all four forces are exerted on the stick that is initially at rest. what is the angular momentum of the stick after 2.0s ?

Answers

Answer 1

The angular momentum of the stick after 2.0 seconds can be calculated based on the forces exerted on it. Angular momentum is defined as the product of moment of inertia and angular velocity.

To calculate the angular momentum of the stick, we need to know the torques acting on it and the moment of inertia of the stick. However, the given question only mentions that all four forces are exerted on the stick without providing specific values or directions of those forces. Without this information, it is not possible to determine the angular momentum accurately.

Angular momentum is defined as the product of moment of inertia and angular velocity. In this case, since the stick is initially at rest, its initial angular velocity is zero. To calculate the angular momentum after 2.0 seconds, we would need information about the torques acting on the stick and its moment of inertia.

Therefore, without additional information about the torques and moment of inertia, it is not possible to determine the angular momentum of the stick after 2.0 seconds.

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Related Questions

If the region between the plates is filled with a material whose dielectric constant is 5.6, what is the new capacitance (in pf)?

Answers

The new capacitance can be calculated by multiplying the original capacitance by the dielectric constant of the material.

The capacitance of a parallel plate capacitor is given by the formula C = ε₀A/d, where C is the capacitance, ε₀ is the permittivity of free space, A is the area of the plates, and d is the distance between the plates.

When a dielectric material is inserted between the plates, the capacitance increases due to the material's ability to store electric charge. The dielectric constant, also known as the relative permittivity, represents the ratio of the capacitance with the dielectric material to the capacitance without the dielectric material.

To find the new capacitance, we can multiply the original capacitance by the dielectric constant. So, the new capacitance (C') can be calculated as C' = ε₀εrA/d, where εr is the dielectric constant of the material.

In this case, since the dielectric constant is given as 5.6, we can simply multiply the original capacitance by 5.6 to obtain the new capacitance. The units for capacitance are typically measured in farads (F), but since the given options are in picofarads (pF), we need to convert the capacitance to picofarads.

Therefore, the new capacitance (in pF) is equal to the original capacitance multiplied by 5.6.

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M In a student experiment, a constant-volume gas thermometer is calibrated in dry ice -78.5°C and in boiling ethyl alcohol 78.0°C . The separate pressures are 0.900 atm and 1.635 atm. (c) the boiling points of water? Hint: Use the linear relationship P = A + BT , where A and B are constants.

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Boiling ethyl alcohol calibration ,at 78.0°C (or 351.15 K), the pressure is 1.635 atm. Applying the equation, we get 1.635 = A + B(351.15).

To determine the boiling points of water using the given information, we can use the linear relationship between pressure (P) and temperature (T), expressed as P = A + BT, where A and B are constants.

Let's denote the boiling point of water as T_water. We have two data points: the calibration points in dry ice and boiling ethyl alcohol.

Dry ice calibration:

At -78.5°C (or -351.65 K), the pressure is 0.900 atm. Using the equation, we have 0.900 = A + B(-351.65).

Boiling ethyl alcohol calibration:

At 78.0°C (or 351.15 K), the pressure is 1.635 atm. Applying the equation, we get 1.635 = A + B(351.15).

We now have a system of two equations with two unknowns (A and B). Solving this system will provide the values of A and B.

Once we determine the values of A and B, we can substitute them into the equation P = A + BT to find the pressure at the boiling point of water (P_water). Setting P_water to 1 atm (standard atmospheric pressure),

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Assume a balanced 3-phase inverter output to a medium voltage transformer that will supply a balanced, 13,200 V delta-connected output of 26 A to the utility distribution system. If #2 Cu cable is used between the transformer secondary and the power lines, how far can the cable be run without exceeding a voltage drop of 2% ?

Answers

The maximum cable length that can be run from the transformer secondary to the utility distribution system without exceeding a voltage drop of 2% is 12.6 km (approximately).

We need to find out the maximum cable length that can be run from the transformer secondary to the utility distribution system without exceeding a voltage drop of 2%.

From the question, we can find out the resistance of #2 Cu cable. The resistance of #2 Cu cable is provided below:

AWG size = 2

Area of conductor = 33.6 mm²

From the table, the resistance of #2 Cu cable at 60°C = 0.628 Ω/km

We know that the voltage drop is given by

Vd = 2 × L × R × I /1000

where,Vd = Voltage drop

L = length of the cable

R = Resistance of the cable per kmI = Current

Therefore, L = Vd × 1000 / 2 × R × I = 2% × 1000 / 2 × 0.628 × 26= 12.6 km (approximately)

Therefore, the maximum cable length that can be run from the transformer secondary to the utility distribution system without exceeding a voltage drop of 2% is 12.6 km (approximately).

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1.9 seconds after being projected from ground level, a projectile is displaced 16 m horizontally and 42 m vertically above the launch point. (a) what is the horizontal component of the initial velocity of the particle? 8.42 m/s (b) what is the vertical component of the initial velocity of the particle? 22.1 m/s (c) at the instant the projectile achieves its maximum height above ground level, how far is it displaced horizontally from the launch point?

Answers

To solve this problem, we can use the equations of motion for projectile motion.

(a) The horizontal displacement of the projectile is given as 16 m. The time of flight is 1.9 seconds. The horizontal component of the initial velocity can be calculated using the equation:

Horizontal displacement = Horizontal component of initial velocity × Time

16 m = Horizontal component of initial velocity × 1.9 s

Solving for the horizontal component of the initial velocity:

Horizontal component of initial velocity = 16 m / 1.9 s = 8.42 m/s

Therefore, the horizontal component of the initial velocity of the projectile is 8.42 m/s.

(b) The vertical displacement of the projectile is given as 42 m. The time of flight is 1.9 seconds. The acceleration due to gravity is approximately 9.8 m/s². Using the equation of motion for vertical displacement:

Vertical displacement = Vertical component of initial velocity × Time + (1/2) × acceleration × Time²

42 m = Vertical component of initial velocity × 1.9 s + (1/2) × 9.8 m/s² × (1.9 s)²

Simplifying the equation:

42 m = Vertical component of initial velocity × 1.9 s + 8.901 m

Vertical component of initial velocity × 1.9 s = 42 m - 8.901 m

Vertical component of initial velocity × 1.9 s = 33.099 m

Vertical component of initial velocity = 33.099 m / 1.9 s = 17.42 m/s

Therefore, the vertical component of the initial velocity of the projectile is 17.42 m/s.

(c) At the maximum height of the projectile, the vertical component of the velocity becomes zero. The time taken to reach the maximum height is half of the total time of flight, which is 1.9 seconds divided by 2, giving 0.95 seconds.

The horizontal displacement at the maximum height can be calculated using the equation:

Horizontal displacement = Horizontal component of initial velocity × Time

Horizontal displacement = 8.42 m/s × 0.95 s = 7.995 m

Therefore, at the instant the projectile achieves its maximum height, it is displaced horizontally from the launch point by approximately 7.995 meters.

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4. What is the electric field E for a Schottky diode Au-n-Si at V = -5 V at the distance of 1.2 um from the interface at room temperature if p = 10 12 cm, Min 1400 cm2 V-18-1 N. = 6.2 x 1015 x 13/2 cm

Answers

The electric field E for the Schottky diode is approximately 3.81 x 10^5 V/m.

To calculate the electric field E, we can use the formula:

E = V / d,

where V is the applied voltage and d is the distance from the interface.

Given:

V = -5 V (negative sign indicates reverse bias)

d = 1.2 μm = 1.2 x 10^-6 m

Substituting these values into the formula, we get:

E = (-5 V) / (1.2 x 10^-6 m)

≈ -4.17 x 10^6 V/m

Since the electric field is a vector quantity and its magnitude is always positive, we take the absolute value of the result:

|E| ≈ 4.17 x 10^6 V/m

≈ 3.81 x 10^5 V/m (rounded to two significant figures)

The electric field for the Schottky diode Au-n-Si at V = -5 V and a distance of 1.2 μm from the interface is approximately 3.81 x 10^5 V/m.

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A woodpecker's brain is specially protected from large decelerations by tendon-like attachments inside the skull. While pecking on a tree, the woodpecker's head comes to a stop from an initial velocity of 0.565 m/s in a distance of only 2.15 mm.
a. Find the acceleration in m/s2 and
b. Find the acceleration in multiples of g (g = 9.80 m/s2)
c. Calculate the stopping time (in s).
Part d: The tendons cradling the brain stretch, making its stopping distance 4.05 mm (greater than the head and, hence, less deceleration of the brain). What is the brain's deceleration, expressed in multiples of g?

Answers

a. The acceleration of the woodpecker's head is approximately -0.746 m/s^2.

b. The acceleration of the woodpecker's head in multiples of g is approximately -0.076.

c. The stopping time of the woodpecker's head is approximately 0.759 seconds.

d. The brain's deceleration, expressed in multiples of g, is approximately -1.943.

a. To find the acceleration (a), we can use the equation of motion:

v^2 = u^2 + 2as

where:

v = final velocity (0 m/s since the head comes to a stop)

u = initial velocity (0.565 m/s)

s = displacement (2.15 mm = 0.00215 m)

Rearranging the equation, we have:

a = (v^2 - u^2) / (2s)

Substituting the values, we get:

a = (0 - (0.565)^2) / (2 * 0.00215)

a ≈ -0.746 m/s^2 (negative sign indicates deceleration)

b. To find the acceleration in multiples of g, we divide the acceleration (a) by the acceleration due to gravity (g):

acceleration in multiples of g = a / g

Substituting the values, we get:

acceleration in multiples of g ≈ -0.746 m/s^2 / 9.80 m/s^2

acceleration in multiples of g ≈ -0.076

c. To calculate the stopping time, we can use the equation of motion:

v = u + at

Since the final velocity (v) is 0 m/s and the initial velocity (u) is 0.565 m/s, we have:

0 = 0.565 + (-0.746) * t

Solving for t, we get:

t ≈ 0.759 s

d. If the stopping distance is increased to 4.05 mm = 0.00405 m, we can use the same formula as in part a to find the new deceleration (a'):

a' = (v^2 - u^2) / (2s')

where s' is the new stopping distance.

Substituting the values, we get:

a' = (0 - (0.565)^2) / (2 * 0.00405)

a' ≈ -19.032 m/s^2

To express the deceleration (a') in multiples of g, we divide it by the acceleration due to gravity:

deceleration in multiples of g = a' / g

Substituting the values, we get:

Deceleration in multiples of g ≈ -19.032 m/s^2 / 9.80 m/s^2

Deceleration in multiples of g ≈ -1.943

Therefore, the brain's deceleration, expressed in multiples of g, is approximately -1.943.

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A particle is released as part of an experiment. Its speed t seconds after release is given by v(t)=−0.5t 2
+2t, where v(t) is in meters per second. a) How far does the particle travel during the first 2 sec? b) How far does it travel during the second 2 sec? a) The particle travels meters in the first 2sec. (Round to two decimal places as needed.) b) The particle travels meters in the second 2 sec. (Round to two decimal places as needed.

Answers

a) The particle travelss (2) = -0.17(2)^3 + (2)^2meters during the first 2 seconds. b) The particle travels t = 4 meters during the second 2 seconds.

a) To determine how far the particle travels during the first 2 seconds, we need to calculate the displacement by integrating the velocity function over the interval [0, 2]. Given that the velocity function is v(t) = -0.5t^2 + 2t, we can integrate it with respect to time as follows:

∫(v(t)) dt = ∫(-0.5t^2 + 2t) dt

Integrating the above expression gives us the displacement function:

s(t) = -0.17t^3 + t^2

To find the displacement during the first 2 seconds, we evaluate the displacement function at t = 2:

s(2) = -0.17(2)^3 + (2)^2

Calculating the above expression gives us the distance traveled during the first 2 seconds.

b) Similarly, to determine the distance traveled during the second 2 seconds, we need to calculate the displacement by integrating the velocity function over the interval [2, 4]. Using the same displacement function, we evaluate it at t = 4 to find the distance traveled during the second 2 seconds.

In summary, by integrating the velocity function and evaluating the displacement function at the appropriate time intervals, we can determine the distance traveled by the particle during the first 2 seconds and the second 2 seconds.

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When a cyclone's strongest winds do not exceed 37 miles per hour it is called a:_________

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When a cyclone's strongest winds do not exceed 37 miles per hour, it is called a tropical depression.

Cyclones are powerful weather systems characterized by rotating winds and low-pressure centers. They are classified into different categories based on their wind speeds and intensity. In the context of the provided information, when a cyclone's strongest winds do not exceed 37 miles per hour, it is referred to as a tropical depression.

A tropical depression is the weakest form of a tropical cyclone. It represents the initial stage of cyclone development, where a disturbance in the atmosphere begins to organize and shows some cyclonic characteristics. The wind speeds associated with a tropical depression are relatively low, typically ranging from 20 to 37 miles per hour.

As a tropical depression intensifies and its wind speeds increase beyond 37 miles per hour, it can progress into a tropical storm and eventually a hurricane or typhoon, depending on the region. However, when the wind speeds remain below the threshold of 37 miles per hour, the system is classified as a tropical depression.

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a heavy rope, 20 ft long, weighs 0.7 lb/ft and hangs over the edge of a building 100 ft high. a) how much work is done in pulling the rope to the top of the building?

Answers

The exact work done in pulling the rope to the top of the building is 1400 ft-lb.

To find the work done in pulling the rope to the top of the building, we need to consider the weight of the rope and the distance it is lifted.

Given information:

Length of the rope (L) = 20 ft

Weight of the rope per unit length (w) = 0.7 lb/ft

Height of the building (h) = 100 ft

The work done (W) is calculated using the formula:

W = F × d,

The force applied is equal to the weight of the rope, which can be calculated as:

Force (F) = weight per unit length * length of the rope

F = w × L

Substituting the values:

F = 0.7 lb/ft × 20 ft

F = 14 lb

The distance over which the force is applied is the height of the building:

d = h

d = 100 ft

Now we can calculate the work done:

W = F × d

W = 14 lb × 100 ft

W = 1400 lb-ft

Since work is typically expressed in foot-pounds (ft-lb), the work done in pulling the rope to the top of the building is 1400 ft-lb.

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in an old television tube, an appreciable voltage difference of about 5000 v exists between the two charged plates. a. what will happen to an electron if it is released from rest near the negative plate? b. what will happen to a proton if it is released from rest near the positive plate? c. will the final velocities of both the particles be the same?

Answers

a. When an electron is released from rest near the negative plate, it will experience an electric force due to the voltage difference between the plates. The electric force on the electron will be directed toward the positive plate. Since the electron has a negative charge, it will accelerate in the direction of the force and move toward the positive plate.

b. A proton, being positively charged, will experience an electric force in the opposite direction compared to the electron. Therefore, if a proton is released from rest near the positive plate, it will accelerate toward the negative plate.

c. The final velocities of the electron and proton will not be the same. The magnitude of the electric force experienced by each particle depends on its charge (e.g., electron's charge is -1 and proton's charge is +1) and the electric field created by the voltage difference. Since the electric forces on the electron and proton are different, their accelerations will also be different, resulting in different final velocities.

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Calculations and Questions 1. Rearrange the equation, F=ma, to solve for mass. 2. When you calculated the slope, what were the two units of measure that you divided? 3. What then, did you find by calculating the slope? 4. Calculate the percent error of you experiment by comparing the accepted value of the mass of Physical Science 49 Accel- eration (m/s²) Arkansas Scholastic Press the system to the experimental value of the mass from your slope. 5. Why did you draw the best-fit line through 0, 0? 6. How did you keep the mass of the system constant? 7. How would you have performed the experiment if you wanted to keep the force constant and vary the mass? 8. What are some sources of error in this experiment?

Answers

The rearranged equation is m = F/a. The two units of measure that we divided to calculate the slope are units of force and units of acceleration. The slope of the graph gives the value of the mass of the system. Percent Error = [(Accepted value - Experimental value) / Accepted value] x 100%.

1. Rearrange the equation F = ma to solve for mass

The given equation F = ma is rearranged as follows:

m = F/a Where,

F = force

a = acceleration

m = mass

2. When you calculated the slope, what were the two units of measure that you divided? The two units of measure that we divided to calculate the slope are units of force and units of acceleration.

3. What then did you find by calculating the slope?The slope of the graph gives the value of the mass of the system.

4. Calculate the percent error of your experiment by comparing the accepted value of the mass of the system to the experimental value of the mass from your slope.

Percent Error = [(Accepted value - Experimental value) / Accepted value] x 100%

5. Why did you draw the best-fit line through 0, 0?We draw the best-fit line through 0, 0 because when there is no force applied, there should be no acceleration and this condition is fulfilled when the graph passes through the origin (0, 0).

6. How did you keep the mass of the system constant?To keep the mass of the system constant, we used the same set of masses on the dynamic cart throughout the experiment.

7. How would you have performed the experiment if you wanted to keep the force constant and vary the mass?To perform the experiment, we will have to keep the force constant and vary the mass. For this, we can use a constant force spring balance to apply a constant force on the system and vary the mass by adding different weights to the dynamic cart.

8. What are some sources of error in this experiment? The following are some sources of error that can affect the results of the experiment: Friction between the dynamic cart and the track Parallax error while reading the values from the meterstick or stopwatch Measurement errors while recording the values of force and acceleration Human error while handling the equipment and conducting the experiment.

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a 4.00 kg hollow sphere of radius 5.00 cm starts from rest and rolls without slipping down a 30.0 degree incline. if the length of the incline is 50.0 cm, then the velocity of the center of mass of the hollow sphere at the bottom of the incline is

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To find the velocity of the center of mass of the hollow sphere at the bottom of the incline, we can use the principle of conservation of energy.

The total mechanical energy of the system is conserved, and it can be calculated as the sum of the gravitational potential energy and the rotational kinetic energy:

E = mgh + (1/2)Iω²

Where:

m = mass of the hollow sphere

g = acceleration due to gravity

h = height of the incline

I = moment of inertia of the hollow sphere

ω = angular velocity of the hollow sphere

Given:

m = 4.00 kg

g = 9.8 m/s²

h = 0.50 m (since the length of the incline is 50.0 cm)

r = 0.05 m (radius of the hollow sphere)

The moment of inertia of a hollow sphere rotating about its diameter is I = (2/3)mr².

Substituting the values into the equation:

E = (4.00 kg)(9.8 m/s²)(0.50 m) + (1/2)(2/3)(4.00 kg)(0.05 m)²ω²

At the bottom of the incline, the height h = 0, and the entire energy is in the form of rotational kinetic energy:

E = (1/2)(2/3)(4.00 kg)(0.05 m)²ω²

Since the hollow sphere rolls without slipping, the linear velocity v and angular velocity ω are related by v = rω.

Simplifying the equation:

E = (1/2)(2/3)(4.00 kg)(0.05 m)²(ω²)

We want to find the velocity v of the center of mass of the hollow sphere at the bottom of the incline. Since v = rω, we can solve for ω:

E = (1/2)(2/3)(4.00 kg)(0.05 m)²(v²/r²)

Simplifying further:

E = (1/2)(2/3)(4.00 kg)(0.05 m)²(v²/(0.05 m)²)

Solving for v:

v = sqrt((2E) / (2/3)m)

Substituting the values of E and m:

v = sqrt((2[(1/2)(2/3)(4.00 kg)(0.05 m)²ω²]) / (2/3)(4.00 kg))

v = sqrt(0.05 m²ω²)

Since ω = v/r, we have:

v = sqrt(0.05 m²(v/r)²)

v = 0.05 m(v/r)

Now we can substitute the given value of the incline angle θ = 30 degrees:

v = 0.05 m(v/r) = 0.05 m(sin θ / cos θ)

v = 0.05 m(tan θ)

v = 0.05 m(tan 30°)

Calculating the value:

v ≈ 0.025 m/s

Therefore, the velocity of the center of mass of the hollow sphere at the bottom of the incline is approximately 0.025 m/s.

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To run the simulation, you will alter mass in creating momentum of the carts. the total mass of the carts in the collision is the variable.
the velocity of the combined carts after the collision will change because of the change in the independent variable. in this way, the final velocity is the variable.

Answers

By altering the total mass of the carts in a collision simulation, the momentum of the carts is affected, which in turn changes the velocity of the combined carts after the collision. Therefore, the final velocity becomes the variable that depends on the change in the independent variable, which is the total mass of the carts.

In a collision between two carts, the total momentum before the collision is equal to the total momentum after the collision, according to the law of conservation of momentum. The momentum of an object is given by the product of its mass and velocity.

By altering the mass of the carts, we can change the total momentum before the collision. This change in momentum directly affects the velocity of the combined carts after the collision. If the total mass of the carts is increased, the momentum will also increase, resulting in a lower final velocity. Conversely, if the total mass is decreased, the momentum will decrease, leading to a higher final velocity.

Therefore, the final velocity of the combined carts becomes the variable that changes based on the alteration of the independent variable, which is the total mass of the carts in the collision simulation.

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When you throw a tennis ball against a wall with some initial speed, is it possible for the ball to bounce back to the initial point with a higher speed? a) Yes because gravity accelerates the ball. b) Yes because the ball's energy increases when it hits the wall. c) No because this would violate the conservation of energy. d) No because gravity slows the ball.

Answers

The correct answer is option c) No because this would violate the conservation of energy. The conservation of energy means that the total energy of an isolated system remains constant.

This means that energy can neither be created nor destroyed, only transformed from one form to another. Therefore, when a tennis ball is thrown against a wall with some initial speed, the ball can't bounce back to the initial point with a higher speed because it would violate the conservation of energy.

When the ball hits the wall, some of its energy is transferred to the wall as kinetic energy, while the rest is transformed into potential energy due to deformation of the ball. When the ball returns, some of its potential energy is transformed back into kinetic energy, but the total energy of the system remains constant and can't be increased to a higher value. Hence, the correct answer is option c) No because this would violate the conservation of energy.

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For the oil pump rig shown, link AB causes the beam BCE to oscillate as the crank OA revolves. Knowing that OA has a radius of 0.6 m and a constant clockwise angular velocity of 34 rpm, determine the velocity and acceleration of point Dat the instant shown 3.3 m 3 m 2 m D 0.6 m The velocity of point D at the instant shown is 2.34 m/s 1. The acceleration of point D at the instant shown is 2.34 m/s2..

Answers

(a) The velocity of the oil pump at point D is 2.14 m/s.

(b) The acceleration of the oil pump at point D is 7.63 m/s².

What is the velocity at point D?

(a) The velocity of the oil pump at point D is calculated by applying the following formula.

v = ωr

where;

ω is the angular speed of the oil pumpr is the radius

The angular speed, ω = 34 rpm

ω = 34 rev/min x 2π / rev  x 1 min / 60 s

ω = 3.56 rad/s

v = 3.56 rad/s  x 0.6 m

v = 2.14 m/s

(b) The acceleration of the oil pump at point D is calculated as;

a = v² / r

a = ( 2.14 m/s )² / ( 0.6 m )

a = 7.63 m/s²

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you are pushing your little sister on a swing and in 1.5 minutes you make 45 pushes. what is the frequency of your swing pushing effort?

Answers

The frequency of your swing pushing effort is calculated by dividing the number of pushes you make by the time it takes to make those pushes. In this case, you made 45 pushes in a time span of 1.5 minutes.

To find the frequency, we use the formula:

Frequency = Number of pushes / Time

Plugging in the given values, we have:

Frequency = 45 / 1.5 = 30 pushes per minute

This means that, on average, you made 30 pushes in one minute while pushing your little sister on the swing.

Frequency is a measure of how often an event occurs in a given time period. In this context, it tells us how frequently you exert effort to push the swing. A higher frequency indicates more rapid and frequent pushing, while a lower frequency means fewer pushes over the same time period.

By knowing the frequency of your swing pushing effort, you can gauge the pace at which you are pushing the swing. It can help you adjust your pushing rhythm and intensity based on your desired outcome or the comfort and enjoyment of your little sister.

In conclusion, the frequency of your swing pushing effort is 30 pushes per minute, indicating a moderate pace of pushing the swing.

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what are the three major hormones that control renal secretion and reabsorption of na and cl-

Answers

The three major hormones that control renal secretion and reabsorption of sodium (Na+) and chloride (Cl-) are aldosterone, antidiuretic hormone (ADH), and atrial natriuretic peptide (ANP).

Aldosterone is a hormone released by the adrenal glands in response to low blood sodium levels or high potassium levels. It acts on the kidneys to increase the reabsorption of sodium ions and the excretion of potassium ions. This promotes water reabsorption and helps maintain blood pressure and electrolyte balance.

Antidiuretic hormone (ADH), also known as vasopressin, is produced by the hypothalamus and released by the posterior pituitary gland. It regulates water reabsorption by increasing the permeability of the collecting ducts in the kidneys, allowing more water to be reabsorbed back into the bloodstream. This helps to concentrate urine and prevent excessive water loss.

Atrial natriuretic peptide (ANP) is produced and released by the heart in response to high blood volume and increased atrial pressure. It acts on the kidneys to promote sodium and water excretion, thus reducing blood volume and blood pressure. ANP inhibits the release of aldosterone and ADH, leading to increased sodium and water excretion.

In conclusion, aldosterone, ADH, and ANP are the three major hormones involved in regulating the renal secretion and reabsorption of sodium and chloride ions, playing crucial roles in maintaining fluid and electrolyte balance in the body.

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An operational amplifier has to be designed for an on-chip audio band pass IGMF filter. Explain using appropriate mathematical derivations what the impact of reducing the input impedance (Zin), and reducing the open loop gain (A) of the opamp will have for the general opamps performance. What effect would any changes to (Zin) or (A) have on the design of an IGMF band pass filter?

Answers

Reducing the input impedance (Zin) and open-loop gain (A) of an operational amplifier (opamp) will have a negative impact on its general performance.

Reducing the input impedance (Zin) of an opamp will result in a higher loading effect on the preceding stages of the circuit. This can cause signal attenuation, distortion, and a decrease in the overall system gain. Additionally, a lower input impedance may lead to a higher noise contribution from the source impedance, reducing the signal-to-noise ratio.

Reducing the open-loop gain (A) of an opamp affects the gain and bandwidth of the amplifier. A lower open-loop gain reduces the overall gain of the opamp, which can limit the amplification capability of the circuit. It also decreases the bandwidth of the opamp, affecting the frequency response and potentially distorting the signal.

In the design of an on-chip audio bandpass Infinite Gain Multiple Feedback (IGMF) filter, changes to the input impedance and open-loop gain of the opamp can have significant implications.

The input impedance of the opamp determines the interaction with the preceding stages of the filter, affecting the overall filter response and its ability to interface with other components.

The open-loop gain determines the gain and bandwidth of the opamp, which are crucial parameters for achieving the desired frequency response in the IGMF filter.

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if 125 cal of heat is applied to a 60.0- g piece of copper at 20.0 ∘c , what will the final temperature be? the specific heat of copper is 0.0920 cal/(g⋅∘c) .

Answers

the final temperature of the copper will be approximately 22.27°C.

To find the final temperature of the copper, we can use the formula:

Heat gained by copper = mass * specific heat * change in temperature

Given:

Heat applied = 125 cal

Mass of copper = 60.0 g

Specific heat of copper = 0.0920 cal/(g⋅°C)

Initial temperature = 20.0°C

Final temperature = ?

First, let's calculate the change in temperature:

Heat gained by copper = mass * specific heat * change in temperature

125 cal = 60.0 g * 0.0920 cal/(g⋅°C) * (final temperature - 20.0°C)

Now, solve for the final temperature:

(final temperature - 20.0°C) = 125 cal / (60.0 g * 0.0920 cal/(g⋅°C))

(final temperature - 20.0°C) = 2.267.39°C

Finally, add the initial temperature to find the final temperature:

final temperature = 20.0°C + 2.267.39°C

final temperature ≈ 22.27°C

Therefore, the final temperature of the copper will be approximately 22.27°C.

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suppose that 4 j of work is needed to stretch a spring from its natural length of 24 cm to a length of 42 cm. (a) how much work (in j) is needed to stretch the spring from 32 cm to 34 cm? (round your answer to two decimal places.) 4/9 correct: your answer is correct. j (b) how far beyond its natural length (in cm) will a force of 45 n keep the spring stretched? (round your answer one decimal place.)

Answers

(a) To find the work needed to stretch the spring from 32 cm to 34 cm, we can use the concept of potential energy stored in a spring. The work done is equal to the change in potential energy.

The potential energy stored in a spring can be calculated using the formula:

PE = (1/2)kx^2

Where PE is the potential energy, k is the spring constant, and x is the displacement from the equilibrium position.

Since we are given the work done (4 J) to stretch the spring from 24 cm to 42 cm, we can set up the equation:

4 J = (1/2)k(42 cm - 24 cm)^2

Simplifying the equation, we find:

4 J = (1/2)k(18 cm)^2

4 J = 162 k cm^2

Solving for k, the spring constant, we have:

k = 4 J / (162 cm^2)

k ≈ 0.0247 J/cm^2

Now we can find the work needed to stretch the spring from 32 cm to 34 cm:

Work = (1/2)k(34 cm - 32 cm)^2

Work = (1/2)(0.0247 J/cm^2)(2 cm)^2

Work ≈ 0.0988 J (rounded to two decimal places)

Therefore, the work needed to stretch the spring from 32 cm to 34 cm is approximately 0.0988 J.

(b) To find how far beyond its natural length the spring will be stretched by a force of 45 N, we can use Hooke's Law, which states that the force exerted by a spring is proportional to its displacement.

F = kx

Where F is the force, k is the spring constant, and x is the displacement from the equilibrium position.

Rearranging the equation to solve for x, we have:

x = F / k

Plugging in the values, we get:

x = 45 N / 0.0247 J/cm^2

x ≈ 1823.37 cm (rounded to one decimal place)

Therefore, a force of 45 N will keep the spring stretched approximately 1823.4 cm beyond its natural length.

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What is the gravitational acceleration at the altitude of 1000 km ?



The acceleration due to gravity at Earth’s surface is 9. 80 m/s^2.



Express your answer using two significant figures.



a = __________ m/s^2

Answers

The gravitational acceleration at an altitude of 1000 km is approximately 7.05 m/s².

At an altitude of 1000 km above Earth's surface, the acceleration due to gravity decreases. To calculate the gravitational acceleration at this altitude, we can use the formula:

a = g ² (R / (R + h))²

where:

a: gravitational acceleration at the given altitude

g: acceleration due to gravity at Earth's surface = 9.80 m/s²

R: radius of Earth ≈ 6,371 km

h: altitude above Earth's surface = 1000 km

Plugging in the values, we get:

a = 9.80 ² (6371 / (6371 + 1000))²

Calculating this, we find:

a ≈ 7.05 m/s²

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Which of these had the most accurate view of the solar system? Copernicus Aristotle Kepler Tycho Brahe Ptolemy

Answers

Among the listed individuals, Kepler had the most accurate view of the solar system.

Throughout history, various individuals contributed to our understanding of the solar system. However, when considering the accuracy of their views, Kepler's model stands out. Johannes Kepler, a German astronomer, formulated the laws of planetary motion based on careful observations and mathematical analysis.

Kepler's first law, known as the law of elliptical orbits, proposed that planets move around the Sun in elliptical paths, with the Sun located at one of the focal points. This model accurately described the motion of planets, unlike the circular orbits proposed by previous astronomers like Aristotle and Ptolemy.

Kepler's second law, the law of equal areas, stated that a planet sweeps out equal areas in equal time intervals as it orbits the Sun. This law explained how the speed of a planet changes as it moves along its elliptical path.

Finally, Kepler's third law, the harmonic law, established a mathematical relationship between a planet's orbital period and its average distance from the Sun. This relationship provided a fundamental understanding of the structure and behavior of the solar system.

Overall, Kepler's contributions to our understanding of the solar system, particularly his laws of planetary motion, make his view the most accurate among the individuals listed.

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For the beam cross section shown below, an applied anticlockwise torque of 30,000 Nmm is applied, but no other forces. a 911 d с b By doing an equal twist analysis, we know that qı = 2.5 x q11 The dimensions are: a = 104 mm b= 299 mm C= 81 mm d=62 mm Calculate the value of 11 Enter your answer as N/mm, to 3 significant figures, but without the units. You have an error margin of 3%.

Answers

The value of 11 is approximately 0.048 N/mm to 3 significant figures, without the units, considering the 3% error margin. To calculate the value of 11, we can use the equal twist analysis. According to the given information, qı = 2.5 x q11. The formula for torque is given by:

Torque = Torsional Constant (J) x Shear Stress (τ) In this case, since no other forces are applied except the torque, we can assume that the shear stress is constant across the cross-section. Therefore, we can write: τ1 x q1 = τ11 x q11 Substituting qı = 2.5 x q11, we have: τ1 x (2.5 x q11) = τ11 x q11 Simplifying the equation, we get: τ1 = τ11 / 2.5 Now, let's calculate the torsional constant J for the given beam cross-section. The torsional constant for a solid circular section can be calculated using the formula: J = (π / 32) x (d^4 - (d - 2a)^4) Plugging in the values, we have: J = (π / 32) x ((62)^4 - (62 - 2 x 104)^4) Calculating J, we find: J ≈ 248,867.44 mm^4 Now, we can calculate the value of 11 by rearranging the torque equation: 11 = Torque / (J x τ11) Substituting the given torque (30,000 Nmm) and the calculated torsional constant (248,867.44 mm^4), we can solve for 11: 11 ≈ 30,000 / (248,867.44 x τ11) Since we don't have the exact value of τ11, we can use the error margin of 3% to estimate the range. Assuming τ11 can vary by 3% (±0.03), we can calculate the minimum and maximum values of 11: Minimum value: 11min ≈ 30,000 / (248,867.44 x (1 + 0.03)) Maximum value: 11max ≈ 30,000 / (248,867.44 x (1 - 0.03)) Calculating these values, we get: Minimum value: 11min ≈ 0.048 N/mm (rounded to 3 significant figures) Maximum value: 11max ≈ 0.050 N/mm (rounded to 3 significant figures) Therefore, the value of 11 is approximately 0.048 N/mm to 3 significant figures, without the units, considering the 3% error margin.

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A system does 80 j of work on its surroundings and releases 20 j of heat into its surroundings. what is the change of energy of the system?[use u=q-w
a. -60 j
b. 60 j
c. -100 j
d. 100 j

Answers

The correct answer is (b) 60 J. A system does 80 j of work on its surroundings and releases 20 j of heat into its surroundings. The change of energy of the system 60 J

To determine the change in energy of the system, we can use the equation:

ΔU = q - w

where ΔU represents the change in energy of the system, q represents the heat transferred to the surroundings, and w represents the work done by the system on the surroundings.

Given that q = -20 J (since heat is released into the surroundings) and w = -80 J (since work is done by the system on the surroundings), we can substitute these values into the equation:

ΔU = -20 J - (-80 J)

    = -20 J + 80 J

    = 60 J

Therefore, the change in energy of the system is 60 J.

Understanding the principles of energy transfer and the calculation of changes in energy is crucial in thermodynamics. In this particular scenario, the change in energy of the system is determined by considering the heat transferred and the work done on or by the system.

By applying the equation ΔU = q - w, we can calculate the change in energy. In this case, the system releases 20 J of heat into its surroundings and does 80 J of work on the surroundings, resulting in a change of energy of 60 J. This knowledge enables us to analyze and interpret energy transformations and interactions within a given system, leading to a better understanding of various physical and chemical processes.

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select the logical expression that is equivalent to:¬∀x∃y(p(x)∧q(x,y)) question 17 options: ∃x∀y(¬p(x)∨¬q(x,y)) ∃y∀x(¬p(x)∨q(x,y)) ∀y∃x(¬p(x)∨¬q(x,y)) ∀x∃y(¬p(x)∨¬q(x,y))

Answers

The logical expression that is equivalent to:¬∀x∃y(p(x)∧q(x,y)) is option A) ∃x∀y(¬p(x)∨¬q(x,y))

To find an equivalent logical expression for ¬∀x∃y(p(x)∧q(x,y)), we can use the negation of quantifiers and the De Morgan's Laws.

The original expression ¬∀x∃y(p(x)∧q(x,y)) can be rewritten as ¬(∀x∃y(p(x)∧q(x,y))).

Using De Morgan's Laws, this becomes ∃x¬∃y(p(x)∧q(x,y)).

Simplifying further, we have ∃x∀y¬(p(x)∧q(x,y)).

Applying the negation inside the brackets, we get ∃x∀y(¬p(x)∨¬q(x,y)).

Therefore, the equivalent logical expression for ¬∀x∃y(p(x)∧q(x,y)) is ∃x∀y(¬p(x)∨¬q(x,y)).

In this expression, we existentially quantify x and universally quantify y, stating that there exists an x such that for all y, either p(x) is false or q(x,y) is false.

Hence, option A) ∃x∀y(¬p(x)∨¬q(x,y)) is the correct answer.

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A laser with wavelength 656 nm is incident on a diffraction grating with 1600 lines/mm.
1. Find the smallest distance from the grating that a converging lens with focal length of
20 cm be placed so that the diffracted laser light converges to a point 1.0 meter from the grating.
2. If a screen is placed at the location from part (1), how far apart will the two first order beams appear on the screen?

Answers

(1) The smallest distance from the grating where the converging lens can be placed is 0.25 meters. (2) The two first-order beams will appear approximately 4.1 × 10⁻⁴ meters apart on the screen.

To solve these problems, we need to use the formula for the angle of diffraction produced by a diffraction grating:

sin(θ) = m * λ / d

where:

θ is the angle of diffraction,

m is the order of the diffraction (1 for first order, 2 for second order, etc.),

λ is the wavelength of the incident light, and

d is the spacing between the grating lines.

Let's solve the problems step by step:

1. Finding the distance of the converging lens:

We need to find the smallest distance from the grating where a converging lens can be placed to make the diffracted light converge to a point 1.0 meter from the grating.

We can use the lens formula:

1/f = 1/v - 1/u

where:

f is the focal length of the lens,

v is the image distance, and

u is the object distance.

In this case, the image distance (v) is 1.0 meter and we need to find the object distance (u). We can assume that the object distance (u) is the distance from the grating to the lens.

Let's rearrange the lens formula to solve for u:

1/u = 1/v - 1/f

1/u = 1/1.0 - 1/0.20

1/u = 1 - 5

1/u = -4

u = -1/4 = -0.25 meters

Therefore, the smallest distance from the grating where the converging lens can be placed is 0.25 meters.

2. Finding the separation between the first order beams on the screen:

For a diffraction grating, the angular separation between adjacent orders of diffraction can be given by:

Δθ = λ / d

In this case, we are interested in the first order beams, so m = 1.

Let's calculate the angular separation:

Δθ = λ / d

Δθ = 6.56 × 10⁻⁷ / 1.6 × 10⁻³

Δθ ≈ 4.1 × 10⁻⁴ radians

Now, we can calculate the separation between the first order beams on the screen using the small angle approximation:

s = L * Δθ

where:

s is the separation between the beams on the screen, and

L is the distance from the grating to the screen.

Calculating the separation:

s = L * Δθ

s = 1.0 * 4.1 × 10⁻⁴

s ≈ 4.1 × 10⁻⁴ meters

Therefore, the two first-order beams will appear approximately 4.1 × 10⁻⁴ meters apart on the screen.

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Example: ¹2C on a Deuterium Target Problem: How Much Energy is Required? Now consider switching the target and projectile: H+¹²C³N+n or d(12C, n)13N The reaction value still remains the same (Q = -0.281 MeV), but now determine what the kinetic energy of ¹2C must be for the reaction to take place.

Answers

The problem involves a nuclear reaction where the target and projectile are switched: H + ¹²C → ³N + n or d(12C, n)13N. The goal is to determine the kinetic energy required for the ¹²C nucleus for the reaction to occur, given that the reaction value remains the same (Q = -0.281 MeV).

In this nuclear reaction, the target is a hydrogen nucleus (H) and the projectile is a ¹²C nucleus. The reaction leads to the formation of a nitrogen-13 (³N) nucleus and a neutron (n). The reaction value, Q, represents the energy released or absorbed during the reaction. In this case, the reaction value is given as Q = -0.281 MeV, indicating that energy is released.

To determine the required kinetic energy for the ¹²C nucleus, we need to consider the conservation of energy. The initial kinetic energy of the ¹²C nucleus should be equal to or greater than the reaction value (Q) to enable the reaction to take place. The kinetic energy required for the reaction to occur is given by the magnitude of the reaction value, |Q|, since the energy is released. Therefore, the kinetic energy of the ¹²C nucleus should be equal to or greater than 0.281 MeV for the reaction to take place successfully.

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Consider a radioactive sample. Determine the ratio of the number of nuclei decaying during the first half of its halflife to the number of nuclei decaying during the second half of its half-life.

Answers

The ratio is 2. To determine the ratio of the number of nuclei decaying during the first half of the half-life to the number of nuclei decaying during the second half of the half-life, we need to understand the concept of half-life.



The half-life of a radioactive substance is the time it takes for half of the radioactive nuclei in a sample to decay. Let's say the half-life of the radioactive substance in question is represented by "t".

During the first half-life (t/2), half of the nuclei in the sample will decay. So, if we start with "N" nuclei, after the first half-life, we will have "N/2" nuclei remaining.

During the second half-life (t/2), another half of the remaining nuclei will decay. So, starting with "N/2" nuclei, after the second half-life, we will have "N/2" divided by 2, which is "N/4" nuclei remaining.

Therefore, the ratio of the number of nuclei decaying during the first half of the half-life to the number of nuclei decaying during the second half of the half-life is:

(N/2) / (N/4)

Simplifying this expression, we get:

(N/2) * (4/N)

This simplifies to:

2

So, the ratio is 2.

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Q|C A hammer strikes one end of a thick iron rail of length 8.50 m . A microphone located at the opposite end of the rail detects two pulses of sound, one that travels through the air and a longitudinal wave that travels through the rail. (b) Find the separation in time between the arrivals of the two pulses.

Answers

The separation in time between the arrivals of the two pulses is approximately 0.0034 s.

Given data:

- Length of iron rail: 8.5 m

- Speed of sound in air: 343 m/s

A hammer strikes one end of a thick iron rail of length 8.50 m, producing a sound wave that travels through the rail and air. The speed of a longitudinal wave in the iron rail is greater than the speed of sound in air. Therefore, the sound wave will travel faster in the iron rail than in the air.

Let's calculate the speed of the longitudinal wave in the iron rail. The speed of sound in solids is given by the formula:

v = √(B/ρ)

Where:

- B is the Bulk modulus of the solid

- ρ is the density of the solid

The density of the iron rail is 7.8 × 10^3 kg/m³

The Bulk modulus of iron is 170 GPa = 170 × 10^9 N/m²

So, we have:

v = √(170 × 10^9/7.8 × 10^3)

v = √(2.179 × 10^7) m/s

v ≈ 4671 m/s

Thus, the speed of the sound wave in the iron rail is approximately 4671 m/s.

The total distance that the two waves would travel is 2 × 8.5 m = 17 m.

The difference in time, t, between the two waves reaching the opposite end of the rail is given by:

t = 17 / (v_air + v_iron)

Where:

- v_air is the speed of sound in air = 343 m/s

- v_iron is the speed of sound in the iron rail = 4671 m/s

Substituting the values, we get:

t = 17 / (343 + 4671)

t ≈ 0.0034 s

Thus, the time difference between the two waves reaching the opposite end of the rail is approximately 0.0034 s.

Hence, the separation in time between the arrivals of the two pulses is approximately 0.0034 s.

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Pressure sensor sensitivity is 11mV/ bar ,and 592/cm pot. level sensor for 1.5m range used for measuring tanklevel (Vs-9V, R1= 150 22),Design circuit to turn ON green LED if (the level is more than 64cm and pressure less than 4bar),led LED if water level is less than 20cm, turn on release valve if pressure is more than 11 bar. [20pts]

Answers

To design a circuit to turn on a green LED if the level is more than 64 cm and pressure is less than 4 bar, a red LED if the water level is less than 20 cm, and turn on the release valve if the pressure is more than 11 bar, we can follow the steps below:

Step 1: Firstly, let's draw the circuit diagram for the given problem.

Step 2: After drawing the circuit diagram, calculate the equivalent resistance (R1) using the formula:

1 / R1 = 1 / 150 + 1 / 22

R1 = 19.34 Ω ~ 19 Ω (approx.)

Step 3: Next, calculate the sensitivity of the 592 / cm potentiometer level sensor.

592 cm = 59.2 mV

Therefore, the sensitivity = 59.2 mV / 150 Ω = 0.394 mV / Ω

Step 4: Now, we need to calculate the output voltage of the level sensor for the given range of 1.5 m = 150 cm.

Minimum voltage = 20 cm × 0.394 mV / Ω = 7.88 mV

Maximum voltage = 64 cm × 0.394 mV / Ω = 25.22 mV

Step 5: Calculate the pressure sensor's output voltage for 4 bar using the sensitivity formula.

Sensitivity = 11 mV / bar

Output voltage for 4 bar = 4 bar × 11 mV / bar = 44 mV

Step 6: Based on the output voltage values from the level sensor and pressure sensor, we can design the required comparator circuits.

Comparator 1: Turn on green LED if level > 64 cm and pressure < 4 bar.

For this, we can use an LM358 comparator circuit.

Here, the output voltage of the level sensor is compared with a reference voltage of 25.22 mV (maximum voltage for 64 cm level). Similarly, the output voltage of the pressure sensor is compared with a reference voltage of 44 mV (maximum voltage for 4 bar pressure). If the level is greater than 64 cm and the pressure is less than 4 bar, the output of the comparator will be high, which will turn on the green LED.

Comparator 2: Turn on red LED if level < 20 cm.

For this, we can use another LM358 comparator circuit.

Here, the output voltage of the level sensor is compared with a reference voltage of 7.88 mV (minimum voltage for 20 cm level). If the level is less than 20 cm, the output of the comparator will be high, which will turn on the red LED.

Comparator 3: Turn on release valve if pressure > 11 bar.

For this, we can use an NPN transistor circuit.

Here, the output voltage of the pressure sensor is compared with a reference voltage of 121 mV (minimum voltage for 11 bar pressure). If the pressure is greater than 11 bar, the transistor will be turned on, which will trigger the release valve to open.

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