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lisabon 2012 [21]
3 years ago
5

Workout to the simplest:

5E%7B3%7D%20%29%20dx" id="TexFormula1" title=" \int \: {x}^{2} ln( {x}^{3} ) dx" alt=" \int \: {x}^{2} ln( {x}^{3} ) dx" align="absmiddle" class="latex-formula">
​
Mathematics
2 answers:
goblinko [34]3 years ago
7 0

Answer:

\rm \displaystyle \ln(x)   { {x}^{3} } -  \frac{ {x}^{3} }{3}    + \rm C

Step-by-step explanation:

we would like to integrate the following integration

\displaystyle \int  {x}^{2}   \ln( {x}^{3} ) dx

before doing so we can use logarithm exponent rule in order to get rid of the exponent of ln(x³)

\displaystyle \int 3 {x}^{2}   \ln( {x}^{} ) dx

now notice that the integrand is in the mutilation of two different functions thus we can use integration by parts given by

\rm\displaystyle \int u  \cdot \: vdx = u \int vdx -  \int u' \bigg( \int vdx \bigg)dx

where u' can be defined by the differentiation of u

first we need to choose our u and v in that case we'll choose u which comes first in the guideline ILATE which full from is Inverse trig, Logarithm, Algebraic expression, Trigonometry, Exponent.

since Logarithms come first our

\displaystyle u =   \ln(x)  \quad  \text{and}  \quad v =   {3x}^{2}

and u' is \frac{1}{x}

altogether substitute:

\rm \displaystyle \ln(x)  \int  3{x}^{2} dx -  \int  \frac{1}{x}  \left( \int 3 {x}^{2} dx \right)dx

use exponent integration rule to integrate exponent:

\rm \displaystyle \ln(x)  \int  3{x}^{2} dx -  \int  \frac{1}{x}  \left( 3\frac{ {x}^{3} }{3}  \right)dx

once again exponent integration rule:

\rm \displaystyle \ln(x)   3\frac{ {x}^{3} }{3}  -  \int  \frac{1}{x}  \left( 3\frac{ {x}^{3} }{3}  \right)dx

simplify integrand:

\rm \displaystyle \ln(x)   3\frac{ {x}^{3} }{3}  -  \int  \frac{ 3{x}^{3} }{3x} dx

use law of exponent to simplify exponent:

\rm \displaystyle \ln(x)   \frac{ 3{x}^{3} }{3}  -  \int  \frac{ 3\cancel{ {x}^{3}} }{3 \cancel{x}} dx

\rm \displaystyle \ln(x)   \frac{ 3{x}^{3} }{3}  -  \int  \frac{ 3{x}^{3} }{3} dx

use constant integration rule to get rid of constant:

\rm \displaystyle \ln(x)   \frac{3 {x}^{3} }{3}  -  1  \int  {x}^{2}dx

use exponent integration rule:

\rm \displaystyle \ln(x)   \frac{3 {x}^{3} }{3}  -   \frac{ {x}^{3} }{3}

\rm \displaystyle \ln(x)   { {x}^{3} } -  \frac{ {x}^{3} }{3}

and finally we of course have to add the constant of integration:

\rm \displaystyle \ln(x)   { {x}^{3} } -  \frac{ {x}^{3} }{3}    + \rm C

and we are done!

Roman55 [17]3 years ago
4 0

Answer:

Step-by-step explanation:

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Yuri [45]

Answer:

B<C

Step-by-step explanation:

-a is the opposite of a. Since a is a negative number, it will become positive and be bigger than b, which is negative.

c is a positive number, so the opposite will be negative and can not be bigger than c.

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you were overcharged $4.52 on your cellphone bill 3 months in a row the cell phone company says that it will add -$4.52 to your
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3 years ago
Solve for c<br><br><br> R=5(c/a-0.3)
aalyn [17]

we have

R=5(c/a-0.3)

Solve for c--------> that means that clear variable c

so

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R/5=(c/a-0.3)

Adds 0.3 both sides

(R/5)+0.3=(c/a)

Multiply by a both sides

a[(R/5)+0.3]=c

so

c=a[(R/5)+0.3]

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<u>the answer is</u>

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6 0
3 years ago
Read 2 more answers
A 15 kilogram object is suspended from the end of a vertically hanging spring stretches the spring 1/3 meters. At time t = 0, th
Yuri [45]

Answer:

15\frac{d^{2}y(t)}{dt^{2} }  - 441.45y(t) = ± 170 cos(5t)

y(0)=0, y'(0)=0

Step-by-step explanation:

See the attached image

This problem involves Newton's 2nd Law which is: ∑F = ma, we have that the acting forces on the mass-spring system are: F_{r} (t) that correspond to the force of resistance on the mass by the action of the spring and F(t) that is an external force with unknown direction (that does not specify in the enounce).

For determinate F_{r} (t) we can use Hooke's Law given by the formula F_{r} (t) = k y(t) where k correspond to the elastic constant of the spring and y(t) correspond to  the relative displacement of the mass-spring system with respect of his rest state.

We know from the problem that an 15 Kg mass stretches the spring 1/3 m so we apply Hooke's law and obtain that...

k = \frac{F_{r}}{y} = \frac{mg}{y} = \frac{15 Kg (9.81 \frac{m}{s^{2} } )}{\frac{1}{3} m}  = 441.45 \frac{N}{m}

Now we apply Newton's 2nd Law and obtaint that...

F_{r} (t) ± F(t) = ma(t)

F_{r} (t) = ky(t) = 441.45y(t)

F(t) = 170 cos(5t)

m = 15 kg

a(t) = \frac{d^{2}y(t)}{dt^{2} }

Finally... 15\frac{d^{2}y(t)}{dt^{2} }  - 441.45y(t) = ± 170 cos(5t)

We know from the problem that there's not initial displacement and initial velocity, so... y(0)=0 and y'(0)=0

Finally the Initial Value Problem that models the situation describe by the problem is

\left \{ 15\frac{d^{2}y(t)}{dt^{2} }  - 441.45y(t) = \frac{+}{} 170 cos(5t) \atop {y(0)=0, y'(0)=0\right.

6 0
2 years ago
What is the circumstance of the circle below in terms of pi?
nikklg [1K]
Circumference of a circle=2pi*r

2*(2.2)*π=4.4π




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3 years ago
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