Integrating the rational fractions

In summary, the sphere is moved slowly from the vertical position until the string makes angle θ with the vertical.
  • #1
MadPhysics08
16
0
please... i need a help in integrating the partial fractions
i can't proceed to the integration part if i don't understand the patter in finding the constant...
that is...

if the given is:

ʃ ( (x^5+1) / ((x^3)(x+1)) )dx

then;

ʃ ( x-2 + ( 4x^3+1 ) / ( x^4 + 2x^3) )
ʃ ( x-2 + ( 4x^3 + 1 ) / ( x^3 (x + 2 ) )
ʃ ( x-2 + A/x + B/x^2 + C/x^3 + D/x+2)

Ax^2(x+2) + Bx(x+2) + C(x+2) + D(x^3) = 4x^3 + 1 ----- i don't know what going on
in this part
 
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  • #2
MadPhysics08 said:
if the given is:

ʃ ( (x^5+1) / ((x^3)(x+1)) )dx

then;

ʃ ( x-2 + ( 4x^3+1 ) / ( x^4 + 2x^3) )
ʃ ( x-2 + ( 4x^3 + 1 ) / ( x^3 (x + 2 ) )
ʃ ( x-2 + A/x + B/x^2 + C/x^3 + D/x+2)

Ax^2(x+2) + Bx(x+2) + C(x+2) + D(x^3) = 4x^3 + 1 ----- i don't know what going on
in this part

Hi MadPhysics08;! :smile:

(I assume you mean ʃ ( (x^5+1) / ((x^3)(x+2)) )dx)

Ax^2(x+2) + Bx(x+2) + C(x+2) + D(x^3) = 4x^3 + 1

is simply the previous two lines (except for both the x - 2 s), multiplied by x^3(x + 2)

A B C and D are unknowns, and you find them by solving that equation :smile:

(though I think you can find D using the usual substitution method :wink:)
 
  • #3
Prove that F=mgtanθ

Can everyone help me to solve this problem...

A small sphere of mass hangs from a string of L as in below. A variable horizontal force F is
applied to the sphere in such a way that it moves slowly from the vertical position until the string makes angle θ with the vertical. Assuming the sphere is always in equilibrium

1. show that F=mgtanθ
2.show that work done by F is mgL(1-cosθ)

__________________________
|\......
|..\......
|.θ.\.L......
|...\......
|...\.....
|...0------F...
0...|......
...|......
...|......
...W......
 
  • #4
Prove that F=mgtanθ

Can everyone help me to solve this problem...

A small sphere of mass hangs from a string of L as in below. A variable horizontal force F is
applied to the sphere in such a way that it moves slowly from the vertical position until the string makes angle θ with the vertical. Assuming the sphere is always in equilibrium

1. show that F=mgtanθ
2.show that work done by F is mgL(1-cosθ)

__________________________
|\
| \
| θ \ L
| \
| \
| 0------F
0 |
|
|
W
 
  • #5
MadPhysics08 said:
Can everyone help me to solve this problem...

A small sphere of mass hangs from a string of L as in below. A variable horizontal force F is
applied to the sphere in such a way that it moves slowly from the vertical position until the string makes angle θ with the vertical. Assuming the sphere is always in equilibrium

1. show that F=mgtanθ
2.show that work done by F is mgL(1-cosθ)

Hi MadPhysics08! :smile:

("Can anyone help me to solve this problem..." would be more realistic! :wink:)

"moves slowly" is examiners' code for saying that, at any particular time, the acceleration is so small that you can treat it as zero.

Does that help? :smile:
 
  • #6
so, let d be the displacement W(work)=F*dcosθ
∑F=ma=0 then,
∑F=W+T+F
W+T+F=0
-W*dcosθ + T*dcosθ + F*dcos(θ+90)

[T*dcosθ=0 because they are perpendicular]

W*dcosθ=F*dcos(θ+90)

but cos(θ+90)=sinθ

w*dcosθ=F*dsinθ
F=Wtanθ
F=mgtanθ

is my solution correct?
 
  • #7
thnks tim...

Can i asked one favor...
please... i need a hint for the problem number 2...
 
  • #8
Hi MadPhysics08! :smile:

Let's do part 1 first:
MadPhysics08 said:
w*dcosθ=F*dsinθ
F=Wtanθ
F=mgtanθ

You should say which direction you are taking components in, and why.

Anyway, if w*dcosθ=F*dsinθ, then F = w cotθ. :frown:
so, let d be the displacement W(work)=F*dcosθ
∑F=ma=0 then,
∑F=W+T+F
W+T+F=0
-W*dcosθ + T*dcosθ + F*dcos(θ+90)

[T*dcosθ=0 because they are perpendicular]

Whatever is this supposed to be?? :confused:

Hint: work done = energy gained.

(this is the only reason we bother about work done)
 
  • #9
okay...

There three forces acted on the sphere:
tension(T), applied force F and gravitational force(mg)

so..
W=T*Scosθ=0
the displacement of the sphere along the arc length is perpendicular to the tension
While..
W=-mg*d cos(θ+90)=-mg*dsinθ (trigonometric identity of cos(θ+90)=sinθ)
because the angle between the displacement of the sphere is more than 90 degrees..
thus...work done by weight is negative
however..the displacement of the sphere started from the vertical position to the slanting position until the two position made an angle θ
and,
W=F*dcosθ (angle between F and d is θ)
so...
equate W to W:
F*dcosθ= -mg*dsinθ (cancel d)
F*cosθ=-mg*sinθ
F=-mgtanθ--------this is my problem...i just end up with negative sign...
 
  • #10
work done by gravitational force(W=-mgcos(θ+90)) is negative because it opposed the direction of W=F*dcosθ
 
  • #11
Hi MadPhysics08! :smile:

I'm sorry, I can't follow any of this …

you seem to be using work done to find the value of F. :confused:

1. to find F, just take components perpendicular to the unknown force, whch is … ? :smile:

2. to find the work done, either:

i] integrate the force "dot" the displacement (which works, but is really complicated :frown:), or:

ii] just use the work-energy theorem: work done equals energy gained …

so what is the energy gained? :smile:
 

1. What does it mean to integrate rational fractions?

Integrating rational fractions means finding the antiderivative of a rational function, which is a function that can be expressed as a ratio of two polynomials. This process allows us to find the original function that was differentiated to obtain the rational fraction.

2. Why is integrating rational fractions important?

Integrating rational fractions is important because it allows us to find the area under a curve, which has many real-world applications. It also helps in solving differential equations, which are used to model various physical phenomena.

3. What are the steps involved in integrating rational fractions?

The general steps for integrating rational fractions are: 1) Simplify the fraction by factoring out common terms and reducing the fraction to lowest terms, 2) Decompose the fraction into partial fractions, 3) Integrate each partial fraction separately, and 4) Combine the individual integrals to get the final answer.

4. Are there any special cases to consider when integrating rational fractions?

Yes, there are a few special cases to consider when integrating rational fractions. These include: 1) Improper rational fractions, where the degree of the numerator is greater than or equal to the degree of the denominator, 2) Non-distinct linear factors, where the denominator has repeated linear factors, and 3) Complex roots, where the denominator has complex roots.

5. What are some common techniques used in integrating rational fractions?

Some common techniques used in integrating rational fractions include: 1) Partial fraction decomposition, 2) Integration by substitution, 3) Integration by parts, and 4) Trigonometric substitutions. The specific technique used will depend on the form of the rational fraction and the availability of appropriate substitutions.

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