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The following equation is in the form$$\frac{dy}{dx}=f(y)$$ Solve the diffrential equation$$\frac{dy}{dx}=2+3y$$

$$\frac{dy}{dx}=2+3y$$ $$dy=(2+3y)dx$$ $$\frac{dy}{2+3y}=dx$$

then I integrated bothsides.. $$\int\frac{dy}{2+3y}=\int{dx}$$

and this is what I think you should get but the book says otherwise... $$\frac{1}{3}ln(2+3y)+c = x+c$$

I know I'm wrong about this but why is there no constant when we integrate the RHS? I'm assuming there's a 1 in front of the $dx$ and when you integrate you get $x+c$

If someone could explain why I'd be grateful.

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    $\begingroup$ You can put a constant $C_1$ on the left, and a constant $C_2$ on the right. But these can be combined into a single constant $C$ either on the left or the right. Note that it is not right to do as you did and use the same constant symbol on the left and right, for then you get cancellation. $\endgroup$ Jul 9, 2015 at 18:46
  • $\begingroup$ use $c1 , c2 $ , combine them to make a single $c3$. $\endgroup$
    – Narasimham
    Jul 9, 2015 at 19:19

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The two sides can take different constants, say $c_1$ and $c_2$. But then you can move both constants to one side and call $c = c_1 - c_2$, which also can take any value.

The lesson here is that $c_1$ and $c_2$ can be same or different, in contrary to what your form says.

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Formally speaking, this solution should be $$\frac{1}{3}\ln(2+3y)+c_1=x+c_2.$$ But we can also write this $$\frac{1}{3}\ln(2+3y)=x+c_2-c_1.$$ But we can define a new constant $c=c_2-c_1$, and write this $$\frac{1}{3}\ln(2+3y)=x+c.$$ Usually, we skip all the middle steps and jump straight to the end.

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