How do you find the solution to the differential equation #dy/dx=cos(x)/y^2# where #y(π/2)=0#?

Answer 1
You can write: #y^2dy=cos(x)dx# and integrate; #inty^2dy=intcos(x)dx# Which gives you: #y^3/3=sin(x)+c# #y^3=3sin(x)+c# Now we find the value of #c#; #(0)^3=3sin(pi/2)+c# #0=3+c# And #c=-3# your particular solution is then: #y^3=3sin(x)-3#
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Answer 2

To find the solution to the differential equation (\frac{dy}{dx} = \frac{\cos(x)}{y^2}) with the initial condition (y(\frac{\pi}{2}) = 0), follow these steps:

  1. Separate the variables by multiplying both sides by (y^2) and dividing both sides by (\cos(x)), yielding (y^2 dy = \frac{1}{\cos(x)} dx).

  2. Integrate both sides with respect to their respective variables. This gives (\int y^2 dy = \int \sec(x) dx).

  3. Integrate (\int \sec(x) dx) to get (\ln|\sec(x) + \tan(x)| + C_1), where (C_1) is the constant of integration.

  4. Integrate (\int y^2 dy) to get (\frac{1}{3}y^3 + C_2), where (C_2) is the constant of integration.

  5. Combine the constants of integration into one constant, let's call it (C), so the solution becomes (\frac{1}{3}y^3 + \ln|\sec(x) + \tan(x)| = C).

  6. Apply the initial condition (y(\frac{\pi}{2}) = 0) to find the value of the constant (C).

  7. Substitute (x = \frac{\pi}{2}) and (y = 0) into the solution. This gives (0 + \ln|\sec(\frac{\pi}{2}) + \tan(\frac{\pi}{2})| = C), which simplifies to (0 + \ln|1 + \infty| = C).

  8. Since (\tan(\frac{\pi}{2}) = \infty), the absolute value of (\sec(\frac{\pi}{2}) + \tan(\frac{\pi}{2})) is (\infty), so (\ln|1 + \infty| = \infty).

  9. Therefore, the constant (C) is (+\infty).

  10. The solution to the differential equation with the initial condition is (\frac{1}{3}y^3 + \ln|\sec(x) + \tan(x)| = +\infty).

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Answer from HIX Tutor

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

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