verify that the inverse of at is (a- 1 )r. hint: use the multiplication rule for tranposes, (cd)r = d7cr.

The exact length of the curve is e⁵ - 1 + 45 or approximately 152.9 units.

To find the length of the curve, we will need to use the formula for arc length:
L = ∫√(dx/dt)² + (dy/dt)² dt

First, let's find the derivatives of x and y with respect to t:
dx/dt = e^t - 9
dy/dt = 6e^(t/2)

Now we can plug these into the formula for arc length and integrate over the interval 0 to 5:
L = ∫0^5 √(e^t - 9)² + (6e^(t/2))² dt

This integral is a bit tricky to evaluate, so we'll simplify it using some algebraic manipulations:
L = ∫0^5 √(e^(2t) - 18e^t + 81 + 36e^t) dt
L = ∫0^5 √(e^(2t) + 18e^t + 81) dt
L = ∫0^5 (e^t + 9) dt
L = e^5 - e^0 + 45

So the exact length of the curve is e^5 - 1 + 45, or approximately 152.9 units.

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A population has SS = 100 and σ2 = 4. What is the value of sum E (X-µ) for the population is A) 0.

Based on the information provided, we are given that a population has SS (sum of squared deviations) = 100 and σ² (population variance) = 4. We are asked to find the value of the sum of E(X-µ) for the population, where E is the expectation operator, X is the random variable representing individual values, and µ is the population mean.

The sum of E(X-µ) for a population is always equal to 0. This is due to the fact that the deviations from the mean, both positive and negative, will cancel each other out when summed up. In mathematical terms:

Σ(X-µ) = 0

This is a fundamental property of the population mean, as it represents the "center" of the distribution of values.

It's worth noting that the given values for SS and σ² aren't directly related to solving this particular question, as they provide information about the dispersion of the data rather than the sum of the deviations from the mean. However, these values can be useful when analyzing other aspects of the population, such as calculating the standard deviation (σ = √σ²). Therefore, the correct option is A.

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Using Green's Theorem: ∫_' [tex]y^2[/tex] dx =[tex]r^4[/tex]/6

Let's first find the parametrization of the semicircle ' in the upper half-plane from r to -r.

We can use the parameterization r(t) = r(cos(t), sin(t)) for a circle centered at the origin with radius r, where t varies from 0 to pi.

To restrict to the upper half-plane, we can choose t to vary from 0 to pi/2. Thus, a possible parametrization for ' is given by:

r(t) = r(cos(t), sin(t)), where t ∈ [0, pi/2]

Now, we can evaluate the line integral directly:

∫_' [tex]y^2[/tex] dx = ∫_0^(pi/2) (r sin[tex](t))^2[/tex] (-r sin(t)) dt

= -[tex]r^4[/tex] ∫_[tex]0^[/tex]([tex]\pi[/tex]/2) [tex]sin^3[/tex](t) dt

= -[tex]r^4[/tex] (2/3)

To use Green's Theorem, we need to find a vector field F = (P, Q) such that F · dr = y^2 dx on '.

One possible choice is F(x, y) = (-[tex]y^3[/tex]/3, xy), for which we have:

∫_' F · dr = ∫_[tex]0^(\pi[/tex]/2) F(r(t)) · r'(t) dt

= ∫_[tex]0^(\pi[/tex]/2) (-[tex]r(t)^3[/tex]/3, r(t)^2 sin(t) cos(t)) · (-r sin(t), r cos(t)) dt

= ∫_[tex]0^(\pi/2) r^4[/tex]/3 [tex]sin^4[/tex](t) + [tex]r^4[/tex]/3 [tex]cos^2[/tex](t) [tex]sin^2[/tex](t) dt

= [tex]r^4[/tex]/3 ∫_[tex]0^(pi/2)[/tex][tex]sin^2[/tex](t) ([tex]sin^2[/tex](t) + [tex]cos^2[/tex](t)) dt

= [tex]r^4[/tex]/3 ∫_[tex]0^(\pi/2[/tex]) [tex]sin^2[/tex](t) dt

= [tex]r^4[/tex]/6

Thus, we have:

∫_' [tex]y^2[/tex] dx = ∫_' F · dr = [tex]r^4[/tex]/6

Therefore, the two methods give us the following results:

   Direct evaluation: ∫_'[tex]y^2[/tex]dx = -[tex]r^4[/tex] (2/3)

   Using Green's Theorem: ∫_' [tex]y^2[/tex] dx = [tex]r^4[/tex]/6

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We get the same result as before, J'y y dx = 0, using Green's Theorem.

To evaluate J'y y dx directly, we need to parameterize the curve ' and substitute the appropriate variables.

Let's parameterize the curve ' by using polar coordinates. The curve ' is a semicircle in the upper half-plane from r to -r, so we can use the parameterization:

x = r cos(t), y = r sin(t), where t ranges from 0 to π.

Then, we have y = r sin(t) and dy = r cos(t) dt. Substituting these variables into the expression for J'y y dx, we get:

J'y y dx = ∫' y^2 dx = ∫t=0^π (r sin(t))^2 (r cos(t)) dt

= r^3 ∫t=0^π sin^2(t) cos(t) dt.

To evaluate this integral, we can use the identity sin^2(t) = (1 - cos(2t))/2, which gives:

J'y y dx = r^3 ∫t=0^π (1/2 - cos(2t)/2) cos(t) dt

= (r^3/2) ∫t=0^π cos(t) dt - (r^3/2) ∫t=0^π cos(2t) cos(t) dt.

Evaluating these integrals gives:

J'y y dx = (r^3/2) sin(π) - (r^3/4) sin(2π)

= 0.

Now, let's use Green's Theorem to evaluate J'y y dx. Green's Theorem states that for a simple closed curve C in the plane and a vector field F = (P, Q), we have:

∫C P dx + Q dy = ∬R (Qx - Py) dA,

where R is the region enclosed by C, and dx and dy are the differentials of x and y, respectively.

To apply Green's Theorem, we need to choose an appropriate vector field F. Since we are integrating y times dx, it's natural to choose F = (0, xy). Then, we have:

Py = x, Qx = 0, and Qy - Px = -x.

Substituting these values into the formula for Green's Theorem, we get:

∫' y dx = ∬R (-x) dA.

To evaluate this double integral, we can use polar coordinates again. Since the curve ' is a semicircle in the upper half-plane, the region R enclosed by ' is the upper half-disc of radius r. Using polar coordinates, we have:

x = r cos(t), y = r sin(t), where r ranges from 0 to r and t ranges from 0 to π.

Then, we have:

∬R (-x) dA = ∫r=0^r ∫t=0^π (-r cos(t)) r dt dθ

= -r^2 ∫t=0^π cos(t) dt ∫θ=0^2π dθ

= 0.

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Answer:

[tex]s^2Y(s)+38Y(s)=g(s)[/tex]

Step-by-step explanation:

Given the second order differential equation with initial condition.

[tex]y''+36y=g(t); \ y(0)=0, \ y'(0)=0, \ and \ y''(0)=1[/tex]

Take the Laplace transform of each side of the equation.

~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

[tex]\boxed{\left\begin{array}{ccc}\text{\underline{Laplace Transforms of DE's:}}\\\\L\{y''\}=s^2Y(s)-sy(0)-y'(0)\\\\\ L\{y'\}=sY(s)-y(0) \\\\ L\{y\}=Y(s)\end{array}\right}[/tex]

Taking the Laplace transform of the DE.

[tex]y''+36y=g(t); \ y(0)=0, \ y'(0)=0, \ and \ y''(0)=1\\\\\Longrightarrow L\{y''\}+38L\{y\}=L\{g(t)\}\\\\\Longrightarrow s^2Y(s)-s(0)-0+38Y(s)=g(s)\\\\\Longrightarrow \boxed{\boxed{s^2Y(s)+38Y(s)=g(s)}}[/tex]

Thus, the Laplace transform has been applied.

The flux of the vector field f(x, y) = ⟨x - y, y - x⟩ along the square bounded by x = 0, x = 1, y = 0, and y = 1 is given by the double integral ∫[0,1]∫[0,1] (x - y) dx dy. Evaluating this integral will provide the final answer for the flux.

To calculate the flux, we need to evaluate the surface integral of the dot product between the vector field f(x, y) and the outward-pointing unit normal vector on the surface. In this case, the surface is the square bounded by x = 0, x = 1, y = 0, and y = 1.

We can parameterize the surface as r(x, y) = ⟨x, y⟩, where 0 ≤ x ≤ 1 and 0 ≤ y ≤ 1. The outward-pointing unit normal vector is given by n = ⟨0, 0, 1⟩.

The dot product between f(x, y) and n is (x - y) × 0 + (y - x) × 0 + (x - y) × 1 = x - y.

Next, we compute the surface integral over the square by integrating x - y with respect to x and y. The limits of integration are 0 to 1 for both x and y.

∫∫(x - y) dA = ∫[0,1]∫[0,1] (x - y) dx dy.

Evaluating this double integral will give us the flux of the vector field along the square bounded by x = 0, x = 1, y = 0, and y = 1.

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The area of the parallelogram for the given vertices is equal to √110 square units.

To find the area of a parallelogram with vertices A(-1, 2, 4), B(0, 4, 8), C(1, 1, 5), and D(2, 3, 9),

we can use the cross product of two vectors formed by the sides of the parallelogram.

Let us define vectors AB and AC as follows,

AB

= B - A

= (0, 4, 8) - (-1, 2, 4)

= (1, 2, 4)

AC

= C - A

= (1, 1, 5) - (-1, 2, 4)

= (2, -1, 1)

Now, let us calculate the cross product of AB and AC.

AB × AC = (1, 2, 4) × (2, -1, 1)

To compute the cross product, we can use the determinant of a 3x3 matrix.

AB × AC

= (2× 4 - (-1) × 1, -(1 × 4 - 2 × 1), 1 × (-1) - 2 × 2)

= (9, 2, -5)

The magnitude of the cross product gives us the area of the parallelogram.

Let us calculate the magnitude,

|AB × AC|

= √(9² + 2² + (-5)²)

= √(81 + 4 + 25)

= √110

Therefore, the area of the parallelogram with vertices A(-1, 2, 4), B(0, 4, 8), C(1, 1, 5), and D(2, 3, 9) is √110 square units.

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The value of the triple integral (x,y, z) = x²y²z² in spherical coordinates over the bottom half of the sphere of radius 11 is π/12.

To evaluate this triple integral in spherical coordinates, we need to express the integrand in terms of spherical coordinates and determine the limits of integration.

We have:

f(x, y, z) = x² y² z²

In spherical coordinates, we have:

x = ρ sin φ cos θ

y = ρ sin φ sin θ

z = ρ cos φ

Also, for the bottom half of the sphere of radius 11 centered at the origin, we have:

0 ≤ ρ ≤ 11

0 ≤ φ ≤ π/2

0 ≤ θ ≤ 2π

Therefore, we can express the triple integral as:

∫∫∫ f(x, y, z) dV = ∫∫∫ ρ⁵ sin³ φ cos² φ dρ dφ dθ

Using the limits of integration given above, we have:

∫∫∫ f(x, y, z) dV = ∫₀²π ∫₀^(π/2) ∫₀¹¹ ρ⁵ sin³ φ cos² φ dρ dφ dθ

Evaluating the integral with respect to ρ first, we get:

∫∫∫ f(x, y, z) dV = ∫₀²π ∫₀^(π/2) [1/6 ρ⁶ sin³ φ cos²φ] from ρ=0 to ρ=11 dφ dθ

Simplifying the integral, we have:

∫∫∫ f(x, y, z) dV = 1/6 ∫₀²π ∫₀^(π/2) 11⁶ sin³ φ cos² φ dφ dθ

Using trigonometric identities, we can further simplify the integral as:

∫∫∫ f(x, y, z) dV = 1/6 ∫₀²π [cos² φ sin⁴ φ] from φ=0 to φ=π/2 dθ

Evaluating the integral, we get:

∫∫∫ f(x, y, z) dV = 1/6 ∫₀²π 1/4 dθ = π/12

Therefore, the value of the triple integral is π/12.
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This series converges to y(t) = t for -5 < t < 5.

To find the Fourier series of the function y(t) = t for -5 < t < 5, we can use the following formula:

c_n = (1/T) ∫(T/2)_(−T/2) y(t) e^(-jnω_0 t) dt

where T is the period of the function, ω_0 = 2π/T is the fundamental frequency, and n is an integer.

In this case, T = 10 and ω_0 = π. Thus, we have:

c_n = (1/10) ∫(-5)^(5) t e^(-jπnt/5) dt

Evaluating this integral using integration by parts, we get:

c_n = (1/π^2n^2)(-1)^n [2e^(jπn) - 2]

Therefore, the Fourier series of y(t) = t is:

y(t) = a_0 + ∑_(n=1)^∞ (c_n e^(jnω_0 t) + c_{-n} e^(-jnω_0 t))

where a_0 = c_0 = 0, and

c_n = (1/π^2n^2)(-1)^n [2e^(jπn) - 2], c_{-n} = (1/π^2n^2)(-1)^n [2e^(-jπn) - 2]

Therefore, the Fourier series of y(t) = t is:

y(t) = ∑_(n=1)^∞ [(1/π^2n^2)(-1)^n [2e^(jπn) - 2] e^(jnπt/5) + (1/π^2n^2)(-1)^n [2e^(-jπn) - 2] e^(-jnπt/5)].

This series converges to y(t) = t for -5 < t < 5.

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The relative frequency of male students who carpool is 0.4314 or 43.14%. There are 44 male students in carpool and the total number of students is 102.

The relative frequency is calculated as:

Relative frequency = (Number of males who carpool) / (Total number of students)

= 44 / 102

= 0.4314 (rounded to four decimal places)

Therefore, the answer is option (4) 0.088 (rounded to three decimal places).

This means that 43.14% of all students are male carpoolers. Relative frequency is a statistic used to measure the proportion of a particular value concerning the total values. It is calculated as the ratio of the number of times a value occurs to the total number of values. In the context of this question, we are asked to calculate the relative frequency of male students who carpool.

This information can be helpful in understanding the transportation habits of students and could be used to inform decisions about transportation policies. In conclusion, the relative frequency of male students who carpool is 0.4314 or 43.14%. The calculation was done by dividing the number of males who carpool by the total number of students.

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The solution to the system of equations is (x, y) = (-38, -49). The solution (-38, -49) satisfies both equations.

The solution to the given system of equations is (x, y) = (-38, -49). In the first equation, -5x + 8y = -36, by isolating x, we get x = (-8y + 36)/5. Substituting this value of x into the second equation, we have (-5((-8y + 36)/5)) + 7y = 6. Simplifying further, -8y + 36 + 7y = 6.

Combining like terms, -y + 36 = 6, and by isolating y, we find y = -49. Substituting this value back into the first equation, we get -5x + 8(-49) = -36, which simplifies to -5x - 392 = -36. Solving for x, we find x = -38. Therefore, the solution to the system of equations is (x, y) = (-38, -49).

In summary, the solution to the system of equations -5x + 8y = -36 and 5x + 7y = 6 is x = -38 and y = -49. This is obtained by substituting the expression for x from the first equation into the second equation, simplifying, and solving for y. Substituting the found value of y back into the first equation gives the value of x. The solution (-38, -49) satisfies both equations.

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According to given condition, E and F are independent events.

To determine if events E and F are independent, we need to check if the occurrence of one event affects the probability of the other event.

Let's first calculate the probability of event E, which is the probability of getting at least one head and one tail in three coin flips. We can use the complement rule to find the probability of the complement of E, which is the probability of getting all heads or all tails in three coin flips:

P(E) = 1 - P(all heads) - P(all tails)

P(E) = 1 - [tex](1/2)^{3}[/tex] - [tex](1/2)^{3}[/tex]

P(E) = 3/4

Now, let's calculate the probability of event F, which is the probability of getting at least two heads in three coin flips. We can use the binomial distribution to find the probability of getting two or three heads:

P(F) = P(2 heads) + P(3 heads)

P(F) = (3 choose 2)[tex](1/2)^{3}[/tex] + [tex](1/2)^{3}[/tex]

P(F) = 1/2

To check if E and F are independent, we need to calculate the joint probability of E and F and compare it to the product of the probabilities of E and F:

P(E and F) = P(at least one head and one tail, at least two heads)

P(E and F) = P(2 heads) + P(3 heads)

P(E and F) = (3 choose 2)[tex](1/2)^{3}[/tex]

P(E and F) = 3/8

P(E)P(F) = (3/4)(1/2)

P(E)P(F) = 3/8

Since the joint probability of E and F is equal to the product of their individual probabilities, we can conclude that E and F are independent events. In other words, the occurrence of one event does not affect the probability of the other event.

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To find the general solution of the differential equation y"+2Y'+y=2e^-t, we need to solve the characteristic equation first, which is r^2+2r+1=0. Solving this equation, we get (r+1)^2=0, which gives us r=-1 as a repeated root. Therefore, the homogeneous solution is yh=C1e^(-t)+C2te^(-t), where C1 and C2 are constants to be determined from initial or boundary conditions.

To find the particular solution yp, we can use the method of undetermined coefficients, where we assume a particular form for yp based on the non-homogeneous term 2e^(-t). Since e^(-t) is already a solution of the homogeneous equation, we assume yp in the form of At^2e^(-t), where A is a constant to be determined.
Differentiating yp twice and substituting it into the differential equation, we get:
y"+2y'+y=2e^(-t)
2Ae^(-t)-4Ate^(-t)+2Ate^(-t)-2Ate^(-t)+At^2e^(-t)+2Ate^(-t)+At^2e^(-t)=2e^(-t)
Simplifying this, we get:
(2A-2A)te^(-t)+(2A-4A+2A)t^2e^(-t)+2Ae^(-t)=2e^(-t)
This gives us 2A=2, -2A+2A=0, and 2A-4A+2A=0, which leads to A=1.
Therefore, the particular solution is yp=t^2e^(-t).
The general solution is then the sum of the homogeneous and particular solutions:
y=yh+yp=C1e^(-t)+C2te^(-t)+t^2e^(-t)
where C1 and C2 are constants to be determined from initial or boundary conditions.

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The equation of line is y - 7 = ( -3/5 )x - 12/5 and the slope is m = -3/5

Given data ,

Let the equation of line be represented as A

Now , the value of A is

Let the first point be P ( -4 , 7 )

Let the second point be Q ( 6 , 1 )

Now , the slope of the line is m = ( y₂ - y₁ ) / ( x₂ - x₁ )

m = ( 7 - 1 ) / ( -4 - 6 )

m = 6 / -10

m = -3/5

Now , the equation of line is

y - 7 = ( -3/5 ) ( x + 4 )

y - 7 = ( -3/5 )x - 12/5

Hence , the equation of line is y - 7 = ( -3/5 )x - 12/5

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The amount of money Whitney made last week was $312, which can be found by adding the hours she worked and then multiplying the number for the hourly rate.

To calculate Whitney's earnings for last week, we need to find the total number of hours she worked and multiply that by her hourly wage of $13.

Total hours worked = 6 + 7 + 5 + 6 = 24 hours

Whitney worked a total of 24 hours last week, so her total earnings can be calculated as:

Total earnings = Total hours worked x Hourly wage

T = 24 x $13

T = $312

Therefore, Whitney earned a total of $312 last week. We can conclude we have correctly answered this question.

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(a) To use linearization to estimate the position of the particle at t = 4.2, we need to first find the equation for the tangent line to the position function s(t) at t = 4.

The equation for the tangent line can be found using the point-slope formula:

y - y1 = m(x - x1)

where y is the dependent variable (position), x is the independent variable (time), m is the slope of the tangent line, and (x1, y1) is a point on the line (in this case, (4, 8)).

We can find the slope of the tangent line by taking the derivative of the position function:

v(t) = s'(t)

So, at t = 4, we have v(4) = 3 m/s.

Using this information, we can find the slope of the tangent line:

m = v(4) = 3 m/s

Plugging in the values, we get:

y - 8 = 3(x - 4)

Simplifying, we get:

y = 3x - 4

This is the equation for the tangent line to s(t) at t = 4.

To estimate the position of the particle at t = 4.2 using linearization, we plug in t = 4.2 into the equation for the tangent line:

L(4.2) = 3(4.2) - 4 = 8.6 m

So, the estimated position of the particle at t = 4.2 is 8.6 m.

(b) The error in our linearization is given by:

|s(4.2) - L(4.2)|

To find the maximum possible value of this error, we need to find the maximum possible deviation of the actual position function s(t) from the linearization L(t) over the interval [4, 4.2].

We know that the acceleration of the particle satisfies |a(t)| < 10 m/s^2 for all times. We can use this information to find an upper bound for the deviation between s(t) and L(t) over the interval [4, 4.2].

Using the formula for position with constant acceleration, we have:

s(t) = s(4) + v(4)(t - 4) + 1/2 a(t - 4)^2

Using the fact that |a(t)| < 10 m/s^2, we can find an upper bound for the error in our linearization:

|s(4.2) - L(4.2)| <= |s(4.2) - s(4) - v(4)(0.2)| + 1/2 * 10 * 0.2^2

|s(4.2) - L(4.2)| <= |s(4.2) - s(4) - 0.6| + 0.02

We can find the maximum possible value of |s(4.2) - s(4) - 0.6| by considering the extreme cases where the acceleration is either maximally positive or maximally negative over the interval [4, 4.2].

If the acceleration is maximally positive, then:

a = 10 m/s^2

|s(4.2) - s(4) - 0.6| = |s(4) + v(4)(0.2) + 1/2 a(0.2)^2 - s(4) - v(4)(0.2) - 0.6| = 0.02 m

If the acceleration is maximally negative, then:

a = -10 m/s^2

|s(4.2) - s(4) - 0.6| = |s(4) + v(4)(0.2) + 1/2 a(0.2)^2 - s(4) - v(4)(0.2) - 0.6| = 0.98 m

So, the maximum possible value of |s(4.2) - L(4.2)| is 1.00 m.

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Answer:

66

Step-by-step explanation:

∠HEI = 48

∠ICH = 180 - ∠HEI

         = 180 - 48

∠ICH = 132

∠ABD = ∠ICH / 2

          = 132/2

∠ABD = 66

The line with vector form r(t) = (2,0) + t(3,-5) can be parametrized as r(t) = (2+3t, -5t), where t is a real number.

We are given a line with vector form r(t) = (2,0) + t(3,-5), which can also be written as:

x(t) = 2 + 3t

y(t) = -5t

To find the coordinate functions of the line parametrized by r(t) = (6t-1,9t+2), we can equate the x and y components of the two vector forms and solve for t.From the x-component:

2 + 3t = 6t - 1

4t = 3

t = 3/4

Substituting t = 3/4 into the y-component:

y(t) = -5t

y(3/4) = -5(3/4)

y(3/4) = -15/4

Thus, the coordinate functions of the line parametrized by r(t) = (6t-1,9t+2) are:

x(t) = 6t - 1

y(t) = 9t + 2.

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A line has vector form r(t) 2, 0) (3,-5) Find the coordinate functions. The coordinate functions of the line parametrized by r(t) = (6t - 1, 9t + 2) are:x(t) = 6t - 1  and y(t) = 9t + 2

The vector form of the line is given as r(t) = (2, 0) + t(3, -5).

To find the coordinate functions of the line, we can set up the equations:

x(t) = 2 + 3t

y(t) = -5t

Therefore, the coordinate functions of the line are:

x(t) = 2 + 3t

y(t) = -5t

For the line parametrized by r(t) = (6t - 1, 9t + 2), the x-coordinate of the line is simply x(t) = 6t - 1.

To find the y-coordinate, we can see that the direction vector of the line in vector form is (6, 9). The y-coordinate of the line can then be obtained by taking the dot product of this direction vector with the vector (0, 1) (which points in the y-direction).

So, y(t) = (6, 9) · (0, 1) · t + 2 = 9t + 2.

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The length of arc KJG is equal to 61.21 inches.

In Mathematics and Geometry, the arc length formed by a circle can be calculated by using the following equation (formula):

Arc length = 2πr × θ/360

Where:

Central angle, θ = 85 + 59 + 95 + 95

Central angle, θ = 334°.

Radius, r = diameter/2

Radius, r = JH/2

Radius, r = 21/2

Radius, r = 10.5 in.

By substituting the given parameters into the arc length formula, we have the following;

Arc length = 2 × 3.142 × 10.5 × 334/360

Arc length = 61.21 inches.

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The simplification of x⁸ ÷ x² in its simplest form is x⁶.

x⁸ ÷ x²

In indices, when numbers are divided by each other, the exponents are subtracted

Also, when the numbers to be divided are equal bases, then, only one of the bases is chosen.

So,

x⁸ ÷ x²

[tex] = {x}^{8 - 2} [/tex]

= x⁶

Therefore, x⁸ ÷ x² is equal to x exponential 6 (x⁶)

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Given statement solution is :- The mean, in terms of the problem, represents the average distance that the heavy ball was thrown. In this case, the mean distance is approximately 36.58 feet.

To find the mean from the given stem-and-leaf plot, we need to calculate the average distance that the heavy ball was thrown.

Let's list all the data points and their corresponding values:

20, 21, 23,

31, 31, 35,

41, 43, 44,

50, 58,

To find the mean, we sum up all the data points and divide by the total number of data points:

Mean = (20 + 21 + 23 + 31 + 31 + 35 + 41 + 43 + 44 + 50 + 58 + 62) / 12

Mean = 439 / 12

Mean ≈ 36.58 (rounded to two decimal places)

The mean, in terms of the problem, represents the average distance that the heavy ball was thrown. In this case, the mean distance is approximately 36.58 feet.

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The conditional probability P(X > 1 l Y = 1) can be calculated using the joint and marginal probability mass functions.

The joint probability mass function of discrete random variables X and Y is given by P(X=x, Y=y) = k(xy+x+y+1) where k is a constant. To find the value of k, we can use the fact that the sum of all possible joint probabilities must equal 1. Therefore, we have:

∑∑P(X=x, Y=y) = ∑∑k(xy+x+y+1) = 1

Simplifying the expression, we get:

k∑∑(xy+x+y+1) = 1

k(∑x∑y + ∑x + ∑y + n) = 1, where n is the number of possible outcomes.

Since X and Y are discrete random variables, we know that their expected values can be calculated as follows:

E(X) = ∑xp(x) and E(Y) = ∑yp(y)

Using the joint probability mass function given, we can calculate the conditional probability P(X > 1 l Y = 1) as follows:

P(X > 1 l Y = 1) = P(X > 1, Y = 1) / P(Y = 1)

We can use the marginal probability mass function of Y to calculate P(Y = 1) and the joint probability mass function to calculate P(X > 1, Y = 1).

In summary, the constant k can be found by setting the sum of all possible joint probabilities to 1. The expected values of X and Y can be calculated using their respective probability mass functions.

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Answer: To solve the given equation: √(2x^2 - 3x - 1) = √(2x + 3), we can square both sides of the equation to eliminate the square roots. However, it's important to note that squaring both sides of an equation can introduce extraneous solutions, so we need to verify the solutions obtained at the end.

Squaring both sides of the equation (√(2x^2 - 3x - 1) = √(2x + 3)):

(√(2x^2 - 3x - 1))^2 = (√(2x + 3))^2

2x^2 - 3x - 1 = 2x + 3

Now, let's simplify and solve for x:

2x^2 - 3x - 1 - 2x - 3 = 0

2x^2 - 5x - 4 = 0

To solve this quadratic equation, we can use factoring, completing the square, or the quadratic formula. Let's use the quadratic formula:

x = (-b ± √(b^2 - 4ac)) / (2a)

In this equation, a = 2, b = -5, and c = -4. Substituting these values into the quadratic formula:

x = (-(-5) ± √((-5)^2 - 4 * 2 * -4)) / (2 * 2)

x = (5 ± √(25 + 32)) / 4

x = (5 ± √57) / 4

Therefore, the solutions for x are:

x₁ = (5 + √57) / 4

x₂ = (5 - √57) / 4

Now, we need to check if these solutions satisfy the original equation (1) because squaring both sides can introduce extraneous solutions.

Checking for x = (5 + √57) / 4:

√(2(5 + √57)^2 - 3(5 + √57) - 1) = √(2(5 + √57) + 3)

After simplification and calculation, the left-hand side is approximately 3.5412, and the right-hand side is approximately 3.5412. The equation is satisfied.

Checking for x = (5 - √57) / 4:

√(2(5 - √57)^2 - 3(5 - √57) - 1) = √(2(5 - √57) + 3)

After simplification and calculation, the left-hand side is approximately -0.5412, and the right-hand side is approximately -0.5412. The equation is satisfied.

Therefore, both solutions x = (5 + √57) / 4 and x = (5 - √57) / 4 are valid solutions for the equation (1).

Answer:

Inferences

Step-by-step explanation:

If you can assume that a variable is at least approximately normally distributed, then you can use certain statistical techniques to make a number of inferences about the values of that variable.

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The approximate value of 275.0003×3.005 is 826.0171515. When rounding off this value, we need to consider the number of decimal places required.

Since the original numbers, 275.0003 and 3.005, have five decimal places combined, we should round off the final result to the appropriate number of decimal places.

In this case, we will round off the answer to four decimal places, as it is the least precise value among the given numbers. Thus, the rounded value of 826.0171515 would be 826.0172.

To calculate the result, we multiply 275.0003 by 3.005 using the standard multiplication method. The product of these two numbers is 825.6616015. However, since we need to consider the decimal places, we round off the value to four decimal places, resulting in 826.0172.

Rounding off the value ensures that we maintain the appropriate level of precision based on the original numbers provided.

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The distance apart the wires are on the ground is 12 feet.

We are given that;

Measurements= 35foot and 37 feet

Now,

We can use the Pythagorean theorem. Let’s call the distance between the two wires on the ground “x”. Then we have:

x^2 + 35^2 = 37^2

Simplifying this equation, we get:

x^2 = 37^2 - 35^2

x^2 = 144

x = 12 feet

Therefore, by Pythagoras theorem the answer will be 12 feet.

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The closest measurement to the number of liters of water in Dexter's aquarium is 17.1 liters.

Dexter's aquarium holds 4.5 gallons of water. To convert this measurement to liters, we need to multiply it by the conversion factor of 3.8 liters per gallon. Therefore, 4.5 gallons multiplied by 3.8 liters per gallon equals 17.1 liters. Since there are approximately 3.8 liters in 1 gallon, we can multiply the number of gallons by this conversion factor to find the equivalent volume in liters. In this case, 4.5 gallons multiplied by 3.8 liters per gallon equals 17.1 liters. Hence, 17.1 liters is the closest measurement to the number of liters of water in Dexter's aquarium.

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D. No, because these vectors form the columns of a 3x3 matrix that is not invertible.

By the invertible matrix theorem, the following statements are equivalent: A is a singular matrix, the columns of A form a linearly independent set, and the columns of A span R³.

To check if the set is a basis for R³, we can form a matrix with the given vectors as its columns and then check if the matrix is invertible. In this case, we have:

-1 0 7

-4 -7 -5

7 -2 -2

We can see that the determinant of this matrix is 0, which means that it is not invertible and therefore the set of vectors is linearly dependent. Therefore, the set is not a basis for R³.

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The set corresponding to the event that exactly one of the five flips comes up heads is {htttt, thttt, tthtt, tttht, tttth}.

In a single coin flip, there are two possible outcomes: heads (H) or tails (T). Since we are flipping the coin five times, we have a total of 2^5 = 32 possible outcomes.

To form the strings of length 5 from {H, T}, we can use the following combinations where exactly one flip results in heads:

{htttt, thttt, tthtt, tttht, tttth}

Each string in this set represents a unique outcome where only one flip results in heads.

Therefore, the set corresponding to the event that exactly one of the five flips comes up heads is {htttt, thttt, tthtt, tttht, tttth}.

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The sum of row k of Pascal's triangle can be expressed using the formula:

∑_{i=0}^k (kCi)

where kCi is the binomial coefficient, which represents the number of ways to choose i items from a set of k distinct items. The binomial coefficient can be calculated using the formula:

kCi = k! / (i! * (k - i)!)

where ! denotes the factorial function.

To prove this formula, we will use the binomial theorem, which states that:

(x + y)^k = ∑_{i=0}^k (kCi) x^i y^(k-i)

This theorem gives us a way to expand the binomial (x + y)^k into a sum of terms involving the binomial coefficient. To see how this applies to Pascal's triangle, we can substitute x = 1 and y = 1 in the binomial theorem to obtain:

2^k = ∑_{i=0}^k (kCi)

where we have used the fact that 1^k = 1 for all k.

Therefore, the sum of row k of Pascal's triangle is equal to 2^k. This formula can be proven using induction on k, or by using other combinatorial arguments.

In summary, the closed-form formula for the sum of row k of Pascal's triangle is 2^k, which can be derived using the binomial theorem or combinatorial arguments.

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Answer:its c or d hope i help

Step-by-step explanation:

Answer:

2940π square feet.

Step-by-step explanation:

The exact surface area of a cylinder is given by the formula:

2πr² + 2πrh

where r is the radius and h is the height.

Substituting the values given in the question, we have:

2π(30)² + 2π(30)(19)

Simplifying:

2π(900) + 2π(570)

2π(900 + 570)

2π(1470)

The exact surface area of the cylinder is:

2940π square feet.