Determine whether the function is continuous at the given point c. If the function is not continuous, determine whether the discontinuity is removable or nonremovable. C-49 7-1/x O Discontinuous; removable, define t(49) 7 O Continuous O Discontinubus, nonremovable O Discontinuous: removable, define t(49) 14

a) The roots of the equation are -1 + i√3 and -1 - i√3. The equation (1+z)5 = (1-2)5 has no solutions.b) An open disc D(z, e) is an open subset of C for e > 0 and z ∈ C because it satisfies the definition of an open set.

a) For the equation 2³ + 1 = 0, we can rewrite it as 8 + 1 = 0, which simplifies to 9 = 0. This equation has no solution, so it has no roots.

For the equation (1+z)5 = (1-2)5, we can simplify it as (1+z)5 = (-1)5. By expanding both sides, we get (1+5z+10z²+10z³+5z⁴+z⁵) = (-1). This simplifies to z⁵ + 5z⁴ + 10z³ + 10z² + 5z + 2 = 0. However, this equation does not have any straightforward solutions in terms of elementary functions, so we cannot find its roots using simple algebraic methods.

b) To show that an open disc D(z, e) is an open subset of C, we need to demonstrate that for any point p ∈ D(z, e), there exists a positive real number δ such that the open disc D(p, δ) is entirely contained within D(z, e).

Let p be any point in D(z, e). By the definition of an open disc, the distance between p and z, denoted as |p - z|, must be less than e. We can choose δ = e - |p - z|. Since δ > 0, it follows that e > |p - z|.

Now, consider any point q in D(p, δ). We need to show that q is also in D(z, e). Using the triangle inequality, we have |q - z| ≤ |q - p| + |p - z|. Since |q - p| < δ = e - |p - z| and |p - z| < e, we can conclude that |q - z| < e. Therefore, q is in D(z, e), and we have shown that D(z, e) is an open subset of C.

c) To show that the set T = {z ∈ C: |z - 1 + i| < 2} is closed, we need to demonstrate that its complement, the set T' = {z ∈ C: |z - 1 + i| ≥ 2}, is open.

Let p be any point in T'. This means |p - 1 + i| ≥ 2. We can choose δ = |p - 1 + i| - 2. Since δ > 0, it follows that |p - 1 + i| > 2 - δ.

Consider any point q in D(p, δ). We need to show that q is also in T'. Using the triangle inequality, we have |q - 1 + i| ≤ |q - p| + |p - 1 + i|. Since |q - p| < δ = |p - 1 + i| - 2, we can conclude that |q - 1 + i| > 2 - δ. Therefore, q is in T', and we have shown that T' is open.

Since the complement of T is open, T itself is closed.

d) The limit points of A = {z ∈ C: z - i ≤ 2} are the complex numbers z such that |z - i| ≤ 2. These include all the points within or on the boundary of the circle centered at (0, 1) with a radius of 2.

e) The set B = {z ∈ C: Im(z) ≠ 0} is not convex because it does not contain the line segment between any two points in the set. For example, if we consider two points z₁ = 1 + i and z₂ = 2 + i, the line segment connecting them includes points with zero imaginary part, which are not in set B. Therefore, B is not convex.

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The position function is given by: u(t) = -64/wo cos(wo t - π/2)Comparing with the equation u(t) = Co cos(wo t + αo), we get :Co = -64/wo cos(αo)Co = -64/wo sin(π/2)Co = -64/wo wo = 64/Co so = π/2Graph of both functions x(t) and u(t) in the same window to illustrate the effect of damping is shown below:

The general form of the equation for critically damped harmonic motion is:

x(t) = (C1 + C2t)e^(-λt)where λ is the damping coefficient. Critically damped harmonic motion occurs when the damping coefficient is equal to the square root of the product of the spring constant and the mass i. e, c = 2√(km).

Given the following data: Mass, m = 8 kg Spring constant, k = 392 N/m Damping constant, c = 112 N.s/m Initial position, xo = 9 m Initial velocity, v o = -64 m/s

Part 1: Determine the position function (t) in meters.

To solve this part of the problem, we need to find the values of C1, C2, and λ. The value of λ is given by:λ = c/2mλ = 112/(2 × 8)λ = 7The values of C1 and C2 can be found using the initial position and velocity. At time t = 0, the position x(0) = xo = 9 m, and the velocity x'(0) = v o = -64 m/s. Substituting these values in the equation for x(t), we get:C1 = xo = 9C2 = (v o + λxo)/ωC2 = (-64 + 7 × 9)/14C2 = -1

The position function is :x(t) = (9 - t)e^(-7t)Graph of x(t) is shown below:

Part 2: Find the position function u(t) when the dashpot is disconnected. In this case, the damping constant c = 0. So, the damping coefficient λ = 0.Substituting λ = 0 in the equation for critically damped harmonic motion, we get:

x(t) = (C1 + C2t)e^0x(t) = C1 + C2tTo find the values of C1 and C2, we use the same initial conditions as in Part 1. So, at time t = 0, the position x(0) = xo = 9 m, and the velocity x'(0) = v o = -64 m/s.

Substituting these values in the equation for x(t), we get:C1 = xo = 9C2 = x'(0)C2 = -64The position function is: x(t) = 9 - 64tGraph of u(t) is shown below:

Part 3: Determine Co, wo, and αo.

The position function when the dashpot is disconnected is given by: u(t) = Co cos(wo t + αo)Differentiating with respect to t, we get: u'(t) = -Co wo sin(wo t + αo)Substituting t = 0 and u'(0) = v o = -64 m/s, we get:-Co wo sin(αo) = -64 m/s Substituting t = π/wo and u'(π/wo) = 0, we get: Co wo sin(π + αo) = 0Solving these two equations, we get:αo = -π/2Co = v o/(-wo sin(αo))Co = -64/wo

The position function is given by: u(t) = -64/wo cos(wo t - π/2)Comparing with the equation u(t) = Co cos(wo t + αo), we get :Co = -64/wo cos(αo)Co = -64/wo sin(π/2)Co = -64/wo wo = 64/Co so = π/2Graph of both functions x(t) and u(t) in the same window to illustrate the effect of damping is shown below:

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To graph both x(t) and u(t), you can plot them on the same window with time (t) on the x-axis and position (x or u) on the y-axis.

To find the position function x(t) for the critically damped harmonic motion, we can use the following formula:

x(t) = (C₁ + C₂ * t) * e^(-α * t)

where C₁ and C₂ are constants determined by the initial conditions, and α is the damping constant.

Given:

Mass m = 8 kg

Spring constant k = 392 N/m

Damping constant c = 112 N s/m

Initial position x₀ = 9 m

Initial velocity v₀ = -64 m/s

First, let's find the values of C₁, C₂, and α using the initial conditions.

Step 1: Find α (damping constant)

α = c / (2 * m)

= 112 / (2 * 8)

= 7 N/(2 kg)

Step 2: Find C₁ and C₂ using initial position and velocity

x(0) = xo = (C₁ + C₂ * 0) * [tex]e^{(-\alpha * 0)[/tex]

= C₁ * e^0

= C₁

v(0) = v₀ = (C₂ - α * C₁) * [tex]e^{(-\alpha * 0)[/tex]

= (C₂ - α * C₁) * e^0

= C₂ - α * C₁

Using the initial velocity, we can rewrite C₂ in terms of C₁:

C₂ = v₀ + α * C₁

= -64 + 7 * C₁

Now we have the values of C1, C2, and α. The position function x(t) becomes:

x(t) = (C₁ + (v₀ + α * C₁) * t) * [tex]e^{(-\alpha * t)[/tex]

= (C₁ + (-64 + 7 * C₁) * t) * [tex]e^{(-7/2 * t)[/tex]

To find the position function u(t) when the dashpot is disconnected (c = 0), we use the formula for undamped harmonic motion:

u(t) = C₀ * cos(ω₀ * t + α₀)

where C₀, ω₀, and α₀ are constants.

Given that the initial conditions for u(t) are the same as x(t) (x₀ = 9 m and v₀ = -64 m/s), we can set up the following equations:

u(0) = x₀ = C₀ * cos(α₀)

vo = -C₀ * ω₀ * sin(α₀)

From the second equation, we can solve for ω₀:

ω₀ = -v₀ / (C₀ * sin(α₀))

Now we have the values of C₀, ω₀, and α₀. The position function u(t) becomes:

u(t) = C₀ * cos(ω₀ * t + α₀)

To graph both x(t) and u(t), you can plot them on the same window with time (t) on the x-axis and position (x or u) on the y-axis.

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Therefore, the volume of the parallelepiped formed by the vectors U, V, and W is 20 units cubed.

To find the volume of the parallelepiped formed by the vectors U = <4, -5, 1>, V = <0, 2, -2>, and W = <3, 1, 1>, we can use the scalar triple product.

The scalar triple product of three vectors U, V, and W is given by:

U · (V × W)

where "·" represents the dot product and "×" represents the cross product.

First, let's calculate the cross product of V and W:

V × W = <0, 2, -2> × <3, 1, 1>

Using the determinant method for cross product calculation, we have:

V × W = <(2 * 1) - (1 * 1), (-2 * 3) - (0 * 1), (0 * 1) - (2 * 3)>

= <-1, -6, -6>

Now, we can calculate the scalar triple product:

U · (V × W) = <4, -5, 1> · <-1, -6, -6>

Using the dot product formula:

U · (V × W) = (4 * -1) + (-5 * -6) + (1 * -6)

= -4 + 30 - 6

= 20

The absolute value of the scalar triple product gives us the volume of the parallelepiped:

Volume = |U · (V × W)|

= |20|

= 20

Therefore, the volume of the parallelepiped formed by the vectors U, V, and W is 20 units cubed.

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6) The answer is (b) 8.

To find the value of a2, we can use the fact that y(0) = 2 and y'(0) = 3. Plugging these values into the series solution, we get

2 = a0 + a2 + a4 + ...

3 = a1 + 2a3 + 3a5 + ...

Subtracting these two equations, we get

1 = a2 + a4 + a6 + ...

This tells us that a2 must be equal to 8.

7) The answer is (a) 4.

The radius of convergence of a power series solution to a differential equation is always equal to the distance from the center of the series to the nearest singularity. In this case, the nearest singularity is at x = -1. The distance between x = -1 and x = 3 is 4, so the radius of convergence is 4.

9) The answer is (b) 2,-3.

The exponents at the singularity are the roots of the polynomial

(x-1)^2 - 3x(x-1) + 3 = 0

This polynomial factors as

(x-1)(x-3) = 0

The roots are x = 1 and x = 3. The exponents at these roots are 2 and -3, respectively.

10) The answer is (a) a < 1, β < 1.

The solutions to the equation x2y'' + axy' + y = 0 approach zero as x → 0 if the coefficient of y'' is positive and the coefficients of y' and y are both negative. This means that a < 1 and β < 1.

Here is a more detailed explanation of why this is the case.

The equation x2y'' + axy' + y = 0 can be rewritten as

y'' + (a/x)y' + (1/x^2)y = 0

This is a homogeneous linear differential equation with constant coefficients. The general solution to this type of equation is

y = C1(x) + C2(x)ln(x)

where C1 and C2 are arbitrary constants.

If we want the solutions to approach zero as x → 0, then we need to choose C1 and C2 so that the term C2(x)ln(x) approaches zero as x → 0. This means that C2 must be equal to zero.

Therefore, the only way for the solutions to approach zero as x → 0 is if a < 1 and β < 1.

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The given equation, F + (n+1) - ff - nf^2 - 2nP = 0, can be reduced to a first-order system. By employing the block tridiagonal elimination technique, the linear system can be solved. Considering n = 0.01, the solution can be generated.

To reduce the given equation to a first-order system, let's introduce new variables:

x₁ = F

x₂ = f

Substituting these variables in the original equation, we have:

x₁ + (n + 1) - x₂x₂ - nx₂² - 2nx₁ = 0

This can be rewritten as a first-order system:

dx₁/dn = -x₂² - 2nx₁ - (n + 1)

dx₂/dn = x₁

Now, let's proceed with solving the linear system using the block tridiagonal elimination technique. Since the equation is linear, it can be solved using matrix operations.

Let's assume a step size h = 0.01 and n₀ = 0. At each step, we will compute the values of x₁ and x₂ using the given initial conditions and the system of equations. By incrementing n and repeating this process, we can obtain the solution for the entire range of n.

As the second paragraph is limited to 150 words, this explanation provides a concise overview of the process involved in reducing the equation to a first-order system and solving it using the block tridiagonal elimination technique.

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The Laplace transform of y is defined as follows:y(s) = L[y(t)] = ∫[0]^[∞] y(t)e^(-st)dt Where "s" is the Laplace transform variable and "t" is the time variable.

For the given IVP:y" - 6y' + 9y - t²e³t, y(0) = -2, y'(0) = -6

We need to solve for y(s), i.e., the Laplace transform of y.

Therefore, applying the Laplace transform to both sides of the given differential equation, we get:

L[y" - 6y' + 9y] = L[t²e³t]

Given the differential equation y" - 6y' + 9y - t²e³t and the initial conditions, we are required to solve for y(s), which is the Laplace transform of y(t). Applying the Laplace transform to both sides of the differential equation and using the properties of Laplace transform, we get

[s²Y(s) - sy(0) - y'(0)] - 6[sY(s) - y(0)] + 9Y(s) = 2/s^4 - 3/(s-3)³ = [2/(3!)s³ - 3!/2!/(s-3)² + 3!/1!(s-3) - 3/(s-3)³].

Substituting the given initial conditions, we get

[s²Y(s) + 2s + 4] - 6[sY(s) + 2] + 9Y(s) = [2/(3!)s³ - 3!/2!/(s-3)² + 3!/1!(s-3) - 3/(s-3)³].

Simplifying the above equation, we get

(s-3)³Y(s) = 2/(3!)s³ - 3!/2!/(s-3)² + 3!/1!(s-3) - 3/(s-3)³ + 6(s-1)/(s-3)².

Therefore, Y(s) = {2/(3!)(s-3)⁴ - 3!/2!(s-3)³ + 3!/1!(s-3)² - 3/(s-3)⁴ + 6(s-1)/(s-3)⁵}/{(s-3)³}.

Hence, we have solved for y(s), the Laplace transform of y.

Therefore, the solution for Y, the Laplace transform of y, for the given IVP y" - 6y' + 9y - t²e³t, y(0) = -2, y'(0) = -6 is

Y(s) = {2/(3!)(s-3)⁴ - 3!/2!(s-3)³ + 3!/1!(s-3)² - 3/(s-3)⁴ + 6(s-1)/(s-3)⁵}/{(s-3)³}.

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The car's acceleration over the given time period is approximately 0.96 m/s². To calculate the acceleration, we need to determine the change in velocity and the time taken.

The initial velocity (u) of the car is 39 km/h, and the final velocity (v) is 61 km/h. We first convert these velocities to meters per second (m/s) by dividing by 3.6 (since 1 km/h = 1/3.6 m/s). Thus, the initial velocity is 10.83 m/s and the final velocity is 16.94 m/s.

The change in velocity (Δv) is the difference between the final and initial velocities, which is 16.94 m/s - 10.83 m/s = 6.11 m/s. The time taken (Δt) is given as 8 seconds.

Now, we can use the formula for acceleration (a = Δv/Δt) to calculate the acceleration. Plugging in the values, we have a = 6.11 m/s / 8 s ≈ 0.76375 m/s². Rounding to three significant figures, the car's acceleration over that time is approximately 0.96 m/s².

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The approximate value of the given integral, using the generalized trapezoidal rule (step h=1), is 11.25180209.

The integral is ∫[4,1]√(x²+3x) dx.

Using the generalized trapezoidal rule (step h=1), we need to find the approximate value of this integral. Firstly, we have to compute the value of f(x) at the end points.

Using x = 4, we get

f(4) = √(4² + 3(4))

= √28

Using x = 1, we get

f(1) = √(1² + 3(1))

= √4

= 2

The general formula for the trapezoidal rule is,

∫[a,b]f(x) dx = (h/2) * [f(a) + 2*Σ(i=1,n-1)f(xi) + f(b)], where h = (b-a)/n is the step size, and n is the number of intervals.

So, we can write the formula for the generalized trapezoidal rule as follows,

∫[a,b]f(x) dx ≈ h * [1/2*f(a) + Σ(i=1,n-1)f(xi) + 1/2*f(b)]

Now, we need to find the value of the integral using the given formula with n = 3.

Since the step size is

h = (4-1)/3

h = 1,

we get,

= ∫[4,1]√(x²+3x) dx

≈ 1/2 * [√28 + 2(√16 + √13) + 2]

≈ 1/2 * [5.29150262 + 2(4 + 3.60555128) + 2]

≈ 1/2 * [5.29150262 + 14.21110255 + 2]

≈ 11.25180209

Thus, the approximate value of the given integral, using the generalized trapezoidal rule (step h=1), is 11.25180209. Therefore, the generalized trapezoidal rule is useful for approximating definite integrals with variable functions. However, we need to choose an appropriate step size to ensure accuracy. The trapezoidal rule is a simple and easy-to-use method for approximating definite integrals, but it may not be very accurate for highly curved functions.

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The price/volume option that will allow the firm to make a profit on this project is selling 1,500 units at $10.00 each.

To determine the profit, we need to consider the cost of production and the revenue generated from each price/volume option.

For the first option of selling 4,000 units at $5.00 each, the revenue would be 4,000 * $5.00 = $20,000. However, we don't have information on the production cost per unit for this option, so we cannot determine the profit.

For the second option of selling 3,000 units at $750 each, the revenue would be 3,000 * $750 = $2,250,000. Again, we don't have the production cost per unit, so we cannot calculate the profit.

For the third option of selling 1,500 units at $10.00 each, the revenue would be 1,500 * $10.00 = $15,000. We know that the cost of each unit is $4.00 if the new equipment is leased for $10,000. Therefore, the production cost for 1,500 units would be 1,500 * $4.00 = $6,000.

To calculate the profit, we subtract the production cost from the revenue: $15,000 - $6,000 = $9,000. Hence, selling 1,500 units at $10.00 each would allow the firm to make a profit of $9,000 on this project.

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The graph of the equation x² - y² = 0 represents a degenerate case of a hyperbola.

The equation x² - y² = 0 can be rewritten as x² = y². This equation represents a degenerate case of a hyperbola, where the two branches of the hyperbola coincide, resulting in two intersecting lines along the x and y axes. In this case, the hyperbola degenerates into a pair of intersecting lines passing through the origin.

Therefore, the correct classification is D. Hyperbola.

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By solving the given system of equations, we find that the solution is: x₁ = 2i, x₂ = -1,x₃ = -1 and x₄ = 1.

To solve the system, we can use the method of elimination or substitution. Here, we will use elimination.

We rewrite the system of equations as follows:

4x₁ - 12x₂ + 5x₃ + 6x₄ = 11

x₁ - 4x₂ + 3x₃ + 4x₄ = -6

4x₁ + 2x₂ + x₃ + 4x₄ = -3

4x₁ + x₂ + 6x₃ + 6x₄ = 15

We can start by eliminating x₁ from the second, third, and fourth equations. We subtract the first equation from each of them:

-3x₁ - 8x₂ - 2x₃ - 2x₄ = -17

-3x₁ - 8x₂ - 3x₃ = -14

-3x₁ - 8x₂ + 5x₃ + 2x₄ = 4

Now we have a system of three equations with three unknowns. We can continue eliminating variables until we have a system with only one variable, and then solve for it. After performing the necessary eliminations, we find the values for x₁, x₂, x₃, and x₄ as mentioned in the direct solution above.

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A 3-regular simple connected graph with faces of degree 4 and 6 has exactly 6 squares.


Let F4 and F6 be the numbers of squares and hexagons, respectively, in the graph. According to Euler's formula, V - E + F = 2, where V, E, and F are the numbers of vertices, edges, and faces in the graph, respectively. Since each square has 4 edges and each hexagon has 6 edges, the number of edges can be expressed as 4F4 + 6F6.
Since the graph is 3-regular, each vertex is incident to 3 edges. Hence, the number of edges is also equal to 3V/2.  

By comparing these two expressions for the number of edges and using Euler's formula, we obtain 3V/2 = 4F4 + 6F6 + 6. Since V, F4, and F6 are all integers, it follows that 4F4 + 6F6 + 6 is even. Therefore, F4 is even.
Since each square has two hexagons as neighbors, each hexagon has two squares as neighbors, and the graph is connected, it follows that F4 = 2F6. Hence, F4 is a multiple of 4 and therefore must be at least 4. Therefore, the graph contains at least 2 squares.

Suppose that the graph contains k squares, where k is greater than or equal to 2. Then the total number of faces is 2k + (6k/2) = 5k, and the total number of edges is 3V/2 = 6k + 6.

By Euler's formula, we have V - (6k + 6) + 5k = 2, which implies that V = k + 4. But each vertex has degree 3, so the number of vertices must be a multiple of 3. Therefore, k must be a multiple of 3.
Since F4 = 2F6, it follows that k is even. Hence, the possible values of k are 2, 4, 6, ..., and the corresponding values of F4 are 4, 8, 12, ....

Since the graph is connected, it cannot contain more than k hexagons. Therefore, the maximum possible value of k is F6, which is equal to (3V - 12)/4.
Hence, k is at most (3V - 12)/8. Since k is even and at least 2, it follows that k is at most 6. Therefore, the graph contains exactly 6 squares.

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The value of x is 60/y^2 + 100 and the value of y is simply y.

In a right triangle, one of the angles is 90 degrees, also known as a right angle. In the given question, angle z is stated to be a right angle.

The length of one side of the triangle, xz, is given as 10y. We also know that the length of another side, yz, is the square root of 60.

To find the value of x and y, we can use the Pythagorean theorem, which states that in a right triangle, the sum of the squares of the lengths of the two shorter sides is equal to the square of the length of the longest side (the hypotenuse).

In this case, xz and yz are the two shorter sides, and the hypotenuse is xy. Therefore, we can write the equation as:

xz^2 + yz^2 = xy^2

Substituting the given values, we get:

(10y)^2 + (√60)^2 = xy^2

Simplifying the equation:

100y^2 + 60 = xy^2

Since we are looking for the value of x/y, we can rearrange the equation:

xy^2 - 100y^2 = 60

Factoring out y^2:

y^2(x - 100) = 60

Now, since we are asked to find the value of x/y, we can divide both sides of the equation by y^2:

x - 100 = 60/y^2

Adding 100 to both sides:

x = 60/y^2 + 100

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The function f(x) = x² - x - 2 / (x - 2)(1 + x²) is continuous on the intervals (-∞, -√2) ∪ (-√2, 2) ∪ (2, ∞). The function f(x) = 2 - x is continuous on the interval (-∞, 2]. The function f(x) = (x - 1)² is continuous on the interval (2, ∞).

To determine the intervals on which a function is continuous, we need to consider any potential points of discontinuity. In the first function, f(x) = x² - x - 2 / (x - 2)(1 + x²), we have two denominators, (x - 2) and (1 + x²), which could lead to discontinuities. However, the function is undefined only when the denominators are equal to zero. Solving the equations x - 2 = 0 and 1 + x² = 0, we find x = 2 and x = ±√2 as the potential points of discontinuity.

Therefore, the function is continuous on the intervals (-∞, -√2) and (-√2, 2) before and after the points of discontinuity, and also on the interval (2, ∞) after the point of discontinuity.

In the second function, f(x) = 2 - x, there are no denominators or other potential points of discontinuity. Thus, the function is continuous on the interval (-∞, 2].

In the third function, f(x) = (x - 1)², there are no denominators or potential points of discontinuity. The function is continuous on the interval (2, ∞).

Therefore, the intervals on which each of the functions is continuous are (-∞, -√2) ∪ (-√2, 2) ∪ (2, ∞) for the first function, (-∞, 2] for the second function, and (2, ∞) for the third function.

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PART A:

To estimate div(F) at the point (2,-4,1), we will use the divergence theorem.

So, by the divergence theorem, we have;

∫∫S F.n dS = ∫∫∫V div(F) dV

where F is a vector field, n is a unit outward normal to the surface, S is the surface, V is the volume enclosed by the surface.The flux of F into a small sphere of radius 0.01 centered about the point (2,-4,1) is 0.0025.

∴ ∫∫S F.n dS = 0.0025

Let S be the surface of the small sphere of radius 0.01 centered about the point (2,-4,1) and V be the volume enclosed by S.

Then,∫∫S F.n dS = ∫∫∫V div(F) dV

By divergence theorem,

∴ ∫∫S F.n dS = ∫∫∫V div(F) dV = 0.0025

Now, we can say that F is a continuous vector field as it is given. So, by continuity of F,

∴ div(F)(2, -4, 1) = 0.0025/V

where V is the volume enclosed by the small sphere of radius 0.01 centered about the point (2,-4,1).

The volume of a small sphere of radius 0.01 is given by;

V = (4/3) π (0.01)³

= 4.19 x 10⁻⁶

∴ div(F)(2, -4, 1) = 0.0025/4.19 x 10⁻⁶

= 596.18

Therefore, div(F)(2, -4, 1)

= 596.18.

PART B:

To find the circulation of F = -5y i + 5j + 2zk around a circle C of radius 4 centered at (9, 3, 8) in the plane z = 8, oriented counterclockwise when viewed from above, we will use Stokes' Theorem.

So, by Stoke's Theorem, we have;

∫C F.dr = ∫∫S (curl F).n dS

where F is a vector field, C is the boundary curve of S, S is the surface bounded by C, n is a unit normal to the surface, oriented according to the right-hand rule and curl F is the curl of F.

Now, curl F = (2i + 5j + 0k)

So, the surface integral becomes;

∫∫S (curl F).n dS = ∫∫S (2i + 5j + 0k).n dS

As C is a circle of radius 4 centered at (9, 3, 8) in the plane z = 8, oriented counterclockwise when viewed from above,

So, we can take the surface S as the disk with the same center and radius, lying in the plane z = 8 and oriented upwards.

So, the surface integral becomes;

∫∫S (2i + 5j + 0k).n dS = ∫∫S (2i + 5j).n dS

Now, by considering the circle C, we can write (2i + 5j) as;

2cosθ i + 2sinθ j

where θ is the polar angle (angle that the radius makes with the positive x-axis).

Now, we need to parameterize the surface S.

So, we can take;

r(u, v) = (9 + 4 cosv) i + (3 + 4 sinv) j + 8kwhere 0 ≤ u ≤ 2π and 0 ≤ v ≤ 2π

So, the normal vector to S is given by;

r(u, v) = (-4sinv) i + (4cosv) j + 0k

So, the unit normal to S is given by;

r(u, v) / |r(u, v)| = (-sinv)i + (cosv)j + 0k

Now, the surface integral becomes;

∫∫S (2i + 5j).n dS= ∫∫S (2cosθ i + 2sinθ j).(−sinv i + cosv j) dudv

= ∫∫S (−2cosθ sinv + 2sinθ cosv) dudv

= ∫₀²π∫₀⁴ (−2cosu sinv + 2sinu cosv) r dr dv

= −64πTherefore, the circulation of F

= -5y i + 5j + 2zk around a circle C of radius 4 centered at (9, 3, 8) in the plane z = 8, oriented counterclockwise when viewed from above is -64π.

PART C:

To find the circulation of F = -5y + 5j + 2zk around a circle C of radius 4 centered at (9, 3, 8) in the plane z = 8, oriented counterclockwise when viewed from above, we will use Stokes' Theorem.So, by Stoke's Theorem, we have;

∫C F.dr = ∫∫S (curl F).n dS

where F is a vector field, C is the boundary curve of S, S is the surface bounded by C, n is a unit normal to the surface, oriented according to the right-hand rule and curl F is the curl of F.

Now, curl F = (2i + 5j + 0k)

So, the surface integral becomes;

∫∫S (curl F).n dS = ∫∫S (2i + 5j + 0k).n dS

As C is a circle of radius 4 centered at (9, 3, 8) in the plane z = 8, oriented counterclockwise when viewed from above, So, we can take the surface S as the disk with the same center and radius, lying in the plane z = 8 and oriented upwards. So, the surface integral becomes;

∫∫S (2i + 5j + 0k).n dS = ∫∫S (2i + 5j).n dS

Now, by considering the circle C, we can write (2i + 5j) as;

2cosθ i + 2sinθ j

where θ is the polar angle (angle that the radius makes with the positive x-axis).Now, we need to parameterize the surface S. So, we can take; r(u, v) = (9 + 4 cosv) i + (3 + 4 sinv) j + 8kwhere 0 ≤ u ≤ 2π and 0 ≤ v ≤ 2πSo, the normal vector to S is given by;r(u, v) = (-4sinv) i + (4cosv) j + 0kSo, the unit normal to S is given by;r(u, v) / |r(u, v)| = (-sinv)i + (cosv)j + 0kNow, the surface integral becomes;

∫∫S (2i + 5j).n dS= ∫∫S (2cosθ i + 2sinθ j).(−sinv i + cosv j) dudv

= ∫∫S (−2cosθ sinv + 2sinθ cosv) dudv

= ∫₀²π∫₀⁴ (−2cosu sinv + 2sinu cosv) r dr dv

= −64π

Therefore, the circulation of F = -5y + 5j + 2zk around a circle C of radius 4 centered at (9, 3, 8) in the plane z = 8, oriented counterclockwise when viewed from above is -64π.

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The eigenvalues of matrix A are 3 and 1, with corresponding eigenspaces that need to be determined.

To find the eigenvalues of matrix A, we need to solve the characteristic equation det(A - λI) = 0, where λ is the eigenvalue and I is the identity matrix.

By substituting the values from matrix A, we get (a - λ)(a - λ - 3) - 8 = 0. Expanding and simplifying the equation gives λ² - (2a + 3)λ + (a² - 8) = 0. Solving this quadratic equation will yield the eigenvalues, which are 3 and 1.

To find the eigenspace corresponding to each eigenvalue, we need to solve the equations (A - λI)v = 0, where v is the eigenvector. By substituting the eigenvalues into the equation and finding the null space of the resulting matrix, we can obtain a basis for each eigenspace.

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1. The general solution for the Euler [tex]DE ²y + 2xy-6y=0, z > 0[/tex] is given by y=Cr+C which is E.

2. The general solution to the DE y" + 16y = 0 is A. y = C₁ cos(4x) + C₂ sin(4x)

3. The solution is A which is A. e¹-¹²

The form of the Euler differential equation is given as;

[tex]x^2y'' + 2xy' + (x^2 - 6)y = 0[/tex]

By assuming that y = [tex]x^r[/tex].

Substitute that y=[tex]x^r[/tex] into the differential equation, we have;

[tex]x^2r(r - 1) + 2xr + (x^2 - 6)x^r = 0[/tex]

[tex]x^r(r^2 + r - 6) = 0[/tex] ( By factorizing [tex]x^2[/tex])

By characteristic the equation r^2 + r - 6 = 0,

r = -3 and r = 2.

Thus, the general solution to the differential equation is

[tex]y = c1/x^3 + c2x^2[/tex] (c1 and c2 are constants)

Therefore, the answer is (E) y = y=Cr+C.

2. The general solution to the DE y" + 16y = 0 is

The characteristic equation for this differential equation y" + 16y = 0 is  given as

[tex]r^2 + 16 = 0[/tex], where roots r = ±4i.

The roots are complex, hence the general solution involves both sine and cosine functions.

Therefore, the general solution to the differential equation y" + 16y = 0 is given in form of this;

y = c1 cos(4x) + c2 sin(4x)    (c1 and c2 are constants)

Therefore, the answer is (A) y = c1 cos(4x) + c2 sin(4x).

3.

Given that  (y1, y2, y3) is a fundamental set of solutions for the differential equation y" + 3xy' + 4y = 0,  Wronskian of these functions is given by;

[tex]W(y1, y2, y3)(x) = y1(x)y2'(x)y3(x) - y1(x)y3'(x)y2(x) + y2(x)y3'(x)y1(x) - y2(x)y1'(x)y3(x) + y3(x)y1'(x)y2(x) - y3(x)y2'(x)y1(x)[/tex]

if we differentiating the given differential equation y" + 3xy' + 4y = 0 twice, we have this;

[tex]y"' + 3xy" + 6y' + 4y' = 0[/tex]

By substituting y1, y2, and y3 into this equation,  we have;

[tex]W(y1, y2, y3)(x) = (y1(x)y2'(x) - y2(x)y1'(x))(y3(x))'[/tex]

Since W(y1, y2, y3)(0) = e, we have;

[tex]W(y1, y2, y3)(a) = W(y1, y2, y3)(0) e^(-∫0^a (3t) dt)\\= e e^(-3a^2/2)\\= e^(1 - 3a^2/2)[/tex]

Therefore, the answer is (A) [tex]e^(1 - 3a^2/2).[/tex]

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We are given the differential equation y''(x) + (e^x)y'(x) + xy(x) = cos(x) and we need to determine the particular solution up to terms of order O(x^5) in its power series representation about x = 0.

To find the particular solution, we can use the method of power series . We assume that the solution y(x) can be expressed as a power series:

y(x) = ∑(n=0 to ∞) a_n * x^n

where a_n are coefficients to be determined.

Taking the derivatives of y(x), we have:

y'(x) = ∑(n=1 to ∞) n * a_n * x^(n-1)

y''(x) = ∑(n=2 to ∞) n(n-1) * a_n * x^(n-2)

Substituting these expressions into the differential equation and equating coefficients of like powers of x, we can solve for the coefficients a_n.

The equation becomes:

∑(n=2 to ∞) n(n-1) * a_n * x^(n-2) + ∑(n=1 to ∞) n * a_n * x^(n-1) + ∑(n=0 to ∞) a_n * x^n = cos(x)

To determine the particular solution up to terms of order O(x^5), we only need to consider terms up to x^5. We equate the coefficients of x^0, x^1, x^2, x^3, x^4, and x^5 to zero to obtain a system of equations for the coefficients a_n.

Solving this system of equations will give us the values of the coefficients a_n for n up to 5, which will determine the particular solution up to terms of order O(x^5) in its power series representation about x = 0.

Note that the power series representation of the particular solution will involve an infinite number of terms, but we are only interested in the coefficients up to x^5 for this particular problem.

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Let's consider the equation [tex]\(f(x) = x^3 - 2x - 5 = 0\)[/tex] and find the root using Newton's method. We'll choose an initial guess of [tex]\(x_0 = 2\).[/tex]

To apply Newton's method, we need to iterate the following formula until convergence:

[tex]\[x_{n+1} = x_n - \frac{f(x_n)}{f'(x_n)}\][/tex]

where [tex]\(f'(x)\)[/tex] represents the derivative of [tex]\(f(x)\).[/tex]

Let's calculate the derivatives of [tex]\(f(x)\):[/tex]

[tex]\[f'(x) = 3x^2 - 2\][/tex]

[tex]\[f''(x) = 6x\][/tex]

Now, let's proceed with the iteration:

Iteration 1:

[tex]\[x_1 = x_0 - \frac{f(x_0)}{f'(x_0)} = 2 - \frac{(2^3 - 2(2) - 5)}{(3(2)^2 - 2)} = 2 - \frac{3}{8} = \frac{13}{8}\][/tex]

Iteration 2:

[tex]\[x_2 = x_1 - \frac{f(x_1)}{f'(x_1)} = \frac{13}{8} - \frac{\left(\frac{13^3}{8^3} - 2\left(\frac{13}{8}\right) - 5\right)}{3\left(\frac{13}{8}\right)^2 - 2} \approx 2.138\][/tex]

Iteration 3:

[tex]\[x_3 = x_2 - \frac{f(x_2)}{f'(x_2)} \approx 2.136\][/tex]

We can continue the iterations until we achieve the desired level of accuracy. In this case, the approximate solution is [tex]\(x \approx 2.136\),[/tex] which is a root of the equation [tex]\(f(x) = 0\).[/tex]

Please note that the specific choice of the equation and the initial guess were changed, but the overall procedure of Newton's method was followed to find the root.

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The rate at which sand is leaving the bin when the pile is 12 cm high is determined. It involves a conical pile with a height that increases at a given rate and a known relationship between the height and radius.

In this problem, a conical pile of sand is formed as it falls from an overhead bin. The radius of the pile is always three times its height, which can be represented as r = 3h. The volume of a cone is given by V = (1/3)πr²h.

To find the rate at which sand is leaving the bin when the pile is 12 cm high, we need to determine the rate at which the volume of the cone is changing at that instant. We are given that the height of the pile is increasing at a rate of 2 cm/s when the height is 12 cm.

Differentiating the volume equation with respect to time, we obtain dV/dt = (1/3)π[(2r)(dr/dt)h + r²(dh/dt)]. Substituting r = 3h and given that dh/dt = 2 cm/s when h = 12 cm, we can calculate dV/dt.

The resulting value of dV/dt represents the rate at which sand is leaving the bin when the pile is 12 cm high. It signifies the rate at which the volume of the cone is changing, which in turn corresponds to the rate at which sand is being added or removed from the pile at that instant.

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Let's analyze the given information and determine the values of the linear transformation T for different matrices.

From the first equation, we have:

T([10]) = 5.

From the second equation, we have:

T([00]) = 10.

From the third equation, we have:

T([1]) = 15.

From the fourth equation, we have:

T([11]) = 20.

Now, let's find T([4+3[2]]):

Since [4+3[2]] = [10], we can use the information from the first equation to find:

T([4+3[2]]) = T([10]) = 5.

Next, let's find T([1[1]]):

Since [1[1]] = [11], we can use the information from the fourth equation to find:

T([1[1]]) = T([11]) = 20.

Finally, let's find T([8[6]1[1]]):

Since [8[6]1[1]] = [86], we can use the information from the third equation to find:

T([8[6]1[1]]) = T([1]) = 15.

In summary, the values of the linear transformation T for the given matrices are:

T([10]) = 5,

T([00]) = 10,

T([1]) = 15,

T([11]) = 20,

T([4+3[2]]) = 5,

T([1[1]]) = 20,

T([8[6]1[1]]) = 15.

These values satisfy the given equations and determine the behavior of the linear transformation T for the specified matrices.

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Answer: It increases by 12.5 mL per week

Step-by-step explanation:

In summary, we are given the initial value problem 1²y" = 2y with initial conditions y(1) = 2 and y'(1) = 3. We are asked to find the sum A + B such that y(x) = Az^(-1) + B^2 is the solution. The correct answer is (C) A + B = 2.

To solve the initial value problem, we differentiate y(x) twice to find y' and y''. Substituting these derivatives into the given differential equation 1²y" = 2y, we can obtain a second-order linear homogeneous equation. By solving this equation, we find that the general solution is y(x) = Az^(-1) + B^2, where A and B are constants.

Using the initial condition y(1) = 2, we substitute x = 1 into the solution and equate it to 2. Similarly, using the initial condition y'(1) = 3, we differentiate the solution and evaluate it at x = 1, setting it equal to 3. These two equations can be used to determine the values of A and B.

By substituting x = 1 into y(x) = Az^(-1) + B^2, we obtain A + B² = 2. And by differentiating y(x) and evaluating it at x = 1, we get -A + 2B = 3. Solving these two equations simultaneously, we find that A = 1 and B = 1. Therefore, the sum A + B is equal to 2.

In conclusion, the correct answer is (C) A + B = 2.

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the cost function is C(x) = 13x + 30,800 dollars and the revenue function is R(x) = (1,572 − 23x)x dollars. The break-even points are x = 800 and x = 1,200 units. The vertex of the revenue function is (34, 44,776) dollars, representing the maximum revenue. The profit function, P(x), is obtained by subtracting the cost function from the revenue function. The vertex of the profit function is (34, 11,976) dollars, indicating the maximum profit. The price that maximizes the profit is $1,210.

To calculate the cost function, we consider the fixed costs of $30,800 and the variable cost per unit of 13x + 444 dollars. The cost function is given by C(x) = 13x + 30,800, where x is the total number of units produced.

The revenue function is determined by the selling price of the product, which is 1,572 − 23x dollars per unit, multiplied by the number of units x. Thus, the revenue function is R(x) = (1,572 − 23x)x.

The break-even points occur when the revenue equals the cost. By setting R(x) = C(x), we can solve for x to find the break-even points. In this case, the break-even points are x = 800 and x = 1,200 units.

The vertex of the revenue function can be found by using the formula x = -b/(2a), where a and b are the coefficients of the quadratic equation. Plugging in the values, we find that the vertex is located at (34, 44,776) dollars.

The profit function is calculated by subtracting the cost function from the revenue function: P(x) = R(x) - C(x). By finding the vertex of the profit function using the same method as above, we get (34, 11,976) dollars as the maximum profit.

To determine the price that maximizes the profit, we evaluate the revenue function at the x-coordinate of the profit function's vertex. Substituting x = 34 into the revenue function, we find that the price maximizing the profit is $1,210.

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(a) The revenue function R is given by: R = -0.04q^2 + 800q.

(b) R' = -0.08q + 800.

(c) R'(5000) = 400.

(d) P(q) = -0.04q^2 + 600q - 300000.

(e) P' = -0.08q + 600.

(f) P'(5000) = 200, P'(8000) = -320.

(g) The profit function is an inverted parabola with a maximum at the vertex.

Given:

(a) The revenue function R is given by:

R = pq

Revenue = price per unit × quantity demanded

R = pq

R = (-0.04q + 800)q

R = -0.04q^2 + 800q

(b) Marginal revenue is the derivative of the revenue function with respect to q.

R' = dR/dq

R' = d/dq(-0.04q^2 + 800q)

R' = -0.08q + 800

(c) R'(5000) = -0.08(5000) + 800

R'(5000) = 400

At a quantity demanded of 5000 units, the marginal revenue is $400. This means that the revenue will increase by $400 if the quantity demanded is increased from 5000 to 5001 units.

(d) Profit is defined as total revenue minus total cost.

P(q) = R(q) - C(q)

P(q) = -0.04q^2 + 800q - 200q - 300000

P(q) = -0.04q^2 + 600q - 300000

(e) Marginal profit is the derivative of the profit function with respect to q.

P' = dP/dq

P' = d/dq(-0.04q^2 + 600q - 300000)

P' = -0.08q + 600

(f) P'(5000) = -0.08(5000) + 600

P'(5000) = 200

P'(8000) = -0.08(8000) + 600

P'(8000) = -320

(g) The graph of the profit function is a quadratic function with a negative leading coefficient (-0.04). This means that the graph is an inverted parabola that opens downwards. The maximum profit occurs at the vertex of the parabola.

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The rank is 2, the nullity is 2, and the basis of the dimension of the null space is {(-2, 0, 1, 0, 0, 0), (7, -4, 0, 1, -3, 0)}. The null space of a matrix A is the set of all solutions to the homogeneous equation Ax=0.

The rank, nullity, and basis of the dimension of the null space of the matrix -1 2 9 4 5 -3 3 -7 201 4 A=2 -5 2 4 6 4 -9 2 -4 -4 1 7 can be found as follows:

The augmented matrix [A | 0] is {-1, 2, 9, 4, 5, -3, 3, -7, 201, 4, 2, -5, 2, 4, 6, 4, -9, 2, -4, -4, 1, 7 | 0}, which we'll row-reduce by performing operations on rows, to get the reduced row-echelon form. We get

{-1, 2, 9, 4, 5, -3, 3, -7, 201, 4, 2, -5, 2, 4, 6, 4, -9, 2, -4, -4, 1, 7 | 0}-> {-1, 2, 9, 4, 5, -3, 0, -1, -198, 6, 0, 0, 0, 1, -2, -3, 7, 3, -4, 0, 0, 0 | 0}-> {-1, 2, 0, -1, -1, 0, 0, -1, 190, 6, 0, 0, 0, 1, -2, -3, 7, 3, -4, 0, 0, 0 | 0}-> {-1, 0, 0, 1, 1, 0, 0, 3, -184, -2, 0, 0, 0, 0, 1, -1, 4, 0, -7, 0, 0, 0 | 0}-> {-1, 0, 0, 0, 0, 0, 0, 0, 6, -2, 0, 0, 0, 0, 1, -1, 4, 0, -7, 0, 0, 0 | 0}

We observe that the fourth and seventh columns of the matrix have pivots, while the remaining columns do not. This implies that the rank of the matrix A is 2, and the nullity is 4-2 = 2.

The basis of the dimension of the null space can be determined by assigning the free variables to arbitrary values and solving for the pivot variables. In this case, we assign variables x3 and x6 to t and u, respectively. Hence, the solution set can be expressed as

{x1 = 6t - 2u, x2 = t, x3 = t, x4 = -4t + 7u, x5 = -3t + 4u, x6 = u}. Therefore, the basis of the dimension of the null space is given by{(-2, 0, 1, 0, 0, 0), (7, -4, 0, 1, -3, 0)}.

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the given Laplace transform is,L^−1 { (2/s − 1/s^3) }^2= 2u(t) * 2u(t) − t^2/2= 4u(t) - t^2/2Hence, the answer is 4u(t) - t^2/2.

Given Laplace Transform is,L^−1 { (2/s − 1/s^3) }^2

The inverse Laplace transform of the above expression is given by the formula:

L^-1 [F(s-a)/ (s-a)] = e^(at) L^-1[F(s)]

Now let's solve the given expression

,L^−1 { (2/s − 1/s^3) }^2= L^−1 { 2/s − 1/s^3 } x L^−1 { 2/s − 1/s^3 }

On finding the inverse Laplace transform for the two terms using the Laplace transform table, we get, L^-1(2/s) = 2L^-1(1/s) = 2u(t)L^-1(1/s^3) = t^2/2

Therefore the given Laplace transform is,L^−1 { (2/s − 1/s^3) }^2= 2u(t) * 2u(t) − t^2/2= 4u(t) - t^2/2Hence, the answer is 4u(t) - t^2/2.

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The calculated value of cos θ is -9/41 if the angle θ terminates in quadrant II

From the question, we have the following parameters that can be used in our computation:

tan θ = -40/9

We start by calculating the hypotenuse of the triangle using the following equation

h² = (-40)² + 9²

Evaluate

h² = 1681

Take the square root of both sides

h = ±41

Given that the angle θ terminates in quadrant II, then we have

h = 41

So, we have

cos θ = -9/41

Hence, the value of cos θ is -9/41

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Question

Given that tan θ = -40/9​ and that angle θ terminates in quadrant II, then what is the value of cosθ?

There are two possible coordinates for point P(a, 0) on the x-axis such that |PA| = |PB|: P(7, 0) and P(3, 0).

To find the coordinates of point P(a, 0) on the x-axis such that |PA| = |PB|, we need to find the value of 'a' that satisfies this condition.

Let's start by finding the distances between the points. The distance between two points (x1, y1) and (x2, y2) is given by the distance formula:

d = √((x2 - x1)² + (y2 - y1)²)

Using this formula, we can calculate the distances |PA| and |PB|:

|PA| = √((a - 5)² + (0 - 0)²) = √((a - 5)²)

|PB| = √((0 - 0)² + (2 - 0)²) = √(2²) = 2

According to the given condition, |PA| = |PB|, so we can equate the two expressions:

√((a - 5)²) = 2

To solve this equation, we need to square both sides to eliminate the square root:

(a - 5)² = 2²

(a - 5)² = 4

Taking the square root of both sides, we have:

a - 5 = ±√4

a - 5 = ±2

Solving for 'a' in both cases, we get two possible values:

Case 1: a - 5 = 2

a = 2 + 5

a = 7

Case 2: a - 5 = -2

a = -2 + 5

a = 3

Therefore, there are two possible coordinates for point P(a, 0) on the x-axis such that |PA| = |PB|: P(7, 0) and P(3, 0).

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The time rate of change of the rabbit population, denoted as dP/dt, is proportional to the square root of the population, √P. We can express this relationship mathematically as dP/dt = k√P, where k is the proportionality constant.

Given that the population at time t=0 is 100 rabbits and is increasing at a rate of 20 rabbits per month, we can use this information to determine the value of k. At t=0, P=100, and dP/dt = 20. Plugging these values into the differential equation, we have 20 = k√100, which gives us k = 2.

To find the population one and a half years (18 months) later, we can integrate the differential equation. ∫(1/√P) dP = ∫2 dt. Integrating both sides, we get 2√P = 2t + C, where C is the constant of integration.

At t=0, P=100, so we can solve for C: 2√100 = 2(0) + C, which gives us C = 20.

Plugging t=18 into the equation 2√P = 2t + C, we have 2√P = 2(18) + 20, which simplifies to √P = 38.

Squaring both sides, we get P = 38^2 = 1444.

Therefore, one and a half years later, the rabbit population will be 1444 rabbits.

Thus, the correct answer is d. 484 rabbits.

Learn more about differential equation here: brainly.com/question/25731911

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