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Mark throws a ball with initial speed of 125 ft/sec at an angle of 40 degrees. It was thrown 3 ft off the ground. How long was the ball in the air? how far did the ball travel horizontally? what was the ball's maximum height?

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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The paradox you mentioned, which bothered mathematicians of Euler's time, is based on an incorrect manipulation of logarithmic properties and equations involving complex numbers.

Let's examine the steps of the paradox that  bothered mathematicians of Euler and explain where the error lies.

The paradox begins with the expression (-jc)^2 = (jc)^2. This is true, as squaring a complex number only affects its magnitude and not its sign.

Then, the next step is to take the logarithm of both sides: log((-jc)^2) = log((jc)^2). Applying the exponent rule of logarithms, we get 2log(-jc) = 2log(jc).

Here is where the error occurs. In complex analysis, the logarithm function is multivalued for complex numbers. This means that for a given complex number, there can be multiple values for its logarithm. The paradox assumes that the logarithm of a negative number and the logarithm of its positive counterpart are equal, but that is not the case.

When we have log(-jc), it is not well-defined without specifying a branch or principal value of the logarithm. The same applies to log(jc). By assuming they are equal, the paradox leads to the incorrect conclusion that log(-jc) = log(jc).

In reality, the logarithm of a complex number is not a simple function like it is for real numbers. It requires considering complex analysis and the concept of branches or principal values to properly handle logarithmic equations involving complex numbers.

In conclusion, the paradox arises from an invalid assumption about the equality of logarithms of negative and positive complex numbers and ignores the intricacies of complex analysis. It highlights the importance of understanding the properties and limitations of mathematical operations when dealing with complex numbers.

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Answer: For the first pic, c= 17.20. For the second pic, x= 50.

Step-by-step explanation:

We need to use the Pythagorean theorem for these problems. A^2 + B^2= C^2

For the square (first picture).

It doesn't matter what values we put for A and B, as long as the hypotenuse (denoted in the picture as c) is C.

Let A= 10, and B=14

Plug the values into the equation!

[tex](10)^2 + (14)^2 = C^2[/tex]

Simplify: [tex]100 + 196 = C^2[/tex]

[tex]296 = C^2[/tex]

[tex]\sqrt{296} = \sqrt{C^2}[/tex]

[tex]\sqrt{296} = C[/tex]

17.20= C

Therefore, c= 17.20

PICTURE #2:

Complete the problem exactly how you did the first one.

Let A=48, and B=14

Plug those values into the pythagorean theorem...

[tex](48)^2 + (14)^2 = C^2[/tex]

Simplify: [tex]2304 + 196 = C^2[/tex]

2500 = C^2

[tex]\sqrt{2500} =\sqrt{C^2}[/tex]

[tex]\sqrt{2500} = C[/tex]

50= C

SO, 50 = x

Hope this all helps!!

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 unit tangent vector T(t) is incorrect. The correct unit tangent vector T(t) and unit normal vector N(t) need to be determined.

To find the unit tangent vector T(t), we differentiate the vector function r(t) with respect to t and divide the result by its magnitude. The unit tangent vector T(t) represents the direction of motion along the curve.

Differentiating r(t) = (8t, 3 cos t, 3 sin t) with respect to t, we get r'(t) = (8, -3 sin t, 3 cos t). Dividing r'(t) by its magnitude, we obtain the unit tangent vector T(t).

To find the unit normal vector N(t), we differentiate T(t) with respect to t, divide the result by its magnitude, and obtain the unit normal vector N(t). The unit normal vector N(t) represents the direction of curvature of the curve.

Differentiating T(t) = (8, -3 sin t, 3 cos t) with respect to t, we get T'(t) = (0, -3 cos t, -3 sin t). Dividing T'(t) by its magnitude, we obtain the unit normal vector N(t).

For the given vector function r(t) = (8t, 3 cos t, 3 sin t), the correct unit tangent vector T(t) is T(t) = (8, -3 sin t, 3 cos t) / √(64 + 9 sin^2 t + 9 cos^2 t), and the correct unit normal vector N(t) is N(t) = (0, -3 cos t, -3 sin t) / √(9 cos^2 t + 9 sin^2 t).

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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 value of z that satisfies P(Z < z) = 0.9251 is approximately 1.44(d).

The question asks for the value of z that corresponds to a cumulative probability of 0.9251.The value of z represents the standard score or z-score, which corresponds to a particular cumulative probability.To find this value, we can use a standard normal distribution table or a statistical software.

By looking up the closest probability value in the table, we find that the corresponding z-value is approximately 1.44. Therefore, the answer is option (d) 1.44.

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To find an equation of the plane tangent to the surface 8xy + 5yz + 7xz − 80 = 0 at the point (2, 2, 2), we need to find the gradient vector of the surface at that point.

The gradient vector is given b

grad(f) = (df/dx, df/dy, df/dz)

where f(x, y, z) = 8xy + 5yz + 7xz − 80.

Taking partial derivatives,

df/dx = 8y + 7z

df/dy = 8x + 5z

df/dz = 5y + 7x

Evaluating these at the point (2, 2, 2), we get:

df/dx = 8(2) + 7(2) = 30

df/dy = 8(2) + 5(2) = 26

df/dz = 5(2) + 7(2) = 24

So the gradient vector at the point (2, 2, 2) is:

grad(f)(2, 2, 2) = (30, 26, 24)

This vector is normal to the tangent plane. Therefore, an equation of the tangent plane is given by:

30(x − 2) + 26(y − 2) + 24(z − 2) = 0

Simplifying, we get:

30x + 26y + 24z − 136 = 0

So the equation of the plane to the surface at the point (2, 2, 2) is 30x + 26y + 24z − 136 = 0.

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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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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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Given a well-balanced algebraic expression, we can construct a corresponding expression syntax tree using the postfix notation. This involves converting the infix expression to postfix and then building an evaluation tree.

To construct an expression syntax tree, we first need to convert the given infix expression to postfix notation. We can achieve this by using the infixToPostfix algorithm, which uses a stack to convert the infix expression to postfix notation. For example, the infix expression 4 + ((7 + 9) * 2) would be converted to postfix notation as 479+2*+.

Next, we can use the postfix expression to build an evaluation tree. This is done by starting at the first element of the postfix expression and moving left to right. When an operator is encountered, we pop the top two nodes from the stack, create a new node with the operator as its value and the two popped nodes as its left and right children, and push the new node onto the stack.

Once the evaluation tree is constructed, we can perform an infix traversal of the tree to obtain the infix expression. This involves traversing the tree in an inorder fashion (left subtree, current node, right subtree) and appending the nodes' values to form the infix expression. In our example, the infix traversal of the evaluation tree would give us

[tex](4 + ((7 + 9 )* 2 )).[/tex]

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The equation for a multiple regression model with p predictor variables (x1, x2, ..., xp) and a response variable (y) can be written as:

y = β0 + β1*x1 + β2*x2 + ... + βp*xp + ε

In this equation:

- y represents the response variable (the variable we are trying to predict).

- β0 represents the y-intercept or the constant term.

- β1, β2, ..., βp represent the coefficients or weights associated with each predictor variable (x1, x2, ..., xp).

- x1, x2, ..., xp represent the predictor variables.

- ε represents the error term or residual, which accounts for unexplained variation in the model.

The multiple regression model aims to estimate the relationship between the predictor variables and the response variable by finding the best-fitting values for the coefficients β0, β1, β2, ..., βp.

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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) 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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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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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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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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The Taylor polynomials T2 and T3 centered at x=3 for the function f(x)=x^4-7x are: T2(x)=23(x−3)4−56(x−3)+27, T3(x)=23(x−3)4−56(x−3)+27−14(x−3)3

To find the Taylor polynomial centered at x=3, we need to find the derivatives of f(x) up to the nth derivative and evaluate them at x=3. Then, we use the formula for the Taylor polynomial of degree n centered at x=a:

Tn(x)=f(a)+f′(a)(x−a)+f′′(a)(x−a)2+⋯+f(n)(a)(x−a)n/n!

For this particular problem, we are given that a=3 and f(x)=x^4-7x. Taking the derivatives of f(x), we get:

f'(x)=4x^3-7

f''(x)=12x^2

f'''(x)=24x

f''''(x)=24

Evaluating these derivatives at x=3, we get:

f(3)=-54

f'(3)=29

f''(3)=108

f'''(3)=72

f''''(3)=24

Plugging these values into the Taylor polynomial formula, we get the expressions for T2 and T3 as stated above.

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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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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:

[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 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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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 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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the answer is: f · dr = -30

To find f · dr for the line c from (3, 2, -2) to (6, 1, 7), we first need to parametrize the line in terms of a vector function r(t). We can do this as follows:

r(t) = <3, 2, -2> + t<3, -1, 9>

This gives us a vector function that describes all the points on the line c as t varies.

Next, we need to calculate f · dr for this line. We can use the formula:

f · dr = ∫c f · dr

where the integral is taken over the line c. We can evaluate this integral by substituting r(t) for dr and evaluating the dot product:

f · dr = ∫c f · dr = ∫[3,6] f(r(t)) · r'(t) dt

where [3,6] is the interval of values for t that correspond to the endpoints of the line c. We can evaluate the dot product f(r(t)) · r'(t) as follows:

f(r(t)) · r'(t) = <5y, 2, -1> · <3, -1, 9>

= 15y - 2 - 9

= 15y - 11

where we used the given expression for f and the derivative of r(t), which is r'(t) = <3, -1, 9>.

Plugging this dot product back into the integral, we get:

f · dr = ∫[3,6] f(r(t)) · r'(t) dt

= ∫[3,6] (15y - 11) dt

To evaluate this integral, we need to express y in terms of t. We can do this by using the equation for the y-component of r(t):

y = 2 - t/3

Substituting this into the integral, we get:

f · dr = ∫[3,6] (15(2 - t/3) - 11) dt

= ∫[3,6] (19 - 5t) dt

= [(19t - 5t^2/2)]|[3,6]

= (57/2 - 117/2)

= -30

Therefore, the answer is:

f · dr = -30

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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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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 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 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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