Two limited integration questions

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The discussion focuses on the conditions required for two integral equations involving a function f(x). For the first case, the condition is that the primitive function F satisfies F(-a) = -F(a), indicating that f(x) must be an odd function. In the second case, the integral equality holds if f(x) is an even function, as it allows for the cancellation of terms when integrating over symmetric limits. Participants express confusion about applying these conditions in practical scenarios, particularly in physics problems related to electric fields and potentials. Clarification is sought on how to effectively utilize these properties in problem-solving.
hhegab
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Peace!

I want to know the conditions that must be satisfied by a function
f(x) for any of the following two cases to be true (each case independent from the other);

1- \int^a_{-a} f(x) dx = 2 \int^a_0 f(x) dx

2- \int^a_0 f(x) dx = \int^0_a f(x) dx

They gave me confusion when I was solving problems related to electric field and electric potential.
 
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I don't know if this condition is sufficient but a condition would be, if we write the integrals in terms of their primitives,

\int^a_{-a} f(x) dx = 2 \int^a_0 f(x) dx \Leftrightarrow \mathcal{F}(a) - \mathcal{F}(-a) = 2\mathcal{F}(a) \Leftrightarrow \mathcal{F}(-a) = -\mathcal{F}(a)

The condition is that it is true iff the primitive of f is a function F such that F(-a) = -F(a)
 
First case...

\int^a_{-a} f(x) dx = \int^0_{-a} f(x) dx + \int^a_0 f(x) dx

Then use the fact that :

\int^0_{-a} f(x) dx = - \int^{-a}_0 f(x) dx

and replace x by -x...the limit -a will then change to a because of this substitution. and dx will become -dx. Now f(x) becomes f(-x) and there are two possibilities. Either f(-x) = -f(x) or f(-x) = f(x)...you know what you will need to achieve so which one of the two is it...


Question 2 :

Just put the integral in right hand side to the left hand side and use the above property to get rid of the minus-sign...what do you get ?


regards
marlon
 
Can you put like , first case is true if f(x) is even and if such and such...
I shall study your answer. But from my first reading I need more.
I need a condition to apply to f(x) so I can use each of the above properties.

hhegab
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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