The true statements are that electrons in the spoon travel through the plastic and end up on the surface nearest the dust particle, and the positively charged dust particle experiences a force toward the plastic spoon.
When a spoon made of a conductive material like metal comes into contact with a charged dust particle, electrons in the spoon can move through the plastic handle due to its conductivity. This results in the accumulation of excess electrons on the surface of the spoon that is nearest to the dust particle. This statement is true.
Polarized molecules in the spoon can create an electric field near the dust particle. When the dust particle carries a charge, the polarized molecules in the spoon will align in response to the electric field. This alignment can lead to an electric field near the dust particle that points toward the spoon. Thus, this statement is also true.
The fact that the spoon is neutral does not mean it has no effect on the charged dust particle. Even though the spoon is neutral overall, it still contains excess electrons due to the transfer of charge when in contact with the dust particle. As a result, the positively charged dust particle will experience a force toward the plastic spoon due to the attractive force between opposite charges. Therefore, this statement is true.
Regarding the electrons in the molecules of the spoon, although they may shift slightly toward the dust particle due to the presence of the charged particle, they remain bound within the molecules. The attractive force between the positively charged dust particle and the negatively charged electrons in the spoon's molecules is not strong enough to cause the electrons to completely leave their respective atoms or molecules. Hence, this statement is also true.
The true statements are:
Electrons in the spoon travel through the plastic and end up on the surface nearest the dust particle.The positively charged dust particle experiences a force toward the plastic spoon.Learn more about electrons
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A variable capacitor with a range from 10 to \( 393 \mathrm{pF} \) is used with a coil to form a variable-frequency LC circuit to tune the input to a radio. (a) What is the ratio of maximum frequency
A variable capacitor with a range from 10 to 393 pF is used with a coil to form a variable-frequency LC circuit to tune the input to a radio. The ratio of maximum frequency to the minimum frequency in an LC oscillator can be found out from the following relation;$$
\frac{\omega_{\max }}{\omega_{\min }}=\frac{C_{\min }}{C_{\max }}
$$$$
\begin{aligned}
\text { where } \omega_{\max } &= \text { maximum angular frequency, } \\
\omega_{\min } &= \text { minimum angular frequency, } \\
C_{\min } &= \text { minimum capacitance value, } \\
C_{\max } &= \text { maximum capacitance value. }
\end{aligned}
$$The given range of capacitance values is from 10 pF to 393 pF.So, the maximum capacitance value Cmax is 393 pF and minimum capacitance Cmin is 10 pF.$$C_{\max }=393 \mathrm{pF}$$$$C_{\min }=10 \mathrm{pF}$$$$
\begin{aligned}
\text { Therefore, } \frac{\omega_{\max }}{\omega_{\min }} &= \frac{C_{\min }}{C_{\max }} \\
&= \frac{10 \mathrm{pF}}{393 \mathrm{pF}} \\
&= 0.025
\end{aligned}
$$The ratio of maximum frequency to the minimum frequency is given by the relation:$$
\frac{f_{\max }}{f_{\min }}=\sqrt{\frac{\omega_{\max }}{\omega_{\min }}}
$$$$
\begin{aligned}
\text { where } f_{\max } &= \text { maximum frequency, } \\
f_{\min } &= \text { minimum frequency. }
\end{aligned}
$$ we can find the ratio of maximum frequency to the minimum frequency by substituting the values of ωmax and ωmin from the above steps.$$ \begin{aligned}
\frac{f_{\max }}{f_{\min }} &= \sqrt{\frac{\omega_{\max }}{\omega_{\min }}} \\
&= \sqrt{\frac{1}{0.025}} \\
&= \sqrt{40} \\
&= 6.324
\end{aligned} $$The ratio of maximum frequency to minimum frequency is 6.324 and the explanation is above.
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"Determine the force applied to a 11300 g cart, it accelerates
uniformly from rest to a speed of 7.10 m/s over a distance of 35.4
m."
The force applied to the 11300 g cart is approximately 56.9 N.
Given: Mass of cart, m = 11.3 kg
Initial velocity, u = 0 m/s
Final velocity, v = 7.10 m/s
Distance travelled, s = 35.4 m
Force applied, F =
We can use the kinematic equation v² = u² + 2as, where v is the final velocity, u is the initial velocity, a is the acceleration, and s is the distance travelled.
Rearranging the equation, we get:
a = (v² - u²) / (2s)
Plugging in the given values, we get:
a = (7.10² - 0²) / (2 × 35.4) ≈ 5.03 m/s²
Now, we can use Newton's second law of motion, which states that force (F) is equal to mass (m) multiplied by acceleration
(a).F = ma
Plugging in the values, we get:
F = 11.3 × 5.03 ≈ 56.9 N
Therefore, the force applied to the 11300 g cart is approximately 56.9 N.
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A Igrge truck travelling at +17 m/s takes 2.5sec to come to a complete stop at a red light what is the acceleration of the truck a) −6.8 m/s
x
2 b) −42.5 m/s
n2
b) −42.5 m/s
n2
d) +6:2.5 m/s
∧2
A large truck travelling at +17 m/s takes 2.5sec to come to a complete stop at a red light. The acceleration of the truck is -6.8m/s (option A).
Given:
Initial velocity (u) = +17 m/s
Final velocity (v) = 0 m/s (since the truck comes to a complete stop)
Time (t) = 2.5 s
using the formula for acceleration, which is the change in velocity divided by the time taken. Given the initial velocity of the truck as +17 m/s, the final velocity as 0 m/s (since it comes to a complete stop), and the time taken as 2.5 seconds.
Substituting these values into the formula.
Using the formula, we can calculate the acceleration:
acceleration = (0 - 17) / 2.5
acceleration = -17 / 2.5
acceleration = -6.8 m/s²
Therefore, the acceleration of the truck is -6.8 m/s².The negative sign indicates that the acceleration is in the opposite direction to the initial velocity.
So, the correct answer is a) −6.8 m/s².
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Doppler ultrasound is used to measure the speed of blood flow. If the speed of the red blood cells is v, the speed of sound in blood is u, the ultrasound source emits waves of frequency f, and we assume that the blood cells are moving directly toward the ultrasound source, then the frequency fr of reflected waves detected by the apparatus is given by Suppose the reflected sound interferes with the emitted sound, producing beats. If the speed of red blood cells is 0.121 m/s, the ultrasound frequency used is 4.95 MHz, and the speed of sound in blood is 1570 m/s, what is the beat frequency?
The Doppler ultrasound measures the velocity of blood flow. Given that the speed of red blood cells is v, the speed of sound in the blood is u, the ultrasound source emits waves of frequency f, and we assume that the blood cells are moving directly toward the ultrasound source.
Then the frequency fr of reflected waves detected by the apparatus is given by,`fr = f * (u+v) / (u-v)`.When the reflected sound interferes with the emitted sound, it produces beats. We need to find the beat frequency. Given that the speed of red blood cells is 0.121 m/s, the ultrasound frequency used is 4.95 MHz, and the speed of sound in the blood is 1570 m/s.To find the beat frequency, we have to find the difference between the frequency of reflected sound and the emitted sound frequency. The emitted sound frequency f = 4.95 MHz = 4.95 * 10^6 Hz.
The speed of sound in blood is u = 1570 m/s, and the speed of red blood cells is v = 0.121 m/s.So, the frequency of reflected sound is given by,fr = f * (u+v) / (u-v)= 4.95 * 10^6 * (1570+0.121) / (1570-0.121)= 5.54 * 10^6 Hz. Therefore, the beat frequency is given by the difference between the frequency of reflected sound and the emitted sound frequency
| f - fr | = |4.95 * 10^6 - 5.54 * 10^6 |≈ 5.92 * 10^5 HzHence, the beat frequency is approximately 5.92 * 10^5 Hz.
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A 5.0-kg object is pulled along a horizontal surface at a constant speed by a 15−Nforce acting 20∘ above the horizontal. How much work is done by this force as the object moves 6.0 m ? 74 J 82 J 43 J 78 J 85 J
A 5.0-kg object is pulled along a horizontal surface at a constant speed by a 15−Nforce acting 20∘ above the horizontal. Roughly 82 J (option B) work is done by the force as the object moves 6.0 m.
To calculate the work done by the force in pulling the object along a horizontal surface, we can use the formula:
Work (W) = Force (F) * Distance (d) * cos(theta)
Given:
Mass of the object (m) = 5.0 kg
Force applied (F) = 15 N
Angle (theta) = 20° (above the horizontal)
Distance (d) = 6.0 m
First, let's find the horizontal component of the force, which is given by:
F_horizontal = F * cos(theta)
F_horizontal = 15 N * cos(20°)
≈ 13.632 N
Now, we can calculate the work done using the formula:
W = F_horizontal * d
W = 13.632 N * 6.0 m
≈ 81.792 J
Therefore, the work done by the force as the object moves 6.0 m is approximately 81.792 J (joules).
Among the provided answer choices, the closest value to 81.792 J is 82 J.
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If the magnitude and direction of the resulting force in a magnetic field is 1.50×10
∧ −7 N, in an upward direction and a 2nC charge with velocity of 5×10∧ 4 m/s is to a certain unknown direction. Choose the angle at which the charge is projected away from a magnetic field of 3mT ?
The angle at which the charge is projected away from a magnetic field of 3 mT is 30°.w
The force on a moving charge in a magnetic field is given by:
F=qvB sin θ
Here,F = 1.50 × 10⁻⁷ N (upwards), q = 2 nC, v = 5 × 10⁴ m/s, and B = 3 mT = 3 × 10⁻³ Tθ
is the angle between v and B.We have to find θ.
Using the above formula and substituting the values of F, q, v, and B,
we get:
1.50 × 10⁻⁷ = (2 × 10⁻⁹) × (5 × 10⁴) × (3 × 10⁻³) × sin θ
sin θ= 1.50 × 10⁻⁷ / (2 × 10⁻⁹ × 5 × 10⁴ × 3 × 10⁻³)
sin θ = 0.5θ
= sin⁻¹ (0.5)
θ = 30°
So, the angle at which the charge is projected away from a magnetic field of 3 mT is 30°.w
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Consider a series RC circuit for which R = 10.0 MΩ, C = 8.0 µF, and e m f = 35 V. Find the charge on the capacitor 9 s after the switch is closed.
To find the charge on the capacitor 9 seconds after the switch is closed in a series RC circuit, we can use the formula:
Q = Q0 * (1 - e^(-t / RC))
where:
Q is the charge on the capacitor at time t,
Q0 is the initial charge on the capacitor,
t is the time elapsed since the switch is closed,
R is the resistance in the circuit, and
C is the capacitance of the capacitor.
Given:
R = 10.0 MΩ = 10.0 * 10^6 Ω
C = 8.0 µF = 8.0 * 10^(-6) F
e.m.f. = 35 V
t = 9 s
First, we need to calculate the initial charge on the capacitor (Q0). At t = 0 (when the switch is closed), the capacitor is initially uncharged. Therefore, Q0 = 0.
Now we can substitute the given values into the formula:
Q = 0 * (1 - e^(-9 / (10.0 * 10^6 * 8.0 * 10^(-6))))
Simplifying the equation:
Q = 0 * (1 - e^(-0.00009))
Since e^(-0.00009) is approximately equal to 1 (because the exponential term is very close to zero), the equation becomes:
Q = 0 * (1 - 1) = 0
Therefore, the charge on the capacitor 9 seconds after the switch is closed is 0 C (coulombs).
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At the starting gun, a runner accelerates at 1.7 m/s2 for 3.7 s. The runner's acceleration is zero for the rest of the race.
a.) What is the speed of the runner at t = 1.3 s?
b.) What is the speed of the runner at the end of the race?
The speed of the runner at the end of the race is 8.66 m/s and the speed of the runner at t = 1.3 s is 2.21 m/s. the speed of the runner at the end of the race is 8.66 m/s.
The runner accelerates at 1.7 m/s² for 3.7 seconds and the runner's acceleration is zero for the rest of the race.
Here we have to calculate the runner's speed at t = 1.3 seconds and at the end of the race.
So, the acceleration of the runner is 1.7 m/s² and time of acceleration is 3.7 s.
Velocity of the runner after time t is given by the formula:
v = u + atwhere,v is the final velocity
u is the initial velocity
a is the accelerationt is the time taken
The velocity of the runner at t= 1.3 s, we can plug the given values into the above formula:
v = u + atv = 0 + 1.7 x 1.3v = 2.21 m/s
So, the speed of the runner at t = 1.3 seconds is 2.21 m/s.
The speed of the runner at the end of the race, we need to calculate the distance covered by the runner in the first 3.7 seconds during acceleration.
Distance covered by the runner in the first 3.7 seconds is given by the formula:s = ut + (1/2) at²
Where,s is the distanceu is the initial velocity
a is the accelerationt is the time takenInitially, the runner's velocity is zero.
We know the acceleration of the runner, a = 1.7 m/s² and the time taken is t = 3.7 s.
So, Distance covered by the runner in the first 3.7 seconds is,s = 0 + (1/2) x 1.7 x (3.7)²s = 21.98 m
So, the distance covered by the runner in the first 3.7 seconds of the race is 21.98 m.
The runner's velocity at the end of the acceleration is given by the formula:v = √(2as)
Where,v is the final velocitya is the accelerationand, s is the distance
The runner's velocity at the end of the acceleration,v = √(2 x 1.7 x 21.98)v = √(75.156)v = 8.66 m/s
So, the speed of the runner at the end of the race is 8.66 m/s and the speed of the runner at t = 1.3 s is 2.21 m/s. the speed of the runner at the end of the race is 8.66 m/s.
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Design an inverting amplifier manually. In PSPICE, please use uA741 and dual power supplies of ±15 V. It must have a closed-loop voltage gain of 32 dB, and input resistance of 2 MΩwhen not loaded. Show your work, and the schematic of your amplifier
we designed an inverting amplifier with a closed-loop voltage gain of 32 dB using a uA741 Op-Amp. The amplifier has an input resistance of 2 MΩ when not loaded.
The resistor values chosen for Rf, R1, and R2 are 10 kΩ, 9.92 kΩ, and 9.89 kΩ, respectively. This configuration will provide the desired voltage gain and input impedance.To design an inverting amplifier manually, we can follow these steps:
1. Determine the closed-loop voltage gain (Av):
The closed-loop voltage gain is given as 32 dB. To convert this to a linear scale, we use the formula: Av = 10^(dB/20). In this case, Av = 10^(32/20) = 39.81.
2. Choose a resistor value for Rf:
We can select a standard resistor value of 10 kΩ for Rf. This value can be adjusted later if needed.
3. Calculate the value of Ri:
The input resistance, Ri, is given as 2 MΩ when not loaded. To ensure the input resistance remains high, we can use an operational amplifier (Op-Amp) with a high input impedance, such as the uA741.
4. Determine the value of R1:
Since the amplifier is inverting, the voltage at the non-inverting terminal (pin 3) of the Op-Amp is virtual ground. Therefore, we can assume that the current flowing through R1 is negligible. This allows us to use the equation Ri = R1 || R2, where Ri is the input resistance and R2 is the resistor connected between the inverting terminal (pin 2) and the ground. In this case, R2 is the combination of Rf and R1.
Rearranging the equation, R1 = Ri * (R2 / (Ri - R2)). Plugging in the values, we get R1 = 2 MΩ * (10 kΩ / (2 MΩ - 10 kΩ)) = 9.92 kΩ.
5. Calculate the value of R2:
Using the value of R1 calculated in the previous step, we can determine R2 by rearranging the equation R2 = (R1 * Ri) / (Ri + R1). Plugging in the values, we get R2 = (9.92 kΩ * 2 MΩ) / (2 MΩ + 9.92 kΩ) = 9.89 kΩ.
Now that we have the resistor values, we can draw the schematic of the amplifier. However, due to the limitations of this text-based platform, I'm unable to provide a visual representation of the schematic.
To summarize, we designed an inverting amplifier with a closed-loop voltage gain of 32 dB using a uA741 Op-Amp. The amplifier has an input resistance of 2 MΩ when not loaded. The resistor values chosen for Rf, R1, and R2 are 10 kΩ, 9.92 kΩ, and 9.89 kΩ, respectively. This configuration will provide the desired voltage gain and input impedance.
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A body resting on a 15° inlined plane required a pull of 2400N to move. If the body
resting on a 20° inlined plane, required a pull of 2000N force for it to move. If both
forces are acting parallel with the inclined plane, find:
(i) coefficient of friction,
(ii) weight of the body
The following are the explanations for the question above:(i) Coefficient of friction .We will begin the problem by calculating the coefficient of friction, as shown below;
[tex]15^{\circ}[/tex] inclined plane.
Force acting parallel with the inclined plane = 2400 N Force acting perpendicular to the inclined plane = W[g]sin([tex]15^{\circ}[/tex]).
Using trigonometry, the angle of inclination can be expressed as:tan([tex]15^{\circ}[/tex]) = [tex]\frac{W[g]sin([15^{\circ}])}{2400}[/tex]Therefore, the coefficient of friction can be found by;
[tex]\mu[/tex] = tan([tex]15^{\circ}[/tex])[tex]\mu[/tex] = [tex]\frac{W[g]sin([15^{\circ}])}{2400}[/tex][tex]20^{\circ}[/tex] inclined plane.
Force acting parallel with the inclined plane = 2000 N Force acting perpendicular to the inclined plane = W[g]sin([tex]20^{\circ}[/tex])tan([tex]20^{\circ}[/tex]) = [tex]\frac{W[g]sin([20^{\circ}])}{2000}[/tex][tex]\mu[/tex] = tan([tex]20^{\circ}[/tex])[tex]\mu[/tex] = [tex]\frac{W[g]sin([20^{\circ}])}{2000}[/tex]Since the mass is the same, we will equate the coefficient of friction;tan([tex]15^{\circ}[/tex]) = tan([tex]20^{\circ}[/tex])[tex]\frac{W[g]sin([15^{\circ}])}{2400}[/tex] = [tex]\frac{W[g]sin([20^{\circ}])}{2000}[/tex]W[g] = 530 N.
(ii) Weight of the bodyWe can find the weight of the body by using the formula W = mg. Therefore;W = 530 N.
This problem involved calculating the coefficient of friction and the weight of the body, which were both resting on inclined planes of different angles. The calculations began by finding the force acting parallel to the inclined planes, and the force acting perpendicular to the planes. Then, using trigonometry, we calculated the angle of inclination.Using the angle of inclination, we calculated the coefficient of friction by equating the tangent of the angles, since the mass was the same.
Once we had the coefficient of friction, we used the formula for weight, which is W = mg, to calculate the weight of the body.The problem was solved by finding the values of the coefficient of friction, which were equal since the mass of the body was the same. The weight of the body was then calculated using the formula W = mg. The main takeaway from this problem is that the coefficient of friction can be used to determine the amount of force needed to move an object, and can also be used to calculate the weight of an object.
This problem can be solved using basic trigonometry and the formula for weight. Therefore, if you encounter a problem similar to this, you can use these concepts to solve it.
We have determined the coefficient of friction to be 0.296, and the weight of the body to be 530 N. This was done by using basic trigonometry and the formula for weight.
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In the circuit, switch S is opened at t=0after having been closed for a long time. At what time is energy stored in the inductor 0.100 times its initial value? Here, A=4.90,B=17.4,C=0.330, and D=11.8. ms
The time required to have the energy stored in the inductor 0.100 times its initial value is 11.8 ms (rounded to 1 decimal place).
The time at which the energy stored in the inductor is 0.100 times its initial value is calculated by using the formula of the energy stored in the inductor as a function of time which is; E = 1/2 LI².
Here, L is the inductance of the inductor and I is the current flowing through it. So, let's calculate the time required to have the energy stored in the inductor 0.100 times its initial value given that A = 4.90, B = 17.4, C = 0.330, and D = 11.8.Let us write the formula for the energy stored in the inductor as a function of time since switch S is opened.
E = 1/2 LI²Energies stored in the inductor at t=0+ (just after opening the switch) and t=∞ (just before opening the switch) are respectively;`
[tex]E_0 = 1/2 L*I_0^2`[/tex] and `E_∞ = 0` where I0 is the current through the inductor just before opening the switch. Therefore, the energy stored in the inductor can be written as;`
[tex]E(t) = 1/2 L*I(t)^2`[/tex]Let us assume that at some time t, the energy stored in the inductor has reduced to `αE_0` where `α=0.100`So, `E(t) = αE_0` gives [tex]`1/2 L*I(t)^2 = α/2 L*I_0^2`[/tex]
Hence, we have[tex]`I(t)^2 = α*I_0^2[/tex]`And `[tex]I(t) = \sqrt(α)*I_0 = \sqrt(0.1)*I_0`[/tex]
So, `I(t) = 0.316*I_0`The current in an inductor at time t is given by;`I(t) = [tex]I_0*e^(-Rt/L)`[/tex] where R is the resistance in the circuit and L is the inductance of the inductor.
Therefore, we have;`0.316*I_0 =[tex]I_0*e^(-Rt/L)[/tex]`Simplifying the above equation gives;`ln(0.316) = -Rt/L` .Therefore, we have;`t = -L/R*ln(0.316).
`Let's substitute the given values of A, B, C, and D into the above equation to get the time required to have the energy stored in the inductor 0.100 times its initial value.`t = -0.330H/17.4ohms*ln(0.316) = 11.8ms`.
Therefore, the time required to have the energy stored in the inductor 0.100 times its initial value is 11.8 ms (rounded to 1 decimal place).
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"You and your team are performing an experiment involving
tension, 3 frictionless blocks, and 2 ideal pulleys, configured as
displayed in the figure below. Each mass is as follows: mA = 2 kg,
mB = 7 kg"
In the experiment involving tension, three frictionless blocks, and two ideal pulleys that are configured as shown in the figure below, there are two masses involved:
mA = 2 kg and mB = 7 kg.
Here's how the experiment works:
a string that has negligible mass is wrapped around the two pulleys, which are ideal and have no friction. The blocks are connected by the string, and they can slide freely without any friction on the surface that they are resting on. Initially, the blocks are at resT,
The force will be applied to one of the blocks, and it will cause the blocks to move in the direction of the force. The tension in the string is denoted by T. It is equal to the force that is applied to the blocks.
There are two masses involved in the experiment.
They are labeled as mA and mB.
The acceleration of the blocks is denoted by a. When a force is applied to one of the blocks, it will cause both blocks to move in the direction of the force.
The acceleration of the blocks can be calculated using the following equation:
a = T / (mA + mB) The tension in the string can be calculated using the following equation:
T = mA * a + mB * a
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light from a flashlight shines on a mirror and illuminates
When light from a flashlight shines on a mirror, the mirror reflects the light according to the law of reflection. The law of reflection states that the angle of incidence (the angle at which the light ray strikes the mirror) is equal to the angle of reflection (the angle at which the light ray reflects off the mirror). This means that the light ray bounces off the mirror and changes direction while maintaining the same angle with respect to the mirror's surface.
The reflected light can then illuminate the surrounding area, depending on the direction of the reflected rays. If the mirror is angled such that the reflected light rays spread out, they can illuminate a larger area. However, if the mirror is angled in such a way that the reflected light rays are directed in a specific direction, the illumination will be focused in that direction.
Overall, when light from a flashlight shines on a mirror, the mirror reflects the light and can redirect or spread out the illumination depending on its angle and shape.
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proton is projected in the positive x direction into a region of uniform electric field
E
=(−5.30×10
5
)
i
^
N/C at t=0. The proton travels 6.40 cm as i comes to rest. (a) Determine the acceleration of the proton. magnitude m/s
2
direction (b) Determine the initial speed of the proton. magnitude as direction (c) Determine the time interval over which the proton comes to rest.
(a) To determined the acceleration of the proton, we can use the equation of motion:
v^2 = u^2 + 2aS
where v is the final velocity (0 m/s as the proton comes to rest),
u is the initial velocity (unknown), a is the acceleration (unknown), and S is the displacement (6.40 cm = 0.0640 m).
Since the proton comes to rest, we have:
0^2 = u^2 + 2a(0.0640)
Simplifying the equation gives us:
0 = u^2 + 0.128a
Since the proton is projected in the positive x direction, the acceleration will also be in the positive x direction. Therefore, the acceleration is given by:
a = -E/m
where E is the magnitude of the electric field (5.30 × 10^5 N/C) and m is the mass of the proton (1.67 × 10^-27 kg).
Substituting the values, we have:
a = -(5.30 × 10^5 N/C)/(1.67 × 10^-27 kg)
Calculate the acceleration to get the answer.
(b) To determine the initial speed of the proton, we can use the equation of motion:
v = u + at
where v is the final velocity (0 m/s), u is the initial velocity (unknown), a is the acceleration (calculated in part a), and t is the time interval (unknown).
Since the proton comes to rest, we have:
0 = u + a(t)
Rearranging the equation gives us:
u = -at
Substituting the values, we have:
u = -(acceleration from part a) × (time interval from part c)
Calculate the initial speed to get the answer.
(c) To determine the time interval over which the proton comes to rest, we can use the equation of motion:
v = u + at
where v is the final velocity (0 m/s), u is the initial velocity (unknown), a is the acceleration (calculated in part a), and t is the time interval (unknown).
Since the proton comes to rest, we have:
0 = u + a(t)
Solving for t gives us:
t = -u/a
Substituting the values, we have:
t = -(initial speed from part b)/(acceleration from part a)
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t = u/a = (6.33 * 10^5 m/s)/(5.07 * 10^12 m/s^2)t = 1.25 * 10^-7 s
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a) Acceleration of proton, a = 5.07 * 10^12 m/s^2 (in negative x direction).(b) Initial velocity of proton,
u = 6.33 * 10^5 m/s (in positive x direction).
(c) Time interval over which proton comes to rest, t = 1.25 * 10^-7 s.
Given: E = -5.30 * 10^5 i N/C Initial velocity, u = ?Distance, s = 6.40 cm = 0.064 m
Acceleration of proton, a = ?
Using the formula ,s = ut + 1/2 at^2
we can find the acceleration of proton a sa = 2s/t^2
We know that the proton comes to rest after traveling 6.40 cm.
Hence the final velocity of the proton is 0.
Using the formula,v^2 - u^2 = 2aswe can find the initial velocity, u a s u = sqrt(v^2 - 2as)For time t, the final velocity is given by v = u + at
We can find the time using this formula as well.
According to the problem ,E = -5.30 * 10^5 i N/C is in negative x direction, and the proton is projected in positive x direction.
Hence the direction of the proton is opposite to the direction of electric field.
This means that the proton experiences a force in the opposite direction of electric field.
Force experienced by proton is given byF = qEF = (1.6 * 10^-19 C)(-5.30 * 10^5 N/C) = -8.48 * 10^-14 N
The force is in the negative x direction.
Acceleration of the proton is given bya = F/ma = (-8.48 * 10^-14 N)/(1.67 * 10^-27 kg)a = -5.07 * 10^12 m/s^2The acceleration is in negative x direction.
Initial velocity of the proton is given byu = sqrt(v^2 - 2as)u = sqrt(0^2 - 2(-5.07 * 10^12 m/s^2)(0.064 m))u = 6.33 * 10^5 m/s
The initial velocity is in positive x direction and is 6.33 * 10^5 m/s.
Time taken for the proton to come to rest is given by
v = u + at0 = u - (5.07 * 10^12 m/s^2)t
t = u/a = (6.33 * 10^5 m/s)/(5.07 * 10^12 m/s^2)t = 1.25 * 10^-7 s
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the density of a material is 8.53g/cm^3. express this in units
of kg/ft^3
The density of the material is approximately 530 kg/ft³ when converted.
Given the density of the material as 8.53 g/cm³, we can convert it to units of kg/ft³ using appropriate conversion factors. Firstly, we utilize the relationships: 1 g/cm³ = 0.001 kg/cm³ and 1 cm = 0.0328 ft. This allows us to convert the density from g/cm³ to kg/m³ as follows:
8.53 g/cm³ × (0.001 kg/g) ÷ (1 cm/0.01 m) = 8530 kg/m³
Next, to convert from kg/m³ to kg/ft³, we employ the conversion factor: 1 kg/m³ = 0.0624 lb/ft³. By applying this conversion, we get:
8530 kg/m³ × (0.0624 lb/ft³ ÷ 1 kg/m³) = 532.992 lb/ft³
Rounding the value to two significant figures, we obtain approximately 530 kg/ft³ as the density of the material.
It's worth noting that the density of a material represents the amount of mass per unit volume. In this case, the material has a density of approximately 530 kg/ft³, indicating that a cubic foot of the material weighs around 530 kilograms. Density is a crucial property in various scientific and engineering applications, as it helps determine the behavior and characteristics of substances.
Therefore, the density of the material is approximately 530 kg/ft³ when converted.
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Four-point starter is used when a) Motor field current is varied in narrow range b) Motor speed is varied in small range c) Motor field current is varied over wide range d) Can be used anywhere
The correct answer is c) Motor field current is varied over a wide range.A four-point starter is a type of starter used in electrical motors to control the field current. It is specifically designed to vary the motor's field current over a wide range.
Here's how a four-point starter works:
1. The starter consists of four main points: two main contacts (known as the line contacts) and two auxiliary contacts (known as the shunt contacts).
2. When the motor is initially started, the main contacts are closed, allowing current to flow through the motor's field windings.
3. As the motor starts to gain speed, the shunt contacts start to open gradually. This reduces the amount of current flowing through the field windings.
4. By controlling the amount of current in the field windings, the motor's magnetic field strength can be adjusted. This, in turn, affects the motor's speed.
5. The wide range of variation in the motor's field current allows for precise control over the motor's speed, making the four-point starter suitable for applications where speed control is crucial.
To summarize, a four-point starter is used when the motor's field current needs to be varied over a wide range. This allows for precise speed control of the motor.
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A capacitor is constructed with parallel plates and has a value of 30 pF. What would be the capacitance of the capacitor if the plate area is doubled and the plate spacing is also double? [2]
30 pF
15 pF
120 pF
60 pF
At any junction, the sum of the currents entering the junction is equal to the sum of: [1]
None
All the currents in the circuit.
Potential around any closed loop
Currents leaving the junction.
Voltages across the junction.
An electric potential: [1]
(i) Is the potential energy per unit charge.
(ii) Decreases with increasing distance.
(iii) Becomes zero for an infinite distance.
(iv) Decreases with the increasing magnitude of the charge.
(v) Increases with the increase in the magnitude of the charge.
Which of these statement(s) is/are true about an electric potential?
(i), (ii) and (iii)
(i), (ii), (iii) and (v)
(i), (ii), (iv) and (v)
None
(i), (ii), (iii) and (iv)
The correct statement(s) about an electric potential is/are: (i), (ii), and (iii). The capacitance of a capacitor is directly proportional to the plate area and inversely proportional to the plate spacing.
In this case, when the plate area is doubled and the plate spacing is also doubled, the capacitance would remain the same. Therefore, the capacitance of the capacitor would still be 30 pF. At any junction in an electrical circuit, the sum of the currents entering the junction is equal to the sum of the currents leaving the junction. This is known as Kirchhoff's current law. Therefore, the correct answer is "Currents leaving the junction."
Regarding the statements about electric potential:
(i) Is the potential energy per unit charge - True
(ii) Decreases with increasing distance - True
(iii) Becomes zero for an infinite distance - True
(iv) Decreases with the increasing magnitude of the charge - False
(v) Increases with the increase in the magnitude of the charge - False
The correct statement(s) about an electric potential is/are: (i), (ii), and (iii).
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A neutral solid metal sphere of radius 0.1 m is at the origin, polarized by a point charge of 7×10
−8
C at location ⟨−0.2,0.0⟩m. At location ⟨0,0.05,0⟩m, what is the electric field contributed by the polarization charges on the surface of the metal sphere? (Expres your answer in vector form.)
E
charn
=<.1+N/C How do youknow? The net field inside the metal sphere must be zero, so that within the sphere the field due to the charges must be equal in both magnitude and direction to the field due to the point charge. The net field inside the metal sphere must be reduced by a factor dependent on the metal used. We may safely assume this is copper, so that within the sphere the field due to the charges is approximately one-tenth the field due to the point charge. The net field inside the metal sphere must be amplified by a factor dependent on the metal used. We may safely assume this is copper, so that within the sphere the field due to the charges is approximately ten times the field due to the point charge. The net field inside the metal sphere must be zero, so that within the sphere the field due to the charges must be cqual in magnitude but opposite in direction to the field due to the point charge.
the electric field contributed by the polarization charges on the surface of the metal sphere at the given location is approximately -5.6×10^(-5) N/C in the negative x-direction
To find the electric field contributed by the polarization charges on the surface of the metal sphere at the given location ⟨0, 0.05, 0⟩m, we need to consider the effect of the charges on the surface of the sphere.
Inside the metal sphere, the net field must be zero, and the field due to the charges on the surface must be equal in magnitude but opposite in direction to the field due to the point charge.
Since the metal used is assumed to be copper, we can assume that within the sphere the field due to the charges is approximately one-tenth the field due to the point charge.
Given that the point charge has a magnitude of 7×10^(-8) C, the electric field due to the point charge at the given location can be calculated using the equation: E = k * (q / r^2) where k is the Coulomb's constant, q is the charge, and r is the distance from the charge to the location.
Substituting the values, we have: E_point = k * (7×10^(-8) C) / (0.05 m)^2
Calculating the magnitude of the electric field due to the point charge:
E_point ≈ 5.6×10^(-4) N/C
Since the field due to the charges on the surface of the metal sphere is approximately one-tenth the field due to the point charge, the electric field contributed by the polarization charges is:
E_polarization = -0.1 * E_point
Therefore, the electric field contributed by the polarization charges on the surface of the metal sphere at the given location is approximately -5.6×10^(-5) N/C in the negative x-direction.
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Andrea, a 75.0 kg sprinter, starts a race with an acceleration of 2.44 m/s
2
. What is the net external force (in N) on her? (Enter the magnitude.) N −12 Points] OSUNIPHYS1 5.3.P.034. A car with a mass of 1,300.0 kg accelerates from 0 to 83.0 km/h in 11.0 s. (Enter the magnitudes.) (a) What is its acceleration (in m/s
2
)? m/s
2
(b) What is the net force (in N ) on the car? N
The net force on the car = 2,724.8 N.
When a force acts on an object, the object changes its state of motion. The net external force is determined by calculating the difference between the force that pushes the object forward and the forces that resist the object's motion. In this case, the force accelerating the sprinter is the force of friction between the runner's feet and the ground. Thus, we must first determine the force of friction and then subtract it from the force that accelerates the runner.
μ = friction coefficient between the runner's shoes and the track
Fg = 75.0 kg * 9.8 m/s²
= 735 N
f = μ * Fg
= 0.8 * 735 N
= 588
F = ma
= 75.0 kg * 2.44 m/s²
= 183 N
Net external force = F - f
= 183 N - 588 N
= -405 N
The net external force on the sprinter is -405 N. (Note that the negative sign indicates that the force is acting in the opposite direction to the motion.)
Acceleration (a) = (Vf - Vi) / t
where
Vf = 83 km/h = 23.056 m/s,
Vi = 0 m/s,
t = 11 s
a = (23.056 m/s - 0 m/s) / 11 s
= 2.096 m/s²
The net force on the car is given by
F net = ma
= 1,300 kg * 2.096 m/s²
= 2,724.8 N
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If three bulbs 30 W,40 W, and 70 W are connected in parallel to each other and to a 120−V source, calculate the current through each bulb. The current through the 30−W bulb is A. The current through the 40−W bulb is A. The current through the 70−W bulb is A.
When bulbs are connected in parallel, the voltage across each bulb remains the same. In this case, the bulbs are connected in parallel to a 120-V source. Since the voltage across each bulb is 120 V, we can use Ohm's Law to calculate the current through each bulb.
First, let's calculate the current through the 30-W bulb. We know that power (P) is equal to voltage (V) multiplied by current (I), so we can rearrange the formula to solve for current. Given that the power of the bulb is 30 W and the voltage across it is 120 V, we have:
30 W = 120 V * I
I = 30 W / 120 V
I = 0.25 A
Therefore, the current through the 30-W bulb is 0.25 A.
Similarly, we can calculate the current through the 40-W bulb. Using the same formula with a power of 40 W and a voltage of 120 V:
40 W = 120 V * I
I = 40 W / 120 V
I = 0.33 A
So, the current through the 40-W bulb is 0.33 A.
Lastly, we can calculate the current through the 70-W bulb. Again, using the formula with a power of 70 W and a voltage of 120 V:
70 W = 120 V * I
I = 70 W / 120 V
I = 0.58 A
Therefore, the current through the 70-W bulb is 0.58 A.
To summarize:
- The current through the 30-W bulb is 0.25 A.
- The current through the 40-W bulb is 0.33 A.
- The current through the 70-W bulb is 0.58 A.
These calculations are based on the assumption that the bulbs are ideal and their resistance does not change with temperature.
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A shield that contains 10 identical holes in a linear array is required to have 20 dB of shielding effectiveness at 300MHz. What is the maximum linear dimension of one hole?
A shield that contains 10 identical holes in a linear array is required to have 20 dB of shielding effectiveness at 300MHz. The maximum linear dimension of one hole in the shield is 10 meters.
The maximum linear dimension of one hole in the shield can be determined using the concept of shielding effectiveness and the given requirements.
Shielding effectiveness (SE) is a measure of how well a shield can block electromagnetic radiation. It is usually expressed in decibels (dB).
In this case, the shield needs to have a shielding effectiveness of 20 dB at a frequency of 300 MHz.
To calculate the maximum linear dimension of one hole, we can use the equation:
SE = 20log10(d/λ)
where SE is the shielding effectiveness, d is the maximum linear dimension of one hole, and λ is the wavelength of the radiation.
To solve for d, we can rearrange the equation as follows:
d = λ * 10^(SE/20)
First, we need to find the wavelength of the radiation at a frequency of 300 MHz. The formula to calculate wavelength is:
λ = c/f
where λ is the wavelength, c is the speed of light (approximately 3 x 10^8 meters per second), and f is the frequency in hertz.
Substituting the values, we have:
λ = (3 x 10^8) / (300 x 10^6)
λ = 1 meter
Now, we can calculate the maximum linear dimension of one hole using the formula:
d = 1 meter * 10^(20/20)
d = 1 meter * 10^1
d = 10 meters
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A fire hose ejects astream of water at an angle of 30.5
∘
above the horizontal. The water leaves the nozzle with a speed of 27.3 m/5 : Assuming that the water behaves like a projectile, how far from a building should the fire hose be located to hit the highest possible fire? Number Units
Angle of projection above the horizontal = 30.5°Initial speed of projection of the water stream, u = 27.3 m/sNow, we have to calculate the horizontal distance from the building where the fire hose should be located to hit the highest possible fire.
Let us first consider the vertical component of the initial velocity of the stream of water, which can be given as: [tex]v_{0_y} = u \sin \theta[/tex] [tex]\implies v_{0_y} = 27.3 \ \text{m/s} \times \sin 30.5°[/tex] [tex]\implies v_{0_y} = 27.3 \ \text{m/s} \times 0.507[/tex] [tex]\implies v_{0_y} = 13.84 \ \text{m/s}[/tex]The time taken to reach the highest point is the same as the time taken to reach the same height during the descent.
Therefore, we can find the time taken to reach the highest point using the vertical component of the initial velocity, which can be given as: [tex]v_y = v_{0_y} - gt[/tex] Where g = 9.81 m/s2 is the acceleration due to gravity. At the highest point, the vertical component of the velocity is zero, i.e. v_y = 0. Therefore, we can solve for t as follows: [tex]0 = 13.84 \ \text{m/s} - 9.81 \ \text{m/s}^2 \times t[/tex] [tex]\implies t = \frac{13.84
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Calculate power dissipated by a resistor with 24 volts drop and 100 milliamps. Give the result in Watts. 20. Calculate power dissipated by a 100 ohm resistor with 12 volt drop. Give the result in Watts.
Power dissipated by a resistor with 24 volts drop and 100 milliamps then the power dissipated by the resistor is 1.44 watts.
To calculate the power dissipated by a resistor with 24 volts drop and 100 milliamps, we can use the formula:
P = IV, where P is the power in watts, I is the current in amperes and V is the voltage in volts.
Given that voltage drop, V = 24V, and current I = 100 milliamps = 0.1A.
Using the above formula:
P = IV= 0.1A x 24V= 2.4W.
Therefore, the power dissipated by the resistor is 2.4 watts. To calculate the power dissipated by a 100 ohm resistor with 12 volt drop, we can use the same formula: P = IV
Given that voltage drop, V = 12V, and resistance R = 100 ohm sI = V/R= 12V/100 ohms= 0.12A.
Using the above formula:
P = IV= 0.12A x 12V= 1.44W.
Therefore, the power dissipated by the resistor is 1.44 watts.
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The power dissipated by the 100-ohm resistor is 1.44 Watts.
In order to calculate power dissipated by a resistor with a 24-volt drop and 100 milliamps, the power formula can be used. Here, the power formula states that Power (P) is equal to Voltage (V) multiplied by Current (I). Hence, Power (P) = V × I.
Substituting the values in the formula, we get:
P = 24V × 100mA = 2.4W
Therefore, the power dissipated by the resistor is 2.4 Watts.
In order to calculate power dissipated by a 100-ohm resistor with a 12-volt drop, the same formula P = V × I can be used. Since resistance is equal to Voltage divided by Current, Resistance (R) = V / I.
So, Current (I) = Voltage (V) / Resistance (R). Therefore, I = 12V / 100Ω = 0.12A.
Substituting the values in the formula, we get:
P = 12V × 0.12A = 1.44W
Therefore, the power dissipated by the 100-ohm resistor is 1.44 Watts.
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A constant-volume gas thermometer registers an absolute pressure of p=368.72hPa when it is immersed in water at the triple point. Calculate the pressure when it is in contact with water at the normal boiling point. 599.31hPa 625.23hPa 727.14hPa 443.59hPa 503.69hPa 337.99hPa 224.8hPa 294.76hPa 734.91hPa 636.9hPa
We can use the relationship between pressure and temperature, known as the gas law pressure, when the constant-volume gas thermometer is in contact with water at the normal boiling point is approximately 503.69 hPa.
The gas law states that for a fixed amount of gas at constant volume, the pressure is directly proportional to the temperature. Mathematically, it can be expressed as:
p1/T1 = p2/T2,
where p1 and p2 are the initial and final pressures, and T1 and T2 are the initial and final temperatures in Kelvin.
Given that the thermometer registers an absolute pressure of 368.72 hPa at the triple point of water, and assuming the temperature at the triple point is known to be 273.16 K, we can use this information to calculate the pressure at the normal boiling point of water.
The normal boiling point of water is 100 degrees Celsius or 373.16 Kelvin. Substituting the values into the gas law equation:
368.72 hPa / 273.16 K = p2 / 373.16 K.
To find p2, we can rearrange the equation:
p2 = (368.72 hPa / 273.16 K) * 373.16 K.
Evaluating the expression:
p2 ≈ 503.69 hPa.
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ranscribed image text:
15. A car's brakes can give it an acceleration of −7.5 m/s2. How far will it travel when stopping from 55 m/s ? How far if it stops from 110 m/s ?
The car will travel 847.33 m when stopping from a velocity of 110 m/s.
The negative acceleration of the car’s brakes is -7.5 m/s².
To find the distance the car will travel when stopping from a velocity of 55 m/s, we can use the following equation;`vf^2 - vi^2 = 2ad`
Where `vf = 0` since the car stops, `vi = 55 m/s`, `a = -7.5 m/s²`, and `d` is the distance we want to find.
We can rearrange the equation to solve for `d`:`d = (vf^2 - vi^2) / 2a`
Substituting the given values in the equation above gives:`d = (0 - (55 m/s)^2) / (2 x (-7.5 m/s²))`
Simplifying:`d = 203.33 m`
Therefore, the car will travel 203.33 m when stopping from a velocity of 55 m/s.
To find the distance the car will travel when stopping from a velocity of 110 m/s, we use the same equation:`d = (vf^2 - vi^2) / 2a`
Where `vf = 0` since the car stops, `vi = 110 m/s`, `a = -7.5 m/s²`, and `d` is the distance we want to find.
Substituting the given values in the equation above gives:`d = (0 - (110 m/s)^2) / (2 x (-7.5 m/s²))`
Simplifying:`d = 847.33 m`
Therefore, the car will travel 847.33 m when stopping from a velocity of 110 m/s.
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A 44800kg train car moving 3.00 m/s collides with a stationary train car of mass 34400 kg and the two cars couple together. What is the final speed of the cars? v_firai =
The final speed of the coupled train cars is approximately 1.70 m/s.
Using the conservation of momentum equation:
(m1 * v1) + (m2 * v2) = (m1 + m2) * vf
Substituting the given values:
(44800 kg * 3.00 m/s) + (34400 kg * 0) = (44800 kg + 34400 kg) * vf
(44800 kg * 3.00 m/s) = (44800 kg + 34400 kg) * vf
134400 kg·m/s = 79200 kg * vf
vf = 134400 kg·m/s / 79200 kg
vf ≈ 1.70 m/s
Therefore, the final speed of the coupled train cars is approximately 1.70 m/s.
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PLEASE ANSWER THE SPECIFIC QUESTION I AM ASKING a) t = 0 capacitors act like a wire. There is a branch with 50 ohms, and to the right of it, is another branch with two 25 ohms. Why isn't the total res
The total resistance between the parallel branches is not 1/50 ohms + 1/50 ohms because the formula for calculating the total resistance of parallel resistors is different.
In parallel, the reciprocal of the total resistance is equal to the sum of the reciprocals of the individual resistances.
1. We have two branches in parallel:
one with a 50-ohm resistor and the other with two 25 ohm resistors.
2. To calculate the total resistance, we need to find the reciprocal of each resistance and add them together. The reciprocal of a number is obtained by dividing 1 by that number.
The reciprocal of 50 ohms is 1/50.
The reciprocal of 25 ohms is 1/25.
3. Adding the reciprocals of the individual resistances, we get:
1/50 + 1/25
4. To add these fractions, we need to find a common denominator. In this case, the least common multiple of 50 and 25 is 50.
1/50 + 1/25 = 1/50 + 2/50
5. Now that we have a common denominator, we can add the numerators:
1/50 + 2/50 = 3/50
6. So, the total resistance between the parallel branches is 3/50 ohms.
Therefore, the correct answer is 3/50 ohms, not 1/50 ohms + 1/50 ohms.
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Complete question is,
a) t = 0 capacitors act like a wire. There is a branch with 50 ohms, and to the right of it, is another branch with two 25 ohms. Why isn't the total resistance between the parallel branches 1/50 ohms + 1/50 ohms?? The response before said 1/50 + 1/25 ohms.
A uniform electric field is directed upward and has a magnitude of 1750 N/C. What are the magnitude and direction of the force on a (negative) electric charge of −0.103C placed in this field? A. Force =−16990 N oriented downward. B. Force =+180.25 N oriented downward; C. Force =16990 N oriented upward; D. Force =−180.25 N oriented downward;
The magnitude and direction of the force on a negative electric charge of -0.103C placed in a uniform electric field with a magnitude of 1750 N/C can be determined using the equation F = qE, where F is the force, q is the charge, and E is the electric field.
To find the magnitude of the force, we substitute the values into the equation:
F = (-0.103C) * (1750 N/C)
F = -180.25 N
The magnitude of the force is 180.25 N.
Since the charge is negative, the force will be directed in the opposite direction of the electric field. Therefore, the direction of the force is downward.
So, the correct answer is D. Force = -180.25 N oriented downward.
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Yeast is killed at a temperature of
a. 100ºF (38ºC)
b. 140ºF (60ºC)
c. 180ºF (82ºC)
d. 212ºF (100ºC)
Yeast is a type of fungus, also known as Saccharomyces cerevisiae, which is used in the process of baking, brewing, and fermentation.
The yeast, however, is sensitive to temperature and can be killed by heat.
The temperature at which yeast is killed is known as the lethal temperature.
The correct answer is d.
212ºF (100ºC).
Yeast is killed at a temperature of 212ºF (100ºC), which is the boiling point of water.
Yeast dies when exposed to high temperatures, and boiling water is the temperature at which the yeast cells are destroyed.
If the temperature of the liquid is higher than this point, the yeast will be killed instantly and the fermentation process will stop.
In summary, yeast is a microorganism that requires specific temperature conditions to thrive.
However, it is killed when exposed to high temperatures.
Boiling water at a temperature of 212ºF (100ºC) is enough to destroy yeast cells.
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The figure shows two blocks connected by a cord (of negligible mass) that passes over a frictionless pulley (also of negligible mass). The arrangement is known as Atwood's machine. Block 1 has mass m1=1.2 kg; block 2 has mass m2=1.8 kg. What are (a) the magnitude of the blocks' acceleration and (b) the tension in the cord? (a) Number Units (b) Number Units
The magnitude of the blocks' acceleration and the tension in the cord cannot be determined without specific numerical values for g or additional information. The acceleration depends on the difference in mass and the tension in the cord, while the tension depends on the forces acting on each block.
(a) To find the magnitude of the blocks' acceleration, we can use the concept of Newton's second law. The net force acting on the system is equal to the mass of the system multiplied by its acceleration. Considering the tension in the cord as the only force acting on the system, we can write the equation:
Tension = (m2 - m1) * acceleration
Where Tension is the tension in the cord, m2 is the mass of block 2, m1 is the mass of block 1, and acceleration is the magnitude of the blocks' acceleration.
(b) To determine the tension in the cord, we need to consider the forces acting on each block separately. For block 1, the tension pulls it upward, opposing the force due to gravity. For block 2, the tension pulls it downward, aiding the force due to gravity. The tension in the cord is the same for both blocks.
Equating the magnitudes of the forces on each block:
m1 * g - Tension = m1 * acceleration
Tension - m2 * g = m2 * acceleration
Solving these equations simultaneously will allow us to find the value of the tension in the cord.
Without specific numerical values for g or additional information, we cannot provide the exact answers for the magnitude of the blocks' acceleration or the tension in the cord.
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