Name: CA #1 wiem, sketch the area bounded by the equations and revolve it around the axis indicat d. Find Ae volume of the solid formed by this revolution. A calculator is allowed, so round to three decimal places. 1. y = x2 + 4, x = -1, x = 1, and y = 3. Revolve | 2. y = * = 4, and y = 3. Revolve around the y- around the x-axis. axis 2 - y = x2 and y = 2x. Revolve around the x-axis. 4. Same region as #3, but revolve around the y-axis.

The given indefinite integral ∫(ez + 3) da can be transformed into a basic integral by performing the substitution u = ez + 3 and du = dz. After substituting, we have the integral ∫du. Integrating ∫du gives the result of u + C, where C is the constant of integration.

To solve the given indefinite integral ∫(ez + 3) da, we can simplify it by performing a substitution. Let u = ez + 3. Taking the derivative of u with respect to a, we have du = (d/dz)(ez + 3) da = ez da. Rearranging, we get du = ez da.Substituting u and du into the integral, we have ∫du. This is now a basic integral with respect to u. Integrating ∫du gives us the result of u + C, where C is the constant of integration.Therefore, the final result of the given indefinite integral is u + C, which can be expressed as (ez + 3) + C.

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The derivative of f(x) = 8x³ - Vex + T + abx + c, found using first principles, is f'(x) = 24²2 + ab. This derivative represents the rate of change of the function with respect to x.

To find the derivative of the function f(x) = 8x³ - Vex + T + abx + c using first principles, we need to apply the definition of the derivative:

f'(x) = lim(h->0) [f(x+h) - f(x)] / h

Let's calculate it step by step

Replace f(x) with the given function:

f'(x) = lim(h->0) [(8(x+h)³ - Vex+h + T + ab(x+h) + c) - (8x³ - Vex + T + abx + c)] / h

Expand and simplify:

f'(x) = lim(h->0) [8(x³ + 3x²h + 3xh² + h³) - Vex+h + T + abx + abh + c - 8x^3 + Vex - T - abx - c] / h

Cancel out common terms:

f'(x) = lim(h->0) [8(3x²h + 3xh² + h³) + abh] / h

Distribute 8 into the terms inside the parentheses:

f'(x) = lim(h->0) [24x²h + 24xh² + 8h³ + abh] / h

Simplify and factor out h

f'(x) = lim(h->0) [h(24x² + 24xh + 8h² + ab)] / h

Cancel out h:

f'(x) = lim(h->0) 24x² + 24xh + 8h² + ab

Take the limit as h approaches 0:

f'(x) = 24x² + ab

Therefore, the derivative of f(x) = 8x³ - Vex + T + abx + c from first principles is f'(x) = 24x² + ab.

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The largest possible volume for the rectangular box is approximately 160.57 cubic inches. Let x be the side of the square base and h be the height of the rectangular box.

The surface area of the base and four sides is:

SA = x² + 4xh

The volume of the rectangular box is:

V = x²h

We want to maximize the volume of the box subject to the constraint that the surface area is 164 square inches. That is  

SA = x² + 4xh = 164

Therefore:h = (164 - x²) / 4x

We can now substitute this expression for h into the formula for the volume:

V = x²[(164 - x²) / 4x]

Simplifying this expression, we get:V = (1 / 4)x(164x - x³)

We need to find the maximum value of this function. Taking the derivative and setting it equal to zero, we get:dV/dx = (1 / 4)(164 - 3x²) = 0

Solving for x, we get

x = ±√(164 / 3)

We take the positive value for x since x represents a length, and the side length of a box must be positive. Therefore:x = √(164 / 3) ≈ 7.98 inches

To find the maximum volume, we substitute this value for x into the formula for the volume:V = (1 / 4)(√(164 / 3))(164(√(164 / 3)) - (√(164 / 3))³)V ≈ 160.57 cubic inches

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The particular antiderivative of C'(x) = 4x^2 - 2x that satisfies the condition C(0) = 5,000 is C(x) = (4/3)x^3 - (2/2)x^2 + 5,000.

To find the particular antiderivative C(x) of the derivative C'(x) = 4x^2 - 2x, we integrate the derivative with respect to x.

The antiderivative of 4x^2 - 2x with respect to x is given by the power rule of integration. For each term, we add 1 to the exponent and divide by the new exponent. So, the antiderivative becomes:

C(x) = (4/3)x^3 - (2/2)x^2 + C

Here, C is the constant of integration.

To find the particular antiderivative that satisfies the given condition C(0) = 5,000, we substitute x = 0 into the antiderivative equation:

C(0) = (4/3)(0)^3 - (2/2)(0)^2 + C

C(0) = 0 + 0 + C

C(0) = C

We know that C(0) = 5,000, so we set C = 5,000:

C(x) = (4/3)x^3 - (2/2)x^2 + 5,000

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I'll evaluate each of these integrals:

1.[tex]∫ sec^2(x) tan(x) dx[/tex]: This is a straightforward integral using u-substitution. [tex]Let u = sec(x).[/tex] Then, [tex]du/dx = sec(x)tan(x), so du = sec(x)tan(x) dx.[/tex] Substitute to obtain [tex]∫ u^2 du,[/tex]which integrates to[tex](1/3)u^3 + C[/tex]. Substitute back [tex]u = sec(x)[/tex]to get the final answer: [tex](1/3) sec^3(x) + C[/tex].

2. [tex]∫ sec^4(x) tan(x) dx:[/tex] This integral is more complex. A possible approach is to use integration by parts and reduction formulas. This is beyond a quick explanation, so it's suggested to refer to an advanced calculus resource.

3.[tex]∫ (3x(x^2+1) - 2x(x^2+1))/(x^2+1)^2 dx[/tex]: This simplifies to[tex]∫ (x/(x^2+1)) dx = ∫[/tex] [tex]du/u^2 = -1/u + C, where u = x^2 + 1.[/tex] So, the final result is -1/(x^2+1) + C.

4. [tex]∫ (2x^3 + sin(x) - 3x^3 + tan(x)) dx:[/tex] This can be split into separate integrals: [tex]∫2x^3 dx - ∫3x^3 dx + ∫sin(x) dx + ∫tan(x) dx[/tex]. The result is [tex](1/2)x^4 - (3/4)x^4 - cos(x) - ln|cos(x)| + C.[/tex]

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To evaluate the work done by the force field F = (2xy² + 3xz², 2x²y + 2y, 3x²z), we need to compute the line integral of F along the path C from (0,1,0) to (2,3,2).

The line integral of a vector field F along a curve C is given by the formula:

∫ F · dr = ∫ (F₁dx + F₂dy + F₃dz),

where dr is the differential vector along the curve C.

Parametrize the curve C as r(t) = (2t, 1+t, 2t), where t ranges from 0 to 1. Taking the derivatives, we find dr = (2dt, dt, 2dt).

Substituting these values into the line integral formula, we have:

∫ F · dr = ∫ ((2xy² + 3xz²)dx + (2x²y + 2y)dy + (3x²z)dz)

          = ∫ (4ty² + 6tz² + 2(1+t)dt + 6t²zdt + 6t²dt)

          = ∫ (4ty² + 6tz² + 2 + 2t + 6t²z + 6t²)dt

          = ∫ (6t² + 4ty² + 6tz² + 2 + 2t + 6t²z)dt.

Integrating term by term, we get:

∫ (6t² + 4ty² + 6tz² + 2 + 2t + 6t²z)dt = 2t³ + (4/3)ty³ + 2tz² + 2t² + t²z + 2t³z.

Evaluating this expression from t = 0 to t = 1, we find:

∫ F · dr = 2(1)³ + (4/3)(1)(1)³ + 2(1)(2)² + 2(1)² + (1)²(2) + 2(1)³(2)

          = 2 + (4/3) + 8 + 2 + 2 + 16

          = 30/3 + 16

          = 10 + 16

          = 26.

Therefore, the work done by the force field F in moving the object along the path C is 26 units.

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Naya's gross annual income is approximately $46,416.67.

To determine Naya's gross annual income, we need to reverse engineer the tax calculation based on the given information.

Let's denote Naya's gross annual income as G. We know that Naya's net annual income, after income tax, is 36,560. We also know that Naya pays income tax at the same rates and has the same annual tax credits as Emma.

Emma pays income tax on her taxable income at a rate of 20% on the first 35,300 and 40% on the balance. She has annual tax credits of 1,650.

Based on this information, we can set up the following equation:

G - (0.2 * 35,300) - (0.4 * (G - 35,300)) = 36,560 - 1,650

Let's solve this equation step by step:

G - 7,060 - 0.4G + 14,120 = 34,910

Combining like terms, we have:

0.6G + 7,060 = 34,910

Subtracting 7,060 from both sides:

0.6G = 27,850

Dividing both sides by 0.6:

G = 27,850 / 0.6

G ≈ 46,416.67

Therefore, Naya's gross annual income is approximately $46,416.67.

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The area of the surface given by z = f(x,y) that lies above the region R is (16/3) √51. To find the area of the surface given by z = f(x,y) that lies above the region R, we can use the formula for surface area: A = ∫∫√(1 +(f_x)^2 + (f_y)^2) dA

In this case, we have: f(x, y) = 5x + 5y

f_x = 5

f_y = 5

We also have the region R, which is the triangle with vertices (0, 0), (4,0), and (0, 4). To set up the integral, we need to find the limits of integration for x and y. Since the triangle has vertices at (0, 0), (4,0), and (0, 4), we can set up the integral as follows:

A = ∫∫√(1 + (f_x)^2 + (f_y)^2) dA

A = ∫_0^4 ∫_0^(4-x) √(1 + 5^2 + 5^2) dy dx

A = ∫_0^4 √51(4-x) dx

A = √51 ∫_0^4 (4-x)^(1/2) dx. To evaluate this integral, we can use the substitution u = 4-x, which gives us: du = -dx

x = 0 => u = 4

x = 4 => u = 0

Substituting these limits and the expression for x in terms of u into the integral, we get: A = √51 ∫_4^0 u^(1/2) (-du)

A = √51 ∫_0^4 u^(1/2) du

A = √51 (2/3) u^(3/2) |_0^4

A = (2/3) √51 (4^(3/2) - 0)

A = (2/3) √51 (8)

A = (16/3) √51

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The solution set of the given system is {x = 0, x2 = 4a, x3 = -2a}, where 'a' represents an arbitrary number. The given system of equations can be solved using Gaussian elimination.

The solution set of the system is {x = 0, x2 = 4a, x3 = -2a}, where 'a' represents an arbitrary number.

To solve the system using Gaussian elimination, we perform row operations to transform the augmented matrix into row-echelon form. The resulting matrix will reveal the solution to the system.

Step 1: Write the augmented matrix for the given system:

```

1  -1  4 | 0

-2  1   1 | 0

```

Step 2: Perform row operations to achieve row-echelon form:

R2 = R2 + 2R1

```

1  -1   4 | 0

0  -1   9 | 0

```

Step 3: Multiply R2 by -1:

```

1  -1   4 | 0

0   1  -9 | 0

```

Step 4: Add R1 to R2:

R2 = R2 + R1

```

1  -1   4 | 0

0   0  -5 | 0

```

Step 5: Divide R2 by -5:

```

1  -1   4 | 0

0   0   1 | 0

```

Step 6: Subtract 4 times R2 from R1:

R1 = R1 - 4R2

```

1  -1   0 | 0

0   0   1 | 0

```

Step 7: Subtract R1 from R2:

R2 = R2 - R1

```

1  -1   0 | 0

0   0   1 | 0

```

Step 8: The resulting matrix is in row-echelon form. Rewriting the system in equation form:

```

x - x2 = 0

x3 = 0

```

Step 9: Solve for x and x2:

From equation 2, we have x3 = 0, which means x3 can be any value.

From equation 1, we substitute x3 = 0:

x - x2 = 0

x = x2

Therefore, the solution set is {x = 0, x2 = 4a, x3 = -2a}, where 'a' represents an arbitrary number.

In summary, the solution set of the given system is {x = 0, x2 = 4a, x3 = -2a}, where 'a' represents an arbitrary number.

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To find the minimum rate of change, or the smallest directional derivative, of the function f(x, y) = x + ln(xy) at the point (1, 1), we need to calculate the directional derivatives in different directions and determine the smallest value. The correct option will be provided after the explanation. To find the value of f(3, 1) - f(0, 1), we substitute the given values into the function f(x, y) and compute the difference.

The directional derivative of a function represents the rate of change of the function in a specific direction. To find the minimum rate of change at the point (1, 1) for f(x, y) = x + ln(xy), we calculate the directional derivatives in different directions and compare them. The correct option cannot be determined without performing the calculations. To find the value of f(3, 1) - f(0, 1), we substitute x = 3 and y = 1 into the function f(x, y) = x + ln(xy). Then we subtract the value of f(0, 1) by substituting x = 0 and y = 1. Evaluating these expressions will provide the result of /(3, 1) - f(0, 1).

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The rate at which the distance between the two cars is changing at the instant when the first car's speed is 11 ft/sec, 5 seconds after leaving the intersection, is 9 ft/sec.

Let's denote the distance between the first car and the intersection as x and the distance between the second car and the intersection as y. We are given that at time t, y = t + 4t ft.

At the instant when the first car's speed is 11 ft/sec, 5 seconds after leaving the intersection, we have x = 30 ft and y = 11 × 5 = 55 ft.

The distance between the two cars, D, is given by the Pythagorean theorem: D = √(x² + y²).

Taking the derivative of D with respect to time, we get dD/dt = (dD/dx) × (dx/dt) + (dD/dy) × (dy/dt).

Since dx/dt represents the speed of the first car, which is constant at 11 ft/sec, and dy/dt represents the rate at which the second car's position changes, which is 1 + 4 = 5 ft/sec, the equation simplifies to dD/dt = (dD/dx) × 11 + (dD/dy) × 5.

To find dD/dt, we differentiate D = √(x² + y²) with respect to x and y, respectively. By substituting the values x = 30 and y = 55, we find dD/dt = (30/√305) × 11 + (55/√305) × 5 ≈ 9 ft/sec. Therefore, the rate at which the distance between the two cars is changing at that instant of time is approximately 9 ft/sec.

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Complete question:

A car leaves an intersection traveling west. Its position 5 sec later is 30 ft from the intersection. At the same time, another car leaves the same intersection heading north so that its position t sec later is y = t + 4t ft from the intersection. If the speed of the first car 5 sec after leaving the intersection is 11 ft/sec, find the rate at which the distance between the two cars is changing at that instant of time.

a) The critical points of the equation are (-2, 66) and (2, -66).

b) The interval of increase is (-∞, -2) U (2, ∞), and the interval of decrease is (-2, 2).

c) The relative minimum is (-2, 66), and the relative maximum is (2, -66).

d) There are no inflection points in the equation.

e) The concave is upward for the entire graph.

The given equation is y = 3x⁴ - 24x³ + 32 - 24x + 54x + 4.

To determine its critical points, we find the values of x where the derivative of y equals zero.

By taking the derivative, we obtain 12x³ - 72x² - 24, which can be factored as 12(x - 2)(x + 2)(x - 1).

Thus, the critical points are (-2, 66) and (2, -66).

Analyzing the derivative further, we observe that it is positive in the intervals (-∞, -2) and (2, ∞), indicating an increasing function, and negative in the interval (-2, 2), suggesting a decreasing function.

The relative minimum occurs at (-2, 66), and the relative maximum at (2, -66).

There are no inflection points in the equation, and the concave is upward for the entire graph.

The critical points of a function are the points where the derivative is either zero or undefined.

In this case, we found the critical points by setting the derivative of the equation equal to zero. The interval of increase represents the x-values where the function is increasing, while the interval of decrease represents the x-values where the function is decreasing.

The relative minimum and maximum are the lowest and highest points on the graph, respectively, within a specific interval. Inflection points occur where the concavity of the graph changes, but in this equation, no such points exist. The concave being upward means that the graph curves in a U-shape.

Understanding these characteristics helps us analyze the behavior of the equation and its graphical representation.

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To determine f'(x) for the function f(x) = 4x + 7 using the definition of the derivative, the Newton quotient is computed and simplified to eliminate h in the denominator.

The derivative of a function f(x) can be found using the definition of the derivative, which involves the Newton quotient. For the function f(x) = 4x + 7, we calculate f'(x) by evaluating the Newton quotient.

The Newton quotient is given by (f(x + h) - f(x)) / h, where h represents a small change in x.

Substituting f(x) = 4x + 7 into the Newton quotient, we have [(4(x + h) + 7) - (4x + 7)] / h.

Simplifying the expression inside the numerator, we get (4x + 4h + 7 - 4x - 7) / h.

Canceling out the terms that have opposite signs, we are left with (4h) / h.

Now, we can cancel out the h in the numerator and denominator, resulting in the derivative f'(x) = 4.

Therefore, the derivative of the function f(x) = 4x + 7 with respect to x, denoted as f'(x), is equal to 4.

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The linear function in this table is given as follows:

y = 0.2667x + 4.

The slope-intercept equation for a linear function is presented as follows:

y = mx + b

In which:

When x = 0, y = 4, hence the intercept b is given as follows:

b = 4.

When x increases by 60, y increases by 16, hence the slope m is given as follows:

m = 16/60

m = 0.2667.

Hence the equation is given as follows:

y = 0.2667x + 4.

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The surface area of the balloon is changing at a rate of 192π square inches per minute when the radius is 12 inches. In other words, it is changing at a rate of 0.0053 in/min.

To find how fast the surface area is changing with respect to time, we need to use the formula for the surface area of a sphere.

The formula for the surface area (A) of a sphere with radius (r) is given by:

A = 4πr^2.

Given that the rate of change of the radius (dr/dt) is 2 in/min, we want to find the rate of change of the surface area (dA/dt) when the radius is 12 inches.

Differentiating the equation for the surface area with respect to time, we have:

dA/dt = d(4πr^2)/dt.

Using the power rule of differentiation, we get:

dA/dt = 8πr(dr/dt).

Substituting the given values, when r = 12 inches and dr/dt = 2 in/min, we have:

dA/dt = 8π(12)(2) = 192π in^2/min.

Therefore, the surface area of the balloon is changing at a rate of 192π square inches per minute when the radius is 12 inches.

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The volume of the rectangular prism would be = 385 in³.

To calculate the volume of the prism, the formula that should be used would be given below as follows:

Volume of rectangular prism;

Volume of rectangular prism;= length×width×height.

But length×width = base area

Volume = Base area × height.

where;

base area = 35in²

height = 11in

Volume = 35×11= 385 in³

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The value of the limit is equal to the value of the function at a = -1, we can conclude that the function f(x) = (x + 2a³) is continuous at a = -1.

Let's start with problem 13.

Given function:

[tex]f(a) = (x + 2a³), a = -1[/tex]

To show that the function is continuous at a = -1, we need to evaluate the following limit:

[tex]lim(x→a) f(x) = f(-1) = (-1 + 2(-1)³)[/tex]

First, let's simplify the expression:

[tex]f(-1) = (-1 + 2(-1)³)= (-1 + 2(-1))= (-1 - 2)= -3[/tex]

Therefore, we have determined the value of the function at a = -1 as -3.

Now, let's evaluate the limit as x approaches -1:

[tex]lim(x→-1) f(x) = lim(x→-1) (x + 2(-1)³)[/tex]

Substituting x = -1:

[tex]lim(x→-1) f(x) = lim(x→-1) (-1 + 2(-1)³)= lim(x→-1) (-1 + 2(-1))= lim(x→-1) (-1 - 2)= lim(x→-1) (-3)= -3[/tex]

Since the value of the limit is equal to the value of the function at a = -1, we can conclude that the function f(x) = (x + 2a³) is continuous at a = -1.

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The order 3 Taylor polynomial for the function \(f(x) = 3x + 16\) is given by T3(x)=16+3x using exact values.

To find the order 3 Taylor polynomial \(T_3(x)\) for the function \(f(x) = 3x + 16\), we need to calculate the function's derivatives up to the third order and evaluate them at the center \(c = 0\). The formula for the Taylor polynomial is:

\[T_3(x) = f(0) + f'(0)x + \frac{f''(0)}{2!}x^2 + \frac{f'''(0)}{3!}x^3\]

Let's find the derivatives of \(f(x)\):

\[f'(x) = 3\]

\[f''(x) = 0\]

\[f'''(x) = 0\]

Now, let's evaluate these derivatives at \(x = 0\):

\[f(0) = 3(0) + 16 = 16\]

\[f'(0) = 3\]

\[f''(0) = 0\]

\[f'''(0) = 0\]

Substituting these values into the formula for the Taylor polynomial, we get:

\[T_3(x) = 16 + 3x + \frac{0}{2!}x^2 + \frac{0}{3!}x^3\]

Simplifying further:

\[T_3(x) = 16 + 3x\]

Therefore ,The order 3 Taylor polynomial for the function \(f(x) = 3x + 16\) is given by T3(x)=16+3x using exact values.

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The Maclaurin series for e^x is a mathematical representation of the exponential function. It allows us to approximate the value of e^x using a series of terms. The Maclaurin series for e^x is expressed in sigma notation, which represents the sum of terms with increasing powers of x.

The Maclaurin series for e^x can be derived using the Taylor series expansion. The Taylor series expansion of a function represents the function as an infinite sum of terms involving its derivatives evaluated at a specific point. For e^x, the Taylor series expansion is particularly simple and can be expressed as:

e^x = 1 + x + (x^2)/2! + (x^3)/3! + (x^4)/4! + ...

In sigma notation, the Maclaurin series for e^x can be written as:

e^x = ∑ [(x^n)/n!]

Here, the symbol ∑ denotes the sum, n represents the index of the terms, and n! denotes the factorial of n. The series continues indefinitely, with each term involving higher powers of x divided by the factorial of the corresponding index.

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1. Using Newton's method, the only critical number of the function f(x) = ln(1 + x - x^2 + x^3) is approximately 0.789813.

2. The equation of the line passing through the point (3,5) that cuts off the least area from the first quadrant is y = -(5/3)x + 20/3.

3. The function f(x) = sin(x^2) - 137x + 231 is the function that passes through the point (137, 0) and has a derivative function of f'(x) = 12x cos(x^2).

To find the critical number of the function f(x) = ln(1 + x - x^2 + x^3), we can apply Newton's method.

The derivative of f(x) is given by f'(x) = (1 - 2x + 3x^2) / (1 + x - x^2 + x^3). By iteratively applying Newton's method with an initial guess, we can approximate the critical number. The process continues until we reach the desired level of accuracy. In this case, the critical number is approximately 0.789813.

To find the line passing through the point (3,5) that cuts off the least area from the first quadrant, we need to minimize the area of the triangle formed by the line, the x-axis, and the y-axis.

The equation of a line passing through (3,5) can be written as y = mx + c, where m represents the slope and c is the y-intercept. By minimizing the area of the triangle, we minimize the product of the base and height.

This occurs when the line is perpendicular to the x-axis, resulting in the least area. Therefore, the line equation is y = -(5/3)x + 20/3.

To find the function f(x) that passes through the point (137, 0) and has a derivative function of f'(x) = 12x cos(x^2), we integrate the derivative function with respect to x.

Integrating f'(x) gives us f(x) = sin(x^2) - 137x + C, where C is the constant of integration. To determine the value of C, we substitute the given point (137, 0) into the equation. This gives us 0 = sin(137^2) - 137(137) + C, which allows us to solve for C. The resulting function is f(x) = sin(x^2) - 137x + 231.

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1. The concavity is constant

2. the arc length of curve is ∫[0, π/2] √[18 - 18(cosθcos3θ + sinθsin3θ)] dθ

3. The equation in rectangular coordinates are

x = (ρ/2)cosθ

y = (ρ/2)sinθ

z = (√3/2)ρ

1. To find the slope and concavity at θ = π/6 for the curve x = [tex]sin^3\theta\\[/tex], y = [tex]cos^3\theta[/tex], we can differentiate the equations with respect to θ and evaluate the derivatives at the given angle.

Differentiating x = [tex]sin^3\theta[/tex] and y = [tex]cos^3\theta[/tex] with respect to θ, we get:

dx/dθ =[tex]3sin^2\theta cos\theta[/tex]

dy/dθ = [tex]-3cos^2\theta sin\theta[/tex]

To find the slope at θ = π/6, we substitute θ = π/6 into the derivatives:

dx/dθ =[tex]3sin^2(\pi/6)cos(\pi/6)[/tex] = (3/4)(√3/2) = (3√3)/8

dy/dθ = [tex]-3cos^2(\pi/6)sin(\pi /6)[/tex] = -(3/4)(1/2) = -3/8

So, the slope at θ = π/6 is (3√3)/8 for x and -3/8 for y.

To find the concavity at θ = π/6, we need to differentiate the slopes with respect to θ:

d²x/dθ² = d/dθ[(3√3)/8] = 0 (constant)

d²y/dθ² = d/dθ[-3/8] = 0 (constant)

Therefore, the concavity at θ = π/6 is constant (neither concave up nor concave down).

2. To find the arc length of the curve x = 3sinθ - sin3θ, y = 3cosθ - cos3θ, where 0 ≤ θ ≤ π/2, we can use the arc length formula for parametric curves:

Arc length = ∫[a,b] sqrt[(dx/dθ)² + (dy/dθ)²] dθ

In this case, a = 0 and b = π/2. We need to find dx/dθ and dy/dθ:

dx/dθ = 3cosθ - 3cos3θ

dy/dθ = -3sinθ + 3sin3θ

Now, we can substitute these derivatives into the arc length formula and integrate:

Arc length =[tex]\int_0^{\pi/2} \sqrt{(3cos\theta - 3cos3\theta)^2 + (-3sin\theta + 3sin3\theta)^2} d\theta[/tex]

Using trigonometric identities, we have:

(3cosθ - 3cos3θ)² + (-3sinθ + 3sin3θ)²

= 9cos²θ - 18cosθcos3θ + 9cos²3θ + 9sin²θ - 18sinθsin3θ + 9sin²3θ

= 9(cos²θ + sin²θ) + 9(cos²3θ + sin²3θ) - 18(cosθcos3θ + sinθsin3θ)

Using the Pythagorean identity (cos²θ + sin²θ = 1) and the triple-angle formulas (cos³θ = (cosθ)³ - 3cosθ(1 - (cosθ)²) and sin³θ = 3sinθ - 4(sinθ)³), we can simplify further:

= 9 + 9 - 18(cosθcos3θ + sinθsin3θ)

= 18 - 18(cosθcos3θ + sinθsin3θ)

Now, the integral becomes:

∫[0, π/2] √[18 - 18(cosθcos3θ + sinθsin3θ)] dθ

This integral represents the arc length of the curve x = 3sinθ - sin3θ, y = 3cosθ - cos3θ, from θ = 0 to θ = π/2.

3. To find an equation in rectangular coordinates for the surface represented by the spherical equation ϕ = π/6, we can use the spherical-to-rectangular coordinate conversion formulas:

x = ρsinϕcosθ

y = ρsinϕsinθ

z = ρcosϕ

In this case, the spherical equation is given as ϕ = π/6. Substituting ϕ = π/6 into the conversion formulas, we have:

x = ρsin(π/6)cosθ = (ρ/2)cosθ

y = ρsin(π/6)sinθ = (ρ/2)sinθ

z = ρcos(π/6) = (√3/2)ρ

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The given limit of Riemann sums represents the definite integral of a function f on the interval [a, b]. The function f can be identified as f(x) = x². The limit can be expressed as ∫[a, b] x² dx.

The given limit is written as:

lim(n→∞) Σ[xk * Δxk] from k=1 to n.

This limit represents the Riemann sum of a function f on the interval [a, b], where Δxk is the width of each subinterval and xk is a sample point within each subinterval.

Comparing this limit with the definite integral notation, we can identify f(x) as f(x) = x².

Therefore, the given limit can be expressed as the definite integral:

∫[a, b] x² dx.

In this case, the limits of integration [a, b] are not specified, so they can be any valid interval over which the function f(x) = x² is defined.

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The flux of the vector field F = (y, -2, 2) across the part of the plane

z = 1+ 4x + 3y above the rectangle (0, 3) x (0,4) with upwards orientation is 96 Wb.

To find the flux of the vector field F = (y, -2, 2) across the given surface, we can use the surface integral formula. The flux (Φ) of a vector field across a surface S is given by:

Φ = ∬S F · dS

where F is the vector field, dS is the outward-pointing vector normal to the surface, and the double integral is taken over the surface S.

In this case, the surface S is the part of the plane z = 1 + 4x + 3y above the rectangle (0, 3) × (0, 4).

Let's parameterize the surface S. Let's introduce two parameters u and v to represent the coordinates on the rectangle. We can define the position vector r(u, v) = ( x(u, v), y(u, v), z(u, v) ) as follows:

x(u, v) = u

y(u, v) = v

z(u, v) = 1 + 4u + 3v

Next, we calculate the partial derivatives of r(u, v) with respect to u and v:

∂r/∂u = (1, 0, 4)

∂r/∂v = (0, 1, 3)

Now, we can calculate the cross product of the partial derivatives:

∂r/∂u × ∂r/∂v = (-4, -3, 1)

The magnitude of this cross product is the area of the parallelogram defined by ∂r/∂u and ∂r/∂v, which is √((-4)^2 + (-3)^2 + 1^2) = √26.

To find the flux Φ, we integrate the dot product of F and the outward-pointing vector dS over the surface S:

Φ = ∬S F · dS = ∬S (y, -2, 2) · (∂r/∂u × ∂r/∂v) du dv

Since the outward-pointing vector is ∂r/∂u × ∂r/∂v = (-4, -3, 1), we have:

Φ = ∬S (y, -2, 2) · (-4, -3, 1) du dv

  = ∬S (-4y + 6 + 2) du dv

  = ∬S (-4y + 8) du dv

The limits of integration are u = 0 to 3 and v = 0 to 4, representing the rectangle (0, 3) × (0, 4). Therefore, the integral becomes:

Φ = ∫₀³ ∫₀⁴ (-4y + 8) dv du

Now, let's evaluate the integral:

Φ = ∫₀³ ∫₀⁴ (-4y + 8) dv du

  = ∫₀³ [-4yv + 8v]₀⁴ du

  = ∫₀³ (-16y + 32) du

  = [-16yu + 32u]₀³

  = -48y + 96

Finally, we substitute the limits of integration for y:

Φ = -48y + 96 = -48 *4  + 96 = -192 + 96 = -96

Thus, the required flux is 96 Wb

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Answer:

40%

Step-by-step explanation:

Solution to the given initial value problem is y = 9e^7x + 63e^49

To solve the initial value problem dy/dx = 9e^7, y(-7) = 0, we can integrate both sides of the equation with respect to x and apply the initial condition.

∫ dy = ∫ 9e^7 dx

Integrating, we have:

y = 9e^7x + C

Now, we can use the initial condition y(-7) = 0 to determine the value of the constant C:

0 = 9e^7(-7) + C

Simplifying:

0 = -63e^49 + C

C = 63e^49

Therefore, the solution to the initial value problem is:

y = 9e^7x + 63e^49

Expressed as y = f(x), the solution is:

f(x) = 9e^7x + 63e^49

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Since the integral diverges, by the Integral Test, the series Σ(n²+1) also diverges. Therefore, the series Σ(n²+1) diverges.

The Integral Test states that if a series Σaₙ is non-negative, continuous, and decreasing on the interval [1, ∞), then it converges if and only if the corresponding integral ∫₁^∞a(x) dx converges.

In this case, we have the series Σ(n²+1), which is non-negative for all n ≥ 1. To apply the Integral Test, we consider the function a(x) = x²+1, which is continuous and decreasing on the interval [1, ∞).

Now, we evaluate the integral ∫₁^∞(x²+1) dx:

∫₁^∞(x²+1) dx = limₓ→∞ ∫₁ˣ(x²+1) dx = limₓ→∞ [(1/3)x³+x]₁ˣ = limₓ→∞ (1/3)x³+x - (1/3)(1)³-1 = limₓ→∞ (1/3)x³+x - 2/3.

As x approaches infinity, the integral becomes infinite.

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R be the region in the first quadrant bounded below by the parabola

y = x² and above by the line y = 2 then the value of the double integral [tex]\int\int_R yx\, dA[/tex] over the region R is 0.

To evaluate the double integral [tex]\int\int_R yx\, dA[/tex] over the region R bounded below by the parabola y = x² and above by the line y = 2, we need to determine the limits of integration for each variable.

The region R can be defined by the following inequalities:

0 ≤ x ≤ √y (due to y = x²)

0 ≤ y ≤ 2 (due to y = 2)

The integral can be set up as follows:

[tex]\int\int_R yx\, dA[/tex]= [tex]\int\limits^2_0\int\limits^{\sqrt{y}}_0 yx\,dx\,dy[/tex]

We integrate first with respect to x and then with respect to y.

[tex]\int\limits^2_0\int\limits^{\sqrt{y}}_0 yx\,dx\,dy[/tex] =[tex]\int\limits^2_0 [\frac{yx^2}{2}]^{\sqrt{y}}_0 dy[/tex]

Applying the limits of integration:

[tex]\int\limits^2_0 [\frac{yx^2}{2}]^{\sqrt{y}}_0 dy[/tex]= [tex]\int\limits^2_0 (0/2 - 0/2) dy =\int\limits^2_0 0 dy = 0[/tex]

Therefore, the value of the double integral ∫∫_R yx dA over the region R is 0.

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In questions 9-12, we are given two lines l1 and l2. In part (a), we determine whether l1 and l2 are parallel, perpendicular, or neither, and find the distance between the lines. In part (b), we find an equation for the plane that contains both lines.

9. (a) To determine whether l1 and l2 are parallel, perpendicular, or neither, we examine their direction vectors. The direction vector of l1 is (-3, 4, -1) and the direction vector of l2 is (1, 3, -4). Since the dot product of the direction vectors is not zero, l1 and l2 are neither parallel nor perpendicular.

To find the distance between the lines, we can use the formula for the distance between a point and a line. We select a point on one line, such as (2, -1, 1) on l1, and find the shortest distance to the other line. The distance between the lines is the magnitude of the vector connecting the two points, which is obtained by taking the square root of the sum of the squares of the differences of the coordinates.

(b) To find an equation for the plane that contains both lines, we can use the cross product of the direction vectors of l1 and l2 to find a normal vector to the plane. The normal vector is obtained by taking the cross product of (-3, 4, -1) and (1, 3, -4). This gives us a normal vector of (5, 13, 13).

Using the coordinates of a point on one of the lines, such as (2, -1, 1) on l1, we can write the equation of the plane as 5(x - 2) + 13(y + 1) + 13(z - 1) = 0.

Therefore, l1 and l2 are neither parallel nor perpendicular, the distance between the lines can be found using the formula for the distance between a point and a line, and the equation of the plane that contains both lines can be determined using the cross-product of the direction vectors and a point on one of the lines.

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The given differential equation is [tex]$y'+4x^2y=0$[/tex] and the power series solution of the given differential equation is [tex]$y=1-4x^2$[/tex].

The differential equation can be written as $y'=-4x^2y$.

Differentiating y with respect to [tex]x,$$\begin{aligned}y'&=0+a_1+2a_2x+3a_3x^2+...\end{aligned}$$[/tex]

Substitute the expression for $y$ and $y'$ into the differential equation.

[tex]$$y'+4x^2y=0$$$$a_1+2a_2x+3a_3x^2+...+4x^2(a_0+a_1x+a_2x^2+a_3x^3+...)=0$$[/tex]

Grouping terms with the same power of x, we have [tex]$$\begin{aligned}a_1+4a_0x^2&=0\\2a_2+4a_1x^2&=0\\3a_3+4a_2x^2&=0\\\vdots\end{aligned}$$[/tex]

Since the given differential equation is a second-order differential equation, it is necessary to have three non-zero terms of the series.

Thus, [tex]$a_0$[/tex] and [tex]$a_1$[/tex] can be chosen arbitrarily, but [tex]$a_2$[/tex]should be zero for the terms to satisfy the second-order differential equation.

We choose [tex]$a_0=1$[/tex] and [tex].$a_1=0$.[/tex]

Substituting [tex]$a_0$[/tex] and [tex]$a_1$[/tex] in the above equation, we get [tex]$$\begin{aligned}a_1+4a_0x^2&=0\\2a_2&=0\\3a_3&=0\\\vdots\end{aligned}$$$$a_1=-4a_0x^2$$$$a_2=0$$$$a_3=0$$[/tex]

Thus, the power series solution of the given differential equation is

[tex]$$\begin{aligned}y&=a_0+a_1x+a_2x^2+a_3x^3+...\\&=1-4x^2+0+0+...\end{aligned}$$[/tex]

Therefore, the power series solution of the given differential equation is [tex].$y=1-4x^2$.[/tex]

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The equation of the sphere with center (3, -12, 6) and radius 10 can be written as [tex](x - 3)² + (y + 12)² + (z - 6)² = 100.[/tex]

The equation of a sphere with center (h, k, l) and radius r is given by[tex](x - h)² + (y - k)² + (z - l)² = r².[/tex]

In this case, the center of the sphere is (3, -12, 6), so we substitute these values into the equation. Additionally, the radius is 10, so we square it to get 100.

Substituting the values, we obtain the equation[tex](x - 3)² + (y + 12)² + (z - 6)² = 100[/tex], which represents the sphere with a center at (3, -12, 6) and a radius of 10.

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