form entirely—it's not even a solution to our separated equation. Choice B, y=−cos⁡(x)+Cy = -\cos(x) + C, would give y′=sin⁡(x)y' = \sin(x), not y2sin⁡(x)y^2\sin(x). Choice C, y=ln⁡(sec⁡(x))+Cy = \ln(\sec(x)) + C, differentiates to y′=tan⁡(x)y' = \tan(x), again missing the y2y^2 term. For separable differential equations, always check your algebra when solving for the dependent variable—sign errors and reciprocal mistakes are common pitfalls.
  2. What is the general solution to the differential equation dydx=ex+y\frac{dy}{dx} = e^{x+y}?
    Answer: y=−ln⁡(C−ex)y = -\ln(C - e^x) First, use the property of exponents to rewrite the equation: dydx=exey\frac{dy}{dx} = e^x e^y. Separate the variables by dividing by eye^y: 1eydy=exdx\frac{1}{e^y} dy = e^x dx, which is e−ydy=exdxe^{-y} dy = e^x dx. Integrate both sides: ∫e−ydy=∫exdx\int e^{-y} dy = \int e^x dx. This gives −e−y=ex+C1-e^{-y} = e^x + C_1. To solve for yy, first multiply by -1: e−y=−ex−C1e^{-y} = -e^x - C_1. Let C=−C1C = -C_1. Then e−y=C−exe^{-y} = C - e^x. Take the natural logarithm of both sides: −y=ln⁡(C−ex)-y = \ln(C - e^x). Finally, multiply by -1: y=−ln⁡(C−ex)y = -\ln(C - e^x). Distractor B results from a sign error when integrating e−ye^{-y}. Distractors C and D result from fundamental misunderstandings of how to solve this type of differential equation.
  3. Which of the following represents the general solution to the differential equation y′=e2x+yy' = e^{2x+y}?
    Answer: y=−ln⁡(−12e2x+C)y = -\ln(-\frac{1}{2}e^{2x} + C) First, use exponent rules to write y′=e2xeyy' = e^{2x}e^y. Separate the variables: e−ydy=e2xdxe^{-y}dy = e^{2x}dx. Integrate both sides: ∫e−ydy=∫e2xdx\int e^{-y}dy = \int e^{2x}dx, which gives −e−y=12e2x+K-e^{-y} = \frac{1}{2}e^{2x} + K. To solve for y, first multiply by -1: e−y=−12e2x−Ke^{-y} = -\frac{1}{2}e^{2x} - K. Let C=−KC = -K, so e−y=C−12e2xe^{-y} = C - \frac{1}{2}e^{2x}. Now, take the natural logarithm of both sides: −y=ln⁡(C−12e2x)-y = \ln(C - \frac{1}{2}e^{2x}). Finally, y=−ln⁡(C−12e2x)y = -\ln(C - \frac{1}{2}e^{2x}), which is equivalent to choice B.
  4. Given dydx=ysin⁡(x)\frac{dy}{dx} = \sqrt{y} \sin(x) for y>0y > 0, find the general solution for yy.
    Answer: y=(K−12cos⁡(x))2y = (K - \frac{1}{2}\cos(x))^2 Separate the variables: 1ydy=sin⁡(x)dx\frac{1}{\sqrt{y}} dy = \sin(x) dx, or y−1/2dy=sin⁡(x)dxy^{-1/2} dy = \sin(x) dx. Integrate both sides: ∫y−1/2dy=∫sin⁡(x)dx\int y^{-1/2} dy = \int \sin(x) dx. Using the power rule for the left side and the standard integral for the right side, we get: 2y1/2=−cos⁡(x)+C12y^{1/2} = -\cos(x) + C_1. Now, solve for yy. First, divide by 2: y1/2=−12cos⁡(x)+C12y^{1/2} = -\frac{1}{2}\cos(x) + \frac{C_1}{2}. Let K=C12K = \frac{C_1}{2} be the new arbitrary constant. The equation is y=K−12cos⁡(x)\sqrt{y} = K - \frac{1}{2}\cos(x). Finally, square both sides to get the explicit solution: y=(K−12cos⁡(x))2y = (K - \frac{1}{2}\cos(x))^2. Distractor A has a sign error on the integral of sin⁡(x)\sin(x). Distractor B incorrectly handles the constant 2 from the integration. Distractor D incorrectly multiplies by 2 instead of dividing.
  5. Find the general solution for yy given the differential equation dydx=y2+1x2\frac{dy}{dx} = \frac{y^2+1}{x^2}.
    Answer: y=tan⁡(C−1x)y = \tan(C - \frac{1}{x}) First, separate the variables: 1y2+1dy=1x2dx\frac{1}{y^2+1} dy = \frac{1}{x^2} dx. Next, integrate both sides: ∫1y2+1dy=∫x−2dx\int \frac{1}{y^2+1} dy = \int x^{-2} dx. The integral of the left side is arctan⁡(y)\arctan(y). The integral of the right side is −x−1+C-x^{-1} + C, or C−1xC - \frac{1}{x}. So, we have the equation arctan⁡(y)=C−1x\arctan(y) = C - \frac{1}{x}. To solve for yy, we take the tangent of both sides: y=tan⁡(C−1x)y = \tan(C - \frac{1}{x}). Distractor B incorrectly distributes the tangent function. Distractor C forgets to apply the tangent function to solve for yy. Distractor D uses an incorrect antiderivative for 1/x21/x^2.
  6. What is the implicit general solution to the differential equation (1+y2)dx+(1+x2)dy=0(1+y^2)dx + (1+x^2)dy = 0?
    Answer: arctan⁡(y)+arctan⁡(x)=C\arctan(y) + \arctan(x) = C Rearrange the equation to (1+x2)dy=−(1+y2)dx(1+x^2)dy = -(1+y^2)dx. Separate variables: dy1+y2=−dx1+x2\frac{dy}{1+y^2} = -\frac{dx}{1+x^2}. Integrate both sides: ∫dy1+y2=−∫dx1+x2\int \frac{dy}{1+y^2} = -\int \frac{dx}{1+x^2}. This gives arctan⁡(y)=−arctan⁡(x)+C\arctan(y) = -\arctan(x) + C. Rearranging gives the implicit solution arctan⁡(y)+arctan⁡(x)=C\arctan(y) + \arctan(x) = C.
  7. What is the general solution to xdydx=yln⁡(x)x \frac{dy}{dx} = y \ln(x)?
    Answer: y=Ce12(ln⁡x)2y = C e^{\frac{1}{2}(\ln x)^2} Separate the variables: 1ydy=ln⁡(x)xdx\frac{1}{y}dy = \frac{\ln(x)}{x}dx. Integrate both sides. For the right side, use u-substitution with u=ln⁡(x)u = \ln(x), so du=1xdxdu = \frac{1}{x}dx. The integral becomes ∫1ydy=∫udu\int \frac{1}{y}dy = \int u du. This gives ln⁡∣y∣=12u2+K=12(ln⁡x)2+K\ln|y| = \frac{1}{2}u^2 + K = \frac{1}{2}(\ln x)^2 + K. To solve for y, exponentiate both sides: ∣y∣=e12(ln⁡x)2+K=eKe12(ln⁡x)2|y| = e^{\frac{1}{2}(\ln x)^2 + K} = e^K e^{\frac{1}{2}(\ln x)^2}. Let C=±eKC = \pm e^K. The solution is y=Ce12(ln⁡x)2y = C e^{\frac{1}{2}(\ln x)^2}.
  8. Find the general solution to y′=(y+1)2y' = (y+1)^2.
    Answer: y=1C−x−1y = \frac{1}{C-x} - 1 When you encounter a differential equation like y′=(y+1)2y' = (y+1)^2, you're looking at a separable differential equation. The key is to separate the variables so that all terms involving yy are on one side and all terms involving xx are on the other. Starting with dydx=(y+1)2\frac{dy}{dx} = (y+1)^2, you can rewrite this as dy(y+1)2=dx\frac{dy}{(y+1)^2} = dx. Now integrate both sides. The left side requires the substitution u=y+1u = y+1, giving us ∫(y+1)−2dy=∫dx\int (y+1)^{-2} dy = \int dx, which becomes −1y+1=x+C1-\frac{1}{y+1} = x + C_1. Solving for yy, multiply both sides by −1-1: 1y+1=−x−C1\frac{1}{y+1} = -x - C_1. Let C=−C1C = -C_1 to simplify: 1y+1=C−x\frac{1}{y+1} = C - x. Therefore, y+1=1C−xy+1 = \frac{1}{C-x}, and finally y=1C−x−1y = \frac{1}{C-x} - 1. This matches answer choice D. Answer A represents the solution to y′=1+y2y' = 1 + y^2, not (y+1)2(y+1)^2. Answer B incorrectly suggests taking the natural logarithm of the right side, which isn't the proper integration technique for this separable equation. Answer C has the wrong exponent - it would result from integrating incorrectly or confusing the separation step. Remember: for separable equations of the form y′=f(y)y' = f(y), always separate variables first, then integrate. Watch out for the negative sign when integrating 1(y+1)2\frac{1}{(y+1)^2} - it's a common source of errors.
  9. The general solution to the differential equation y′=yxln⁡xy' = \frac{y}{x \ln x} can be written in the form y=f(x)y = f(x). What is f(x)f(x)?
    Answer: f(x)=Aln⁡(x)f(x) = A \ln(x) First, write the equation as dydx=yxln⁡x\frac{dy}{dx} = \frac{y}{x \ln x} and separate the variables: 1ydy=1xln⁡xdx\frac{1}{y} dy = \frac{1}{x \ln x} dx. Next, integrate both sides: ∫1ydy=∫1xln⁡xdx\int \frac{1}{y} dy = \int \frac{1}{x \ln x} dx. The left integral is ln⁡∣y∣\ln|y|. For the right integral, use u-substitution with u=ln⁡xu = \ln x, so du=1xdxdu = \frac{1}{x} dx. The integral becomes ∫1udu=ln⁡∣u∣=ln⁡∣ln⁡x∣\int \frac{1}{u} du = \ln|u| = \ln|\ln x|. So, we have ln⁡∣y∣=ln⁡∣ln⁡x∣+C\ln|y| = \ln|\ln x| + C. To solve for yy, exponentiate both sides: ∣y∣=eln⁡∣ln⁡x∣+C=eln⁡∣ln⁡x∣⋅eC=∣ln⁡x∣⋅eC|y| = e^{\ln|\ln x| + C} = e^{\ln|\ln x|} \cdot e^C = |\ln x| \cdot e^C. Let A=±eCA = \pm e^C. Then y=Aln⁡(x)y = A \ln(x).
  10. The general solution to the differential equation dydx=2x+12y\frac{dy}{dx} = \frac{2x+1}{2y} is a family of curves. Which equation best describes this family?
    Answer: y2=x2+x+Cy^2 = x^2 + x + C Separate the variables: 2y dy=(2x+1) dx2y\,dy = (2x+1)\,dx. Integrate both sides: ∫2y dy=∫(2x+1) dx\int 2y\,dy = \int (2x+1)\,dx. This gives y2=x2+x+Cy^2 = x^2 + x + C. This is the implicit form of the solution. Distractor A incorrectly places the constant outside the square root. Distractor C has an error in the integration of 2y. Distractor D incorrectly takes the square root of the terms individually.
  11. The rate of change of a quantity yy with respect to xx is given by dydx=xyx2+1\frac{dy}{dx} = \frac{xy}{x^2+1}. Find the general solution for yy.
    Answer: y=Cx2+1y = C\sqrt{x^2+1} Separate the variables: 1ydy=xx2+1dx\frac{1}{y}dy = \frac{x}{x^2+1}dx. Integrate both sides. For the right side, use u-substitution with u=x2+1u=x^2+1, so du=2x dxdu=2x\,dx and x dx=du/2x\,dx = du/2. The integral becomes ∫1ydy=∫1udu2\int \frac{1}{y}dy = \int \frac{1}{u} \frac{du}{2}. This gives ln⁡∣y∣=12ln⁡∣u∣+K=12ln⁡(x2+1)+K\ln|y| = \frac{1}{2}\ln|u| + K = \frac{1}{2}\ln(x^2+1) + K. Using log properties, ln⁡∣y∣=ln⁡((x2+1)1/2)+K=ln⁡(x2+1)+K\ln|y| = \ln((x^2+1)^{1/2}) + K = \ln(\sqrt{x^2+1}) + K. Exponentiating gives ∣y∣=eKeln⁡(x2+1)=eKx2+1|y| = e^K e^{\ln(\sqrt{x^2+1})} = e^K \sqrt{x^2+1}. Let C=±eKC = \pm e^K, so y=Cx2+1y = C\sqrt{x^2+1}.
  12. The general solution to the differential equation dydx=−4x(y−1)\frac{dy}{dx} = -4x(y-1) is of the form y=1+f(x,C)y = 1 + f(x, C). What is f(x,C)f(x, C)?
    Answer: Ce−2x2Ce^{-2x^2} When you encounter a differential equation like dydx=−4x(y−1)\frac{dy}{dx} = -4x(y-1), recognize this as a separable differential equation. The key insight is that you can separate variables by moving all terms involving yy to one side and all terms involving xx to the other. Starting with dydx=−4x(y−1)\frac{dy}{dx} = -4x(y-1), separate variables: dyy−1=−4x dx\frac{dy}{y-1} = -4x \, dx Now integrate both sides. The left side gives ln⁡∣y−1∣\ln|y-1|, and the right side gives −2x2+C1-2x^2 + C_1. So: ln⁡∣y−1∣=−2x2+C1\ln|y-1| = -2x^2 + C_1 Exponentiating both sides: ∣y−1∣=e−2x2+C1=eC1⋅e−2x2|y-1| = e^{-2x^2 + C_1} = e^{C_1} \cdot e^{-2x^2} Since eC1e^{C_1} is just another constant, call it CC: y−1=Ce−2x2y-1 = Ce^{-2x^2} Therefore: y=1+Ce−2x2y = 1 + Ce^{-2x^2} This matches the form y=1+f(x,C)y = 1 + f(x,C) where f(x,C)=Ce−2x2f(x,C) = Ce^{-2x^2}, which is choice D. Choice A incorrectly includes (y−1)(y-1) in the function ff, but ff should only depend on xx and CC. Choice B has the wrong exponent—it uses −4x-4x instead of −2x2-2x^2, missing the integration of xx. Choice C adds CC to the exponential instead of multiplying by it, which doesn't arise from the integration process. Study tip: For separable differential equations, always check your integration carefully—especially when integrating polynomials like xx, where ∫−4x dx=−2x2\int -4x \, dx = -2x^2, not −4x-4x.
  13. Find the general solution for y(x)y(x) given that y′=x1−y2y' = x\sqrt{1-y^2}.
    Answer: y(x)=sin⁡(x22+C)y(x) = \sin(\frac{x^2}{2} + C) Separate the variables: 11−y2dy=x dx\frac{1}{\sqrt{1-y^2}}dy = x\,dx. Integrate both sides: ∫11−y2dy=∫x dx\int \frac{1}{\sqrt{1-y^2}}dy = \int x\,dx. The left integral is arcsin⁡(y)\arcsin(y) and the right is x22+C\frac{x^2}{2} + C. So, arcsin⁡(y)=x22+C\arcsin(y) = \frac{x^2}{2} + C. To solve for yy, take the sine of both sides: y=sin⁡(x22+C)y = \sin(\frac{x^2}{2} + C). Distractor A incorrectly adds C after applying the sine function. Distractors B and D use incorrect antiderivatives.
  14. Find the general solution to the differential equation (1+x2)dy−2xydx=0(1+x^2) dy - 2xy dx = 0.
    Answer: y=A(1+x2)y = A(1+x^2) First, rearrange the equation to prepare for separation: (1+x2)dy=2xydx(1+x^2) dy = 2xy dx. Now, separate the variables by moving yy terms to the left and xx terms to the right: 1ydy=2x1+x2dx\frac{1}{y} dy = \frac{2x}{1+x^2} dx. Integrate both sides: ∫1ydy=∫2x1+x2dx\int \frac{1}{y} dy = \int \frac{2x}{1+x^2} dx. The left integral is ln⁡∣y∣\ln|y|. For the right integral, use u-substitution with u=1+x2u = 1+x^2, so du=2xdxdu = 2x dx. The integral becomes ∫1udu=ln⁡∣u∣=ln⁡(1+x2)\int \frac{1}{u} du = \ln|u| = \ln(1+x^2) (absolute value is not needed since 1+x2>01+x^2 > 0). So, ln⁡∣y∣=ln⁡(1+x2)+C\ln|y| = \ln(1+x^2) + C. Exponentiate both sides: ∣y∣=eln⁡(1+x2)+C=eln⁡(1+x2)eC=(1+x2)eC|y| = e^{\ln(1+x^2)+C} = e^{\ln(1+x^2)}e^C = (1+x^2)e^C. Let A=±eCA = \pm e^C. The solution is y=A(1+x2)y = A(1+x^2). Distractor A represents the common error of treating ea+be^{a+b} as ea+ebe^a+e^b. Distractor C results from incorrectly integrating 2x1+x2\frac{2x}{1+x^2} as if it were 11+x2\frac{1}{1+x^2}.
  15. Find the general solution to the differential equation dydx=xy+3x−2y−6\frac{dy}{dx} = xy + 3x - 2y - 6.
    Answer: y=Ce12x2−2x−3y = Ce^{\frac{1}{2}x^2 - 2x} - 3 The right side of the equation can be factored by grouping: xy+3x−2y−6=x(y+3)−2(y+3)=(x−2)(y+3)xy + 3x - 2y - 6 = x(y+3) - 2(y+3) = (x-2)(y+3). The equation becomes dydx=(x−2)(y+3)\frac{dy}{dx} = (x-2)(y+3). Separating variables gives 1y+3dy=(x−2)dx\frac{1}{y+3}dy = (x-2)dx. Integrating both sides yields ln⁡∣y+3∣=12x2−2x+K\ln|y+3| = \frac{1}{2}x^2 - 2x + K. Exponentiating both sides gives ∣y+3∣=e12x2−2x+K=eKe12x2−2x|y+3| = e^{\frac{1}{2}x^2 - 2x + K} = e^K e^{\frac{1}{2}x^2 - 2x}. Let C=±eKC = \pm e^K. Then y+3=Ce12x2−2xy+3 = Ce^{\frac{1}{2}x^2 - 2x}, so y=Ce12x2−2x−3y = Ce^{\frac{1}{2}x^2 - 2x} - 3.
  16. Find the general solution, in implicit form, to the differential equation xydydx=y+1xy \frac{dy}{dx} = y+1.
    Answer: y−ln⁡∣y+1∣=ln⁡∣x∣+Cy - \ln|y+1| = \ln|x| + C To separate the variables, move all yy terms to the left and all xx terms to the right: yy+1dy=1xdx\frac{y}{y+1} dy = \frac{1}{x} dx. To integrate the left side, ∫yy+1dy\int \frac{y}{y+1} dy, we can rewrite the integrand as y+1−1y+1=1−1y+1\frac{y+1-1}{y+1} = 1 - \frac{1}{y+1}. Now integrate both sides: ∫(1−1y+1)dy=∫1xdx\int (1 - \frac{1}{y+1}) dy = \int \frac{1}{x} dx. This yields y−ln⁡∣y+1∣=ln⁡∣x∣+Cy - \ln|y+1| = \ln|x| + C. This is the implicit general solution. Distractor B has a sign error in the integration of the yy term. Distractor C results from an incorrect attempt to integrate yy+1\frac{y}{y+1}. Distractor D uses the wrong antiderivative for 1x\frac{1}{x}.
  17. Find the general solution to the differential equation y′=y+exyy' = y + e^x y.
    Answer: y=Cex+exy = C e^{x+e^x} First, factor the right side: y′=y(1+ex)y' = y(1+e^x). Separate the variables: 1ydy=(1+ex)dx\frac{1}{y}dy = (1+e^x)dx. Integrate both sides: ∫1ydy=∫(1+ex)dx\int \frac{1}{y}dy = \int (1+e^x)dx. This gives ln⁡∣y∣=x+ex+K\ln|y| = x + e^x + K. Exponentiate both sides: ∣y∣=ex+ex+K=eKex+ex|y| = e^{x+e^x+K} = e^K e^{x+e^x}. Let C=±eKC = \pm e^K. The general solution is y=Cex+exy = C e^{x+e^x}.
  18. Determine the general solution of the differential equation dydx−x2y=0\frac{dy}{dx} - x^2y = 0.
    Answer: y=Cex3/3y = C e^{x^3/3} First, rearrange the equation to dydx=x2y\frac{dy}{dx} = x^2y. Separate the variables: 1ydy=x2dx\frac{1}{y}dy = x^2 dx. Integrate both sides: ∫1ydy=∫x2dx\int \frac{1}{y}dy = \int x^2 dx, which results in ln⁡∣y∣=x33+K\ln|y| = \frac{x^3}{3} + K. Exponentiating both sides gives ∣y∣=ex3/3+K=eKex3/3|y| = e^{x^3/3 + K} = e^K e^{x^3/3}. Let C=±eKC = \pm e^K. The general solution is y=Cex3/3y = C e^{x^3/3}.
  19. The general solution of dydx=1y⋅xln⁡x\frac{dy}{dx} = \frac{1}{y \cdot x \ln x} is y2=f(x,C)y^2 = f(x, C). What is f(x,C)f(x, C)?
    Answer: 2ln⁡∣ln⁡x∣+C2\ln|\ln x| + C Separate the variables: y dy=1xln⁡xdxy\,dy = \frac{1}{x \ln x}dx. Integrate both sides. The left side is y22\frac{y^2}{2}. For the right side, use u-substitution with u=ln⁡xu = \ln x, so du=1xdxdu = \frac{1}{x}dx. The integral is ∫1udu=ln⁡∣u∣=ln⁡∣ln⁡x∣\int \frac{1}{u}du = \ln|u| = \ln|\ln x|. So, we have y22=ln⁡∣ln⁡x∣+K\frac{y^2}{2} = \ln|\ln x| + K. Multiply by 2: y2=2ln⁡∣ln⁡x∣+2Ky^2 = 2\ln|\ln x| + 2K. Let C=2KC = 2K. Thus, y2=2ln⁡∣ln⁡x∣+Cy^2 = 2\ln|\ln x| + C.
  20. Which expression represents the general solution to the differential equation dydx=cot⁡(y)cot⁡(x)\frac{dy}{dx} = \frac{\cot(y)}{\cot(x)}?
    Answer: sec⁡(y)=Csec⁡(x)\sec(y) = C\sec(x) The equation can be written as dydx=cot⁡(y)tan⁡(x)\frac{dy}{dx} = \cot(y)\tan(x). Separating variables gives 1cot⁡(y)dy=tan⁡(x)dx\frac{1}{\cot(y)}dy = \tan(x)dx, which is tan⁡(y)dy=tan⁡(x)dx\tan(y)dy = \tan(x)dx. Integrating both sides: ∫tan⁡(y)dy=∫tan⁡(x)dx\int \tan(y)dy = \int \tan(x)dx. This yields ln⁡∣sec⁡(y)∣=ln⁡∣sec⁡(x)∣+K\ln|\sec(y)| = \ln|\sec(x)| + K. Exponentiate both sides: eln⁡∣sec⁡(y)∣=eln⁡∣sec⁡(x)∣+Ke^{\ln|\sec(y)|} = e^{\ln|\sec(x)| + K}, which simplifies to ∣sec⁡(y)∣=eK∣sec⁡(x)∣|\sec(y)| = e^K|\sec(x)|. Let C=±eKC = \pm e^K. This gives sec⁡(y)=Csec⁡(x)\sec(y) = C\sec(x).

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