The Lunar Excursion Module (LEM) was designed to make a soft landing on the lunar surface, which required that the LEM must not bounce back into space upon impact. The LEM, therefore, was modeled as a mass that was supported by four symmetrically located legs.
Each of these legs could be approximated as a spring-damper system with negligible mass.The design of the springs had to be such that the total energy of the system was dissipated during the landing without causing any structural damage to the LEM. This is because the energy of the landing must not cause the spacecraft to bounce back into space.The design of the springs was also affected by the nature of the lunar surface. The lunar surface was not homogeneous and, therefore, the spacecraft had to be designed to deal with different types of soil and rocks.
This meant that the springs had to be able to adjust to different soil types and absorb the energy of the impact.In addition, the design of the springs was also affected by the lunar environment. The temperature on the moon fluctuates widely between day and night. Therefore, the springs had to be designed to withstand extreme temperatures without losing their resilience.
Finally, the design of the springs was affected by the mass of the spacecraft. The springs had to be able to support the weight of the spacecraft without collapsing while also being light enough to not add too much weight to the spacecraft. This meant that the springs had to be designed using lightweight and strong materials such as titanium alloys.
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You measure the current through a 22.5 2 resistor to be 475 mA. What is the potential difference across the contacts of the resistor?
The potential difference across the contacts of the resistor is 10.69 V.
To find the potential difference across the contacts of the resistor, we need to use Ohm's Law, which states that the potential difference across a resistor is proportional to the current flowing through it and its resistance.
Mathematically, this can be represented as V = IR,
where V is the potential difference, I is the current, and R is the resistance. .
To apply this equation to the given problem, we can substitute the values given in the problem.
The current is 475 mA, which is equal to 0.475 A, and the resistance is 22.5 Ω.
Therefore, we have: V = IR = 0.475 A x 22.5 Ω
= 10.69 V
Therefore, the potential difference across the contacts of the resistor is 10.69 V.
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Please help with part A.
E = magnitude of electric field = 1000 N/C is incorrect.
E = 100cos(15) = 965.93 is also incorrect.
* Amount of charge is 1000 N/C at 15 degrees from horizontal. This is all the information provided for the problem. The electric field 6.0 cm from a small charged object is (1000 N/C, 15° above horizontal). Part A What is the magnitude of the electric field 6.0 cm in the same direction from the object? Express your answer with the appropriate units. 12 μA ? Units Request Answer Part B What is the direction of the electric field in the same point as in part A? Express your answer in degrees above horizontal. 0 Π| ΑΣΦ ? 0= Submit E= Submit Value Request Answer
The direction of the electric field in the same point as in Part A is 15° above horizontal.
Part A
In the problem, the electric field 6.0 cm from a small charged object is given as (1000 N/C, 15° above horizontal).
To find the magnitude of the electric field 6.0 cm in the same direction from the object, we will use the following formula:
E = Ecosθ
Here,
E = 1000 N/C and
θ = 15°.
E = 1000 N/C * cos(15°)
= 965.93 N/C
Therefore, the magnitude of the electric field 6.0 cm in the same direction from the object is 965.93 N/C.
Part B
To find the direction of the electric field in the same point as in Part A, we will use the following formula:
tanθ = Esinθ / Ecosθ
tanθ = 1000sin(15°) / 1000cos(15°)
= tan(15°)
θ = 15°
Therefore, the direction of the electric field in the same point as in Part A is 15° above horizontal.
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(11\%) Problem 1: An air-core solenoid has N=1900 turns, d=0.15 m length, and cross sectional areaA=0,025 m
2
Randomized Variables
N=1900 turns
d=0.15 m
A=0.025 m
2
A 50% Part (a) Express the inductance of the solenoid, L, in terms of N,d, and A. L Hints: deduction per hint. Hints remaining: 3 Feedback: 5φ
p
deduction per feedback. A 50% Part (b) Calculate the numerical value of L in henries.
I=4,75 A
L=6,5mH
t=8,01 ms
A What is the magnitude of the average induced emf, in volts, opposing the decrease of the cur ε
ave
=
I=18 A
t=1.7 ms
E=820 V
A What is the value of the self-inductance in mH ? A What value of self-inductance, L, in henries, is needed?
(A) solenoid L = (0.5 x μ x N² x A) / ld = 0.15 mN = 1900 turns = 0.025 m²
(B) |E| = 82.09 V
(C) 4.546 mHL = 0.365 H = 365 mH
(D) 0.365 H or 365 mH
(a) Inductance of the solenoid can be expressed as (0.5 × μ × N² × A)/l where μ is the permeability of free space, N is the number of turns, A is the cross-sectional area of the solenoid, and l is the length of the solenoid. L = (0.5 x μ x N² x A) / ld = 0.15 mN = 1900 turns = 0.025 m²
(b) Numerical value of L in henries is 0.365 H I = 4.75 A L = 6.5 mHt = 8.01 first, we need to convert 6.5 mH into henries. L = 6.5 mH = 0.0065 H Now, we can use the formula
V = -L(di/dt) to calculate the average induced emf, εave.|E| = 82.09 V
(c) The value of the self-inductance in mH is 4.546 mHL = 0.365 H = 365 mH
(d) The value of self-inductance, L, in henries, is needed is 0.365 H or 365 mH.
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convex mirrors can produce both real and virtual images.T/F
The statement : convex mirrors can produce both real and virtual images is False. Convex mirrors can only produce virtual images.
A virtual image is formed when the light rays appear to be coming from a location behind the mirror, regardless of the actual position of the object. In the case of convex mirrors, the reflected rays diverge, and the image formed is always virtual, diminished, and upright.
The virtual image in a convex mirror is formed by the apparent intersection of the diverging rays when traced backward. Convex mirrors are commonly used in applications where a wide field of view is necessary, such as in car side mirrors and surveillance systems.
They allow for a greater area to be observed, although the resulting image is smaller and appears closer than the actual object.
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To create sound echoes, reverberation filter is used to produce various reflection sound. Its output response is given as \( y(n)=x(n-1)-g * y(n-2) \) where \( x(n) \) is the input power level sequenc
A filter that produces sound echoes, reverberation filter, is used to create different reflected sounds. Its output response is given as \(y(n)=x(n−1)−g⋅y(n−2)\),
where \(x(n)\) is the input power level sequence of the sound, and the filter's coefficient, g, determines the strength of the reflections.
The sound waves reflect off the walls, floor, and ceiling, resulting in multiple copies of the original sound that combine to create the room's sound signature. Reverberation is the term for this.The reflected sound is more than simply a delayed version of the original sound. The frequency response, phase response, and envelope of the original sound are all affected by it.
The reflections are absorbed, diffused, or scattered by various surfaces in the room, causing a unique frequency and time response. The reverberation filter recreates these echoes by producing various reflected sounds.Reverberation filters can be implemented as digital filters, and a popular model is the Schroeder reverberator, which uses a comb filter and an all-pass filter in a feedback loop to produce a dense reverberation tail.
The output response of the filter is determined by the comb filter's delay length and all-pass filter's frequency response. The input signal is fed into the comb filter, which generates a series of delayed and attenuated copies of the signal. These delayed copies are then fed into the all-pass filter, which adjusts the phase of each delayed copy to create the diffuse echo effect.
The Schroeder reverberator can be implemented using the given equation, where the impulse response is given as[tex]\[h(n)=d^{n}u(n)\][/tex], where[tex]\[d\][/tex]is the delay length, and[tex]\[u(n)\][/tex]is the unit step function. The output response is obtained by convolving the impulse response with the input signal as[tex]\[y(n)=\sum_{k=0}^{\infty}h(k)x(n-k).\][/tex]
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The two blocks shown have masses of mA = 43 kg and mB = 76 kg . The coefficient of kinetic friction between block A and the inclined plane is μk = 0.12 . The angle of the inclined plane is given by θ = 40. Neglect the weight of the rope and pulley.
Part A - Determine the magnitude of the normal force acting on block A, NA. Express your answer to two significant figures in newtons.
Part B - If both blocks are released from rest, determine the velocity of block B when it has moved through a distance of s = 4.00 m. Express your answer to two significant figures and include the appropriate units.
Part C - If both blocks are released from rest, determine how far block A has moved up the incline when the velocity of block B is (vB)2 = 6.00 m/s. Express your answer to two significant figures and include the appropriate units.
a) The weight of the object perpendicular to the inclined plane is known as the normal force. The normal force is calculated as follows:
F = mg cosθ
= 43 kg × 9.8 m/s² × cos40°NA
= 318 N
b) The velocity of block B when it has moved through a distance of 4.00 m is calculated using the following kinematic equation: vB² = u² + 2asWhere,u = initial velocity of block B, u = 0a = acceleration of block B,
a = g sinθ - μk g cosθ
The distance traveled by block B, s = 4.00 m From the equation above,
vB² = 2 × 9.8 m/s² × sin40° - 0.12 × 9.8 m/s² × cos40° × 4.00 m
= 3.95 m²/s²vB
= 1.99 m/s
c) The velocity of block A is the same as the velocity of the rope since they are connected. Thus, vA = 1.99 m/s The distance block A moves up the incline can be calculated using the following kinematic equation:
sA = uA t + 1/2 a t²
The time taken, t can be found using the velocity and distance traveled by block B.
sB = uB t + 1/2 a t²
By the time block B moves 4.00 m, block A has moved up the inclined plane by a distance, sA. Therefore, the distance sA is given by:sA = sB sinθuA can be found using the following kinematic equation:
vA² = uA² + 2 a sAs
uA = 0,
sA = 1/2
vA² / a= 3.34 m
The distance block A has moved up the incline is 3.34 meters.
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Write down the ideal sinusoidal voltage, current and power functions. Using the above definitions, calculate rms voltage, current and power in time and in frequency domains.
In a sinusoidal voltage, current and power functions are essential for measuring the power consumption of a circuit. The ideal sinusoidal voltage, current and power functions are described as follows;Ideal sinusoidal voltage function:The ideal sinusoidal voltage function can be expressed as: v(t) = Vm sin(ωt + Φv)The variables in this function are as follows:
Vm is the maximum value of the sinusoidal voltage,ω is the angular frequency in radians per second,t is the time in seconds,Φv is the phase angle in radians.Ideal sinusoidal current function:The ideal sinusoidal current function can be expressed as: i(t) = Im sin(ωt + Φi)The variables in this function are as follows:Im is the maximum value of the sinusoidal current,ω is the angular frequency in radians per second,t is the time in seconds,
Φi is the phase angle in radians.Ideal sinusoidal power function:The ideal sinusoidal power function can be expressed as: p(t) = Vm Im cos(Φp)The variables in this function are as follows:Vm is the maximum value of the sinusoidal voltage,Im is the maximum value of the sinusoidal current,Φp is the phase angle between the voltage and current RMS voltage:RMS voltage can be defined as the square root of the mean of the squared voltage waveform over a cycle. VRMS = Vm / √2RMS current:RMS current can be defined as the square root of the mean of the squared current waveform over a cycle. IRMS = Im / √2RMS power:RMS power can be defined as the square root of the mean of the squared power waveform over a cycle.
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Please read the question carefully . Use MATLAB show
step by step solution .
Investigation of a unit negative feedback system with an open-loop
transfer
function of G(s) :
a. With the value K limit
In the question, we are given the open-loop transfer function of the negative feedback system. The transfer function of a system is the ratio of its output to its input under steady-state conditions. In this case, the output is the system's response to an input signal.
The transfer function of a negative feedback system is of the form:
[tex]G(s) = H(s)/(1 + G(s)H(s))[/tex]
Where G(s) is the open-loop transfer function and H(s) is the feedback function. The transfer function is used to analyze the behavior of the system. It can be used to determine the stability, transient response, and steady-state response of the system. Now, let's move on to the solution of the problem:Given, the open-loop transfer function of the negative feedback system is G(s).a. With the value of K limit To investigate the system, we need to plot the Bode plot of the open-loop transfer function.
The Bode plot is a graph of the magnitude and phase of the transfer function as a function of frequency. MATLAB can be used to plot the Bode plot of the open-loop transfer function.The magnitude of the transfer function is represented in decibels (dB) and the phase is represented in degrees. We can read off the gain margin and phase margin from the Bode plot. The gain margin is the amount of gain that can be added to the system before it becomes unstable. The phase margin is the amount of phase shift that can be added to the system before it becomes unstable.
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Conceptual Physics by Paul Hewitt
What are the 2 things that enter into every case where work is done?
Force and displacement are the two essential factors that consistently come into play in every scenario where work is performed, forming the foundation of understanding work and its relationship to physical systems.
In the field of physics, particularly in conceptual physics as described by Paul Hewitt, two fundamental factors come into play in every scenario where work is done. These factors are force and displacement.
Force is a vector quantity that describes the push or pull applied to an object. It is responsible for initiating or resisting motion. When work is done, force is required to exert an influence on an object and cause it to move or change its state.
Displacement, also a vector quantity, refers to the change in position of an object from its initial to final location. It is the path covered by the object as a result of the applied force. Displacement provides the distance and direction information for the movement caused by the force.
Work is defined as the product of force and displacement. When a force acts upon an object and causes it to move or undergo a displacement, work is done. The amount of work done depends on the magnitude and direction of the force, as well as the magnitude and direction of the displacement.
Thus, force and displacement are the two essential factors that consistently come into play in every scenario where work is performed, forming the foundation of understanding work and its relationship to physical systems.
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11. Would the two sides of equation 8.5 agree if the air track
had been inclined instead of level? If not, why?
8.5 equation: mA (VAi - VAf) = mB (VBi - VBf)
The two sides of equation 8.5 would not agree if the air track had been inclined instead of level because the gravitational potential energy(GPE) would vary due to the different heights above the ground level. Thus, the potential energies on both sides would be different.
The answer to the question about whether the two sides of equation 8.5 would agree if the air track had been inclined instead of level is no, they would not agree. The reason is that the inclined surface would cause the gravitational potential energy to vary. Here's an explanation: Air tracks are experimental setups that reduce friction (f)and allow the study of mechanics more closely. A track of this kind can be a level, flat surface. The level and inclined tracks have different potential energies(PE) due to differences in height (h)or distance(d) from the ground to the air track. In physics, the gravitational potential energy is the energy stored in an object that is due to its position relative to the Earth or another planet. When an object is lifted to a higher altitude, the potential energy increases, and when it is lowered to a lower altitude, the potential energy decreases .
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Gasoline (p = 680 kg/m3 and v = 4.29 x 10-7 m2/s) is transported at a rate of 240 L/s for a distance of 2 km. The surface roughness of the piping is 0.03 mm. If the head loss due to pipe friction is not to exceed 10 m, determine the minimum diameter of the pipe.
The minimum diameter of the pipe is 0.22 meters or 220 millimeters.
The minimum diameter of the pipe can be determined by the Darcy Weisbach equation.
Here's the formula: Darcy Weisbach equation: hf = (f L D V²) / (2 g)where
hf is the head loss due to pipe friction f is the friction factor
L is the length of the pipe
D is the diameter of the pipe
V is the velocity of the fluid
g is the acceleration due to gravity
For water, D is a function of Q. However, for gasoline, D is constant, so we will use the Darcy-Weisbach equation to calculate the required diameter of the pipe.
Let's use the given values in the above equation as follows: hf = 10 mL = 2000 m
Q = 240 L/s = 0.24 m³/s
D = ?
A = π/4 D² = (π/4) (D)²v = Q / A = (0.24 m³/s) / ((π/4) (D)²) = 0.3061 / D²g = 9.81 m/s²f = 0.003 (assuming commercial steel pipes)
Putting the above values in the Darcy Weisbach equation, we get:10 = (0.003 x 2000 x D x (0.3061/D²)²) / (2 x 9.81)
Simplifying, we get:
D³ = (0.003 x 2000 x 0.3061²) / (20 x 9.81)D³
= 0.0092413D
= 0.22 meters
Hence, the minimum diameter of the pipe is 0.22 meters or 220 millimeters.
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1. Which compressor that impart energy to the gas by converting velocity force to pressure.
2. Dynamic compressors also called:___________
3. Centrifugal compressors are of two types: ___________
The compressor that imparts energy to the gas by converting velocity force to pressure is known as Dynamic compressors, Dynamic compressors are also called Centrifugal compressors, Centrifugal compressors are of two types, axial and radial.
1.These compressors are used when there is a requirement for high pressure, low flowrate of compressed gas, or air.
The dynamic compressor also takes in high-speed air and imparts energy to the gas by converting velocity force to pressure. This type of compressor can be used in industries where there is a requirement for high pressure, low flow rate of compressed gas, or air.
2. These types of compressors are used for a wide range of applications and they are one of the most common types of compressors used in industry. The centrifugal compressor works by converting the kinetic energy of the gas into pressure energy.
It uses a high-speed impeller to impart velocity to the gas and then converts the velocity into pressure. These compressors are widely used in the oil and gas industry, as well as in chemical plants, power plants, and other industries.
3. Axial compressors are used for low-pressure applications while radial compressors are used for high-pressure applications. In an axial compressor, the air or gas flows parallel to the axis of rotation and is compressed by a series of rotating blades.
Radial compressors, on the other hand, have the gas flow perpendicular to the axis of rotation and are compressed by a series of rotating vanes or impellers.
Radial compressors are typically used for higher pressures and are more efficient than axial compressors. Overall, centrifugal compressors are widely used in industry due to their efficiency, reliability, and flexibility in different applications.
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A bird flies from her nest at 8:15 AM and flies 8.4 km toward the WEST to point A. She arrives at point A at 2:00 PM. She then flies from point A 4.5 km toward the WEST to point B and arrives at point B at 6:30 PM. The bird's average velocity for the entire trip is
A. 2.6km/h towards west
b. 0.02km/h towards the west
c. 0.02km/h towards the east
d. 1.3km/h towards the east
e. 1.3km/h towards the west
The correct option is (e) 1.3km/h towards the west. The average velocity of the bird is 1.26 km/h towards the west.
The bird flies 8.4 km west in 2:00 PM - 8:15 AM = 5:45 hours = 5.75 hours to reach point A.
Her velocity is, therefore:
velocity = displacement/time
velocity = -8.4 km / 5.75 hours
velocity = -1.46 km/h west
The negative velocity implies that the bird flies towards the west.
From point A, the bird flies west again, this time for 4.5 km for 6:30 PM - 2:00 PM = 4.5 hours = 4.5 hours.
The velocity of the bird, once more, is:
velocity = displacement/time
velocity = -4.5 km / 4.5 hours
velocity = -1 km/h west
Again, the negative velocity implies that the bird flies towards the west.
To find the bird's average velocity for the entire trip, we need to divide the total displacement of the bird by the time taken to cover this displacement.
We can calculate the displacement as follows:
displacement = -8.4 km + (-4.5 km)
displacement = -12.9 km
The total time taken to travel the distance is:
time = 4.5 hours + 5.75 hours
time = 10.25 hours
Therefore, the average velocity of the bird is:
average velocity = displacement/time
average velocity = -12.9 km / 10.25 hours
average velocity = -1.26 km/h west
The average velocity of the bird is 1.26 km/h towards the west. Therefore, the option (e) 1.3km/h towards the west is the correct answer.
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A three-phase lossless transmission line has length 1 = 200 km, and the following parameters (per phase, per km of length): self-inductance Lş = 1.6 mH/km, mutual inductance Lm = 0.6 mH/km, self- capacitance C₁ = 16 nF/km, mutual capacitance Cm = 1.6 nF/km. At the receiving end of the line, there is a three-phase star connected resistance of 600 Ohm (per phase). Determine characteristic impedances, propagation velocities and one-way propagation times for the three transmission transient modes (mode 0, 1 and 2).
The values of impedance, propagation velocity and one-way propagation time for the three transmission transient modes (mode 0, 1, and 2) are given above.
For a three-phase lossless transmission line, the following are the given parameters (per phase, per km of length):
self-inductance Lş = 1.6 mH/km,
mutual inductance Lm = 0.6 mH/km,
self- capacitance C₁ = 16 nF/km,
mutual capacitance Cm = 1.6 nF/km.
Velocity: Propagation velocity (v) is given by the formula:$$v = \frac{1}{\sqrt{L_{ș}(C_{1}+C_{m})}}$$One-way propagation time: Mode Characteristic Impedance (Z0)(Ω)Propagation Velocity(v)(m/s)One-way propagation time (t)(ms)0Z0 = 76.10v
= 1.50 × 10^8t
= 1.33 × 10^31Z0
= 115.16v
= 1.50 × 10^8t
= 0.88 × 10^32Z0
= 104.13v
= 1.50 × 10^8t
= 1.00 × 10^3
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Suppose that you take data and fill the Table-1 of your lab sheet (page7) for an applied current of 1.01A using colts with 10 cm radius. Then, assume that after plotting the data as instructed in Part-1 of your analysis (page6) you choose the following slope points on your fitted line: (0;0mT) (2.9;0.019mT) From the slope, calculate the experimental value for po Express your answer in units of mT* mm/A, (MiliTesla Milimeter/ Amperes)with two decimals.
The experimental value for po is [tex]13509.23 mT*mm/A[/tex] (two decimal places).
Given the applied current, i = 1.01A and the radius of the colts is 10 cm.
The slope points on the fitted line are (0;0mT) and (2.9;0.019mT).Find the experimental value for po with the following steps.
Step 1:Calculate the slope of the graph by using the slope points on the fitted line.
Slope (m) = y₂ - y₁ / x₂ - x₁= (0.019 - 0) / (2.9 - 0)
Slope (m) = 0.00655 mT/mm.
Step 2:Calculate the magnetic field intensity for the given applied current by using the following formula;
[tex]B = µo * i * n * r² / (2 * r)Where µo = 4π * 10⁻⁷ Tm/A[/tex] is the permeability of free space.
n = 130 is the number of turns per unit length.
r = 0.1 m is the radius of the colts.
i = 1.01A is the applied current.
So, B = 2.066 * 10⁻³ T or 2.066 mT.
Step 3:Calculate the experimental value for po by using the following formula;
[tex]po = m * B * 10⁶ \\po = 0.00655 * 2.066 * 10⁶\\po = 13509.23 mT*mm/A[/tex]
Therefore, the experimental value for po is 13509.23 mT*mm/A (two decimal places).
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A slit 0.370 mm wide is illuminated by parallel rays of light that have a wavelength of 560 nm. The diffraction pattern is observed on a screen that is 1.00 m from the slit. The intensity at the center of the central maximum (0 = 0°) is Io. What is the distance on the screen from the center of the central maximum to the first minimum? Express your answer in millimeters. ₁ 1.5 mm Submit Previous Answers ✓ Correct Correct answer is shown. Your answer 1.51352 mm was either rounded differently or used a different number of significant figures than required for this part. Part B What is the distance on the screen from the center of the central maximum to the point where the intensity has fallen to ? ((Hint: Your equation for cannot be solved analytically. You must use trial and error or solve it graphically.) Express your answer in millimeters. IVE ΑΣΦ ? y = 0.75 Submit Previous Answers Request Answer X Incorrect; Try Again; 2 attempts remaining mm
The distance on the screen from the center of the central maximum to the first minimum is found by using the formula `dsin θ = mλ`. The distance on the screen from the center of the central maximum to the first minimum is 1.51 mm, and the distance on the screen from the center of the central maximum to the point where the intensity has fallen to `y = 0.75 Io` is 0.34 mm.
Given:Width of slit, a = 0.370 mm
Wavelength of light, λ = 560 nm
Distance from slit to screen, D = 1.00 m
Formula used:
For the first minimum,
`θ = sin⁻¹ (λ/a)`
Therefore,
`sin θ = λ/a`
= `(560 × 10⁻⁹)/0.370 × 10⁻³
` = 1.51 × 10⁻⁶
First minimum is given by the equation
`dsin θ = mλ`
Taking m = 1,
`d × 1.51 × 10⁻⁶
= 560 × 10⁻⁹`d
= 1.51 mm
The distance on the screen from the center of the central maximum to the point where the intensity has fallen to
`y = 0.75 Io`
is given by the equation
`sin θ = ± (√y/y_max)`.
Where
`y_max = Io`.
The distance on the screen from the center of the central maximum to the point where the intensity has fallen to
`y = 0.75 Io`
is found using trial and error.We assume that
`y = 0.75 Io` at `θ = 20°`.
Therefore,
`sin 20° = ± (√0.75)`
The negative value is discarded. Hence
`sin 20° = √0.75`.
Using
`sin 20° = 0.342`,
we get
`y = y_max × 0.75 = 0.75 Io`.
For the point where the intensity has fallen to
`y = 0.75 Io`,
`θ = 20°` and
`dsin θ = D × sin θ = 1.00 × sin 20°`.
Thus, `d = 0.34 mm`.
Therefore, the distance on the screen from the center of the central maximum to the first minimum is 1.51 mm, and the distance on the screen from the center of the central maximum to the point where the intensity has fallen to `y = 0.75 Io` is 0.34 mm.
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Question 1 A hospital in Darwin needs 24ug (micrograms) of the radioisotope technetium - 99, dispatched from Sydney to satisfy the Darwin order? Give your answer in micrograms didered from Sydney. The
The amount of Tc-99m dispatched from Sydney to Darwin is approximately 12 micrograms (150 words).
Technetium-99m (Tc-99m) is the most common medical radioisotope used in diagnostic imaging. It is produced from molybdenum-99 (Mo-99), which is a parent radioisotope and undergoes beta decay to produce Tc-99m. Hence, Tc-99m has a short half-life (6 hours) and decays by emitting gamma radiation that can be detected by imaging equipment, making it ideal for medical imaging
.A hospital in Darwin requires 24ug (micrograms) of the radioisotope technetium - 99. The radioisotope is dispatched from Sydney to satisfy the Darwin order, which means that the hospital in Darwin will receive the radioisotope from Sydney.
The half-life of Tc-99m is 6 hours, which means that half of the initial activity will decay after 6 hours.
Using the following formula, we can calculate the activity of Tc-99m that will be dispatched from Sydney to Darwin, given the decay constant and time of transportation:
Activity = Initial Activity x (1/2)t/t1/2
where t is the time of transportation (in hours), t1/2 is the half-life of Tc-99m (in hours), and the initial activity is the amount of Tc-99m at the time of dispatch (in microcuries or millicuries).
Since the question gives the amount required in micrograms, we need to convert it to millicuries, as the initial activity is usually measured in millicuries.
The specific activity of Tc-99m is approximately 2.2 Ci/mg (curies per milligram), which means that 1 millicurie (mCi) of Tc-99m is equivalent to 22 micrograms (ug).
Hence, the amount of Tc-99m required by the hospital in Darwin is:
24 ug x (1 mg/1000 ug) x (1 mCi/22 ug) = 1.09 x 10-3 mCi
Now, we can calculate the activity of Tc-99m that will be dispatched from Sydney to Darwin, assuming a transportation time of 6 hours:
Activity = 1.09 x 10-3 mCi x (1/2)6/6 = 5.44 x 10-4 mCi
To convert this to micrograms, we use the specific activity of Tc-99m:5.44 x 10-4 mCi x (22 ug/1 mCi) = 1.20 x 10-2 ug
Hence, the amount of Tc-99m dispatched from Sydney to Darwin is approximately 12 micrograms.
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Assume the Fermi energy level is exactly in the center of the band-gap energy of a semiconductor at T=300 K. (a) Calculate the probability that an energy state at E=Ec+kgI is occupied by an electron for Si, Ge, and GaAs. (b) Calculate the probability that an energy state at E= Ev-kgt is empty for Si, Ge, and GaAs.
a. For Si: [tex]= 0.56 \, \text{eV}[/tex], For Ge: [tex]= 0.335 \, \text{eV}[/tex], For GaAs: [tex]= 0.715 \, \text{eV}[/tex]
b. the probabilities for the energy states in the top of the valence band are:
[tex]\[ f(E)_{\text{Si}} = 1 \]\\\\f(E)_{\text{Ge}} = 1 \]\\\ f(E)_{\text{GaAs}} = 1 \][/tex]
To calculate the probability that an energy state in the bottom of the conduction band is occupied by an electron, we can use the Fermi-Dirac distribution function:
[tex]\rm \[ f(E) = \frac{1}{1 + e^{\frac{E - E_F}{kT}}} \][/tex]
where:
[tex]\( f(E) \)[/tex] = Probability that the energy state with energy E is occupied by an electron
E = Energy of the state
[tex]\rm \( E_F \)[/tex] = Fermi energy level
k = Boltzmann constant [tex](\( 8.617333262145 \times 10^{-5} )[/tex] eV/K, or you can use ([tex]\( 8.617333262145 \times 10^{-5} \)[/tex] eV/K for better accuracy)
T = Temperature in Kelvin
For part (a), the Fermi energy level is in the center of the bandgap energy, so [tex]\( E_F = \frac{E_{\text{gap}}}{2} \)[/tex], where [tex]\( E_{\text{gap}} \)[/tex] is the bandgap energy of the semiconductor.
Given the bandgap energies for Si, Ge, and GaAs are approximately 1.12 eV, 0.67 eV, and 1.43 eV, respectively, and [tex]\rm \( T = 300 \)[/tex] K, we can calculate the probabilities for each semiconductor.
For Si:
[tex]\[ E_F = \frac{1.12 \, \text{eV}}{2} \\\\= 0.56 \, \text{eV} \][/tex]
For Ge:
[tex]\[ E_F = \frac{0.67 \, \text{eV}}{2}\\\\= 0.335 \, \text{eV} \][/tex]
For GaAs:
[tex]\[ E_F = \frac{1.43 \, \text{eV}}{2} \\\\= 0.715 \, \text{eV} \][/tex]
Now, we can use the Fermi-Dirac distribution function to calculate the probabilities:
For Si:
[tex]\[ f(E) = \frac{1}{1 + e^{\frac{E - 0.56 \, \text{eV}}{k \times 300 \, \text{K}}}} \]\\\\\ f(E) = \frac{1}{1 + e^{\frac{E - 0.56 \, \text{eV}}{0.0259 \, \text{eV}}}} \][/tex]
For Ge:
[tex]\[ f(E) = \frac{1}{1 + e^{\frac{E - 0.335 \, \text{eV}}{k \times 300 \, \text{K}}}} \]\\\\\\ \[f(E) = \frac{1}{1 + e^{\frac{E - 0.335 \, \text{eV}}{0.0259 \, \text{eV}}}} \][/tex]
For GaAs:
[tex]\[ f(E) = \frac{1}{1 + e^{\frac{E - 0.715 \, \text{eV}}{k \times 300 \, \text{K}}}} \]\[ f(E) = \frac{1}{1 + e^{\frac{E - 0.715 \, \text{eV}}{0.0259 \, \text{eV}}}} \][/tex]
b.
To calculate the probability that an energy state in the top of the valence band is empty, we can use the Fermi-Dirac distribution function again.
For part (b), we can assume [tex]\( f(E) = 1 \)[/tex] (almost completely filled) because the energy states in the valence band are already filled with electrons.
Therefore, the probabilities for the energy states in the bottom of the conduction band are:
[tex]\[ f(E)_{\text{Si}} = \frac{1}{1 + e^{\frac{E - 0.56 \, \text{eV}}{0.0259 \, \text{eV}}}} \]\[ f(E)_{\text{Ge}} = \frac{1}{1 + e^{\frac{E - 0.335 \, \text{eV}}{0.0259 \, \text{eV}}}} \]\[ f(E)_{\text{GaAs}} = \frac{1}{1 + e^{\frac{E - 0.715 \, \text{eV}}{0.0259 \, \text{eV}}}} \][/tex]
And the probabilities for the energy states in the top of the valence band are:
[tex]\[ f(E)_{\text{Si}} = 1 \]\\\\f(E)_{\text{Ge}} = 1 \]\\\ f(E)_{\text{GaAs}} = 1 \][/tex]
The probabilities calculated will give us the likelihood of an energy state being occupied by an electron for each semiconductor at a temperature of 300 K and Fermi energy level in the center of the bandgap.
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How many moles of helium atoms are in 7.94 cubic meters of helium gas at a temperature of 298 K and 101,000 Pa of pressure?
At a temperature of 298 K and a pressure of 101,000 Pa, a volume of 7.94 cubic meters of helium gas corresponds to approximately 817.14 moles of helium atoms. This calculation is based on the application of the ideal gas law equation, which relates pressure, volume, temperature, and the number of moles.
By rearranging the equation and substituting the given values, the number of moles can be determined. This information is valuable for quantifying the number of helium atoms present in a given volume of gas and understanding the behavior of gases. The ideal gas law provides a fundamental framework for analyzing gas properties and enables the calculation of various gas-related parameters.
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b. A tape measure is made of a particular material which has a linear thermal expansion coefficient of 20×10
−6
K
−1
. At −10
∘
C, using it you measure a piece of the material (which has a linear thermal expansion coefficient of 80×10
−6
K
−1
) to have a length of 10 m. What length would the tape measure say the piece of material has at 30
∘
C ? Assume the tape measure if marked to the mm level, and give your answer to that level of accuracy. [15 pts]
The length measurement of the material at `30°C` would be `10.040 m`.
Given that, A tape measure is made of a particular material which has a linear thermal expansion coefficient of `20×10^(-6)` K^(-1).At `-10°C`, using it you measure a piece of the material (which has a linear thermal expansion coefficient of `80×10^(-6)` K^(-1)) to have a length of `10 m`.
We need to find what length the tape measure would say the piece of material has at `30°C`.
Formula used: `∆L = Lα∆T` where, ∆L = Change in length L = Lengthα = Coefficient of linear expansion ∆T = Change in temperature
Length measurement of the material at `-10°C`, L₁ = `10 m`
Coefficient of linear expansion of the material, α₁ = `80×10^(-6)` K^(-1)
To find Length measurement at `30°C`
Coefficient of linear expansion of the tape measure, α₂ = `20×10^(-6)` K^(-1)
Change in temperature, ∆T = (`30°C`) - (`-10°C`) = `40°C`
Change in length, ∆L = Lα∆T = `10×80×10^(-6)×40 = 0.032 m`
Increase in length of the tape measure, ∆L₂ = L₂α₂∆T = `10×20×10^(-6)×40 = 0.008 m`
Total length at `30°C` = L + ∆L + ∆L₂ = `10 + 0.032 + 0.008 = 10.040 m`
Therefore, the length measurement of the material at `30°C` would be `10.040 m`.
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12) A Boat is traveling at 4 m/s north relative to the water on a river that is flowing east at 2 m/s.
A) What is the boats velocity relative to the ground?
B) How far downstream does the boat drift in 10s?
C) How long does it take the boat to move 100m across the river?
The time taken by the boat to move 100 meters across the river is 50 seconds.
Given data:
Velocity of Boat= 4 m/s (North)
Velocity of river= 2 m/s (East)
A) Velocity of boat relative to ground = √(4² + 2²)
≈ 4.47 m/s (northeastward)
B) Distance travelled downstream in 10 seconds
= Velocity of river × time taken
= 2 m/s × 10 s
= 20 meters
C) Distance travelled towards east in 1 second
= Velocity of river
= 2 m/s
Distance to be covered towards east = 100 meters
So, time taken = Distance/Speed
= 100 m/2 m/s
= 50 seconds
Therefore, the time taken by the boat to move 100 meters across the river is 50 seconds.
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Write the Schroedinger equation and explain how Max Born interpreted this equation to describe the behavior of quantum-mechanical particles.
The Schrödinger equation describes quantum particles, and Max Born interpreted it as the probability distribution of particle behavior.
The Schrödinger equation is a fundamental equation in quantum mechanics that describes the behavior of quantum-mechanical particles. It is given by:
iħ ∂Ψ/∂t = ĤΨ
In this equation, ħ is the reduced Planck constant, t represents time, Ψ is the wave function of the particle, and Ĥ is the Hamiltonian operator, which represents the total energy of the system.
Max Born interpreted the Schrödinger equation in a profound way. He proposed that the square of the absolute value of the wave function, |Ψ|^2, represents the probability density of finding a particle at a particular position in space.
Born's interpretation introduced the concept of wave function collapse upon measurement, stating that when a measurement is made, the wave function "collapses" to a specific value, corresponding to the observed state of the particle.
This interpretation revolutionized the understanding of quantum mechanics by providing a probabilistic framework for predicting the behavior of quantum particles.
Born's interpretation emphasized that quantum particles do not possess well-defined properties until measured, and their behavior is inherently probabilistic. The square of the wave function, or the probability density, provides a statistical description of the likelihood of finding a particle in a particular state.
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Sakshi is on her way to the Grand Mall from her apartment. She walks 5 blocks west, 3 blocks south, 6 blocks east, and 3 blocks north. Her displacement is a. 1 block [E] b. 5 blocks [W] c. 17 blocks d. 17 blocks [SE] 3. An object is thrown vertically upward at 25.0 m/s. If it experiences an acceleration due to gravity of 9.8 m/s
2
[down], what is the object's velocity 3.0 s later? a. 22.0 m/s[D] b. 4.4 m/s[D] c. 22.0 m/s[U]d.4.4 m/s[U] 4. The force of friction always acts in a direction exactly opposite to the a. Net force b. applied force c. Motion d. Normal force 5. Newton's third law essentially states a. acceleration only occurs if there is net force. b. Objects won't move unless pushed c. Forces always occur in pairs d. Objects which are moving tend to stay moving
1. Her displacement is 17 blocks [SE].
2. The object's velocity 3.0 s later is 4.4 m/s [down]. So the correct option is d.
4. The force of friction always acts in a direction exactly opposite to the motion.
5. The second object exerts an equal and opposite force on the first object.
1. Sakshi is on her way to the Grand Mall from her apartment. She walks 5 blocks west, 3 blocks south, 6 blocks east, and 3 blocks north. Her displacement is 17 blocks [SE]. So the answer is 17 blocks [SE] . We can use the Pythagorean theorem to find the magnitude and direction of the displacement. The displacement is the vector difference between the initial and final positions of the object. The magnitude of the displacement is given by the distance between the initial and final positions.Using Pythagoras' theorem, we getDisplacement = √(5² + 3² + 6² + 3²) = √(25 + 9 + 36 + 9) = √79Thus, the magnitude of the displacement is 8.89 blocks. We can use the tangent function to find the direction of the displacement.
2. An object is thrown vertically upward at 25.0 m/s. If it experiences an acceleration due to gravity of 9.8 m/s² [down], The initial velocity of the object, u = 25.0 m/sThe acceleration due to gravity, a = 9.8 m/s²The time, t = 3.0 using the formula:v = u + substituting the given values, we get:v = 25.0 - 9.8 × 3.0v = 25.0 - 29.4v = -4.4 m/sThe negative sign indicates that the object is moving downwards. Therefore, the object's velocity 3.0 s later is 4.4 m/s [down]. So the correct option is d.
4. The force of friction always acts in a direction exactly opposite to the motion.
5. Newton's third law essentially states that forces always occur in pairs. The third law states that for every action, there is an equal and opposite reaction. This means that whenever one object exerts a force on another object.
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3. A pump draws water at 300 liters per second from reservoir A and lifts it to reservoir B as shown. The head loss from A to 1 is 20 times the velocity head in the 200 mm diameter and the head loss from 2 to B is 20 times the velocity head in the 150-mm diameter pipe. Assume your own reservoir B elevation then compute for the energy that must be supplied to the pump in kW if said appurtenance has an efficiency of 80%. Compute also the pressure at points 1 and 2. Reservoir A 200 mm pipe | julod. Elevation=-20 m Point 2 Pump 150 mm Reservoir B 7
The pressure at point 1 is calculated as = 5.010 × 10⁶ Pa and the pressure at point 2 is calculated as to be equal to 4.998 × 10⁶ Pa.
The head loss from 2 to B = 20 times the velocity head in the 150-mm diameter pipe. Efficiency of the pump = 80%.Formulae used: Energy supplied by the pump = Head × Discharge × Weight of water × Gravity ÷ 3600 ÷ 1000 ÷ Efficiency. Pressure at a point = (Velocity head + Datum head + Pressure head).
Energy supplied by the pump: From the given data, the head from A to B is, Head = Head loss from A to 1 + Head loss from 2 to B + Elevation difference
Between A and B = 20 × Velocity head in 200 mm diameter pipe + 20 × Velocity head in 150 mm diameter pipe + Elevation of B - Elevation of A.
Hence, Head = 20 × [(Velocity in 200 mm diameter pipe)² ÷ 2g] + 20 × [(Velocity in 150 mm diameter pipe)² ÷ 2g] + (Elevation of B - Elevation of A)= 20 × [(3000 / π / (0.2)²)² ÷ 2 × 9.81] + 20 × [(3000 / π / (0.15)²)² ÷ 2 × 9.81] + Elevation of B - (- 20)= 124.63 + 416.71 + Elevation of B + 20
Therefore, Head = 541.34 + Elevation of B. Here, the elevation of B is not given, so we assume it to be 10 m above the datum level.
Therefore, Elevation of B = - 20 + 10
= - 10 m.
Hence, Head = 541.34 - 10
= 531.34 m.
Since the discharge of water = 300 liters/sec
= 0.3 m³/sec.
The weight of water = 0.3 × 1000 kg/m³
= 300 kg/s.
So, energy supplied by the pump = Head × Discharge × Weight of water × Gravity ÷ 3600 ÷ 1000 ÷ Efficiency.
= 531.34 × 0.3 × 300 × 9.81 ÷ 3600 ÷ 1000 ÷ 0.8.
= 54.98 kW.
Pressure at point 1: Velocity in the 200 mm diameter pipe is given by, Q = πd²/4 × V.
= π/4 × (0.2)² × V.
= 3000 L/s
= 3 m³/s.
Therefore, V = Q / π/4 × (0.2)²
= 3 / π/4 × 0.04
= 2.39 m/s.
Velocity head at point 1 = V²/2g
= 2.39²/2 × 9.81
= 0.289 m.
The datum head is - 20 m.
Therefore, the pressure head at point 1 = 531.34 - 20 - 0.289
= 511.05 m.
Hence, the pressure at point 1 = 511.05 × 1000 × 9.81
= 5.010 × 10⁶ Pa.
Pressure at point 2:Velocity in the 150 mm diameter pipe is given by, Q = πd²/4 × V.
= π/4 × (0.15)² × V.
= 3000 L/s
= 3 m³/s.
Therefore, V = Q / π/4 × (0.15)²
= 3 / π/4 × 0.0225.
= 5.305 m/s.
Velocity head at point 2 = V²/2g
= 5.305²/2 × 9.81
= 1.465 m.
The datum head is - 20 m.
Therefore, the pressure head at point 2 = 531.34 - 20 - 1.465
= 509.875 m.
Hence, the pressure at point 2 = 509.875 × 1000 × 9.81
= 4.998 × 10⁶ Pa.
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A smooth wooden block is placed on a smooth wooden table top. You find that you must exert a force of 14 N to keep the 40 N blocks moving a constant velocity.
a.) What is the coefficient of sliding friction for the block and the table?
b.) If a 20 N Brick is placed on the block, what force will be required to keep the block and brick moving at constant velocity?
The force required to keep the block and brick moving at constant velocity is 46 N.
Given data:
Force needed to keep the block moving with constant velocity = 14 N
Weight of the wooden block = 40 N
Weight of the brick = 20 N
We have to calculate:
a) Coefficient of sliding friction between the block and the table.
b) Force needed to keep the block and brick moving at constant velocity.
Calculation:
a) Coefficient of sliding friction between the block and the table:
Let μ be the coefficient of sliding friction between the block and the table and n be the normal force between the block and the table.
μ = Force of friction / Normal force
We know that normal force is equal to the weight of the block.
n = 40
N = Weight of the block
Force of friction = 14 N (as the block is moving at a constant velocity)
μ = 14 / 40
μ = 0.35
Therefore, the coefficient of sliding friction between the block and the table is 0.35.
b) Force needed to keep the block and brick moving at constant velocity:
For the block and brick to move at a constant velocity, the force required to move the block and brick together should be equal to the force of friction acting on the block and table.
Forces acting on the block and brick:
1) Weight of the block and brick acting downwards
2) Force of friction acting upwards
Net force acting on the block and brick = (Weight of the block + Weight of the brick) - Force of friction
Net force acting on the block and brick = (40 + 20) N - 14 N
Net force acting on the block and brick = 46 N
Force required to keep the block and brick moving at constant velocity = 46 N
Therefore, the force required to keep the block and brick moving at constant velocity is 46 N.
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3. With an aid of a diagram/s discuss the switching speed of a transistor. [10]
4. With an aid of a diagram discuss the optical system and pickup. [9]
The optical system and pickup is essential for the operation of a CD player, as it allows the device to read the information stored on a CD.
3. Switching speed of a transistor:
Switching speed of transistor refers to the time taken by the transistor to transition from its ON state to OFF state, or vice versa. Transistor switching speed is an important factor to consider in many electronic circuits because it influences the overall performance of the system.
The speed of the switching transistor can be analysed by its current-voltage (I-V) characteristics. The I-V characteristics of the switching transistor will show how the device performs when a voltage is applied across its terminals.
The switching speed of a transistor is influenced by various factors like base current, temperature, collector current, base resistance, and so on.
A faster switching transistor is desirable because it allows the device to operate more quickly, thus improving the performance of the electronic circuit.
4. Optical system and pickup:
An optical system and pickup is an important component of a compact disc (CD) player that is responsible for reading the digital information stored on a CD.
The optical system and pickup is made up of a laser diode, a lens system, a photodetector, and associated electronics. The operation of the optical system and pickup can be understood by examining the diagram below.
The laser diode emits a laser beam which is focused onto the surface of the CD by a lens system. As the CD rotates, the laser beam reflects off the CD surface, and the reflected beam is detected by a photodetector.
The electronics associated with the photodetector convert the light signal into an electrical signal, which is then sent to a digital-to-analog converter (DAC) to produce an audio signal.
The optical system and pickup is essential for the operation of a CD player, as it allows the device to read the information stored on a CD.
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Explain why must copper-based communications links be a circuit
(or loop)? Explain in detail.
Do not attach your answer as a photo, please!!!
Copper-based communications links must be a circuit (or loop) because of the nature of copper. Copper is an excellent conductor of electricity, meaning that it can transmit electrical signals over long distances with minimal loss of signal strength.
Copper is also susceptible to electromagnetic interference (EMI), which can cause noise and other distortions in the signal. By creating a closed loop or circuit, the electrical signals traveling through the copper can be protected from EMI, making the communication link more reliable and secure. A circuit is created by connecting two or more devices together so that they can communicate with each other.
For example, a telephone line is a circuit that connects a telephone at one end to a telephone network at the other end. In a copper-based communication link, a circuit is created by connecting two or more copper wires together to form a loop.
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2) Suppose you wanted to use an electron microscope to see individual atoms that visible light can't see. Would you want fast moving electrons or slow moving electrons? Why?
Fast moving electrons would be better than slow moving electrons to see individual atoms that visible light can't see.
An electron microscope is a type of microscope that uses electrons instead of visible light to produce an image. The wavelength of electrons is much shorter than that of visible light, which allows electron microscopes to produce much higher-resolution images. The two types of electron microscopes are transmission electron microscopes (TEMs) and scanning electron microscopes (SEMs).
A TEM works by firing a beam of electrons through a thin specimen, allowing the electrons to pass through the specimen and create an image on a screen. SEMs, on the other hand, fire a beam of electrons at the surface of a specimen and use the reflected electrons to create an image.
While both types of electron microscopes use electrons to produce images, the speed of the electrons is an important factor in their ability to resolve individual atoms. In order to see individual atoms, the electrons need to have a very short wavelength, which requires them to be moving very quickly. Therefore, fast moving electrons would be better than slow moving electrons to see individual atoms that visible light can't see.
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Derive the I-V equation of the Schottky Diode (n-type semiconductor) and draw the I-V characteristic curves as Linear Scale and Semi-Log Scale.
A Schottky diode is a type of diode that uses a metal-semiconductor junction rather than a p-n junction to generate a rectifying action. A metal-semiconductor junction is created when a metal is placed on an n-type semiconductor material like silicon.
When a voltage is applied, the diode becomes forward biased, and a current flows. When the voltage is reversed, no current flows across the junction.In forward bias, electrons flow from the n-type semiconductor material to the metal and combine with holes in the metal. As a result, a depletion region is formed near the junction, which increases in size as the forward bias voltage is increased.
When the depletion region reaches the metal-semiconductor junction, it becomes very thin, allowing electrons to flow across the junction and into the metal. As a result, current flows across the junction. The I-V equation of a Schottky diode can be derived as follows:$$I=I_0[e^{\frac{qV}{nkT}}-1]$$Where:I = Current flowing through the diodeI0= Reverse saturation current, also called the diode’s leakage currentq = Charge of an electronk = Boltzmann’s constantT = TemperatureV = Voltage applied across the dioden = Ideality factor (usually between 1 and 2)The I-V characteristic curves for a Schottky diode can be plotted on both linear and semi-log scales. The linear scale plots current versus voltage in a straight line, whereas the semi-log scale plots current versus voltage on a logarithmic scale.
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After confirming that your pet electron Elecpatra was safe (thank goodness she doesn't need food and water), she gave you a request: she wanted some friends of her own kind. She says the more the merrier, but you had space constraints in your apartment. All you could afford was a 3D infinite well of Lx = 20 pm, Ly = 30 pm, and Lz = 20 pm. You also had an energy constraint--considering your energy level, the highest energy you could afford for each electron was T²² 6 2mL2 ? where m is the mass of an electron and L = Lx = 20 pm. Assuming that this system will in its ground state, what is the maximum number of electrons you can add for your dear pet electron? Include spin and do not count Elecpatra. Note (for those more used to h than hbar), T22 h2 8mL 2mL2 9 10 O 11 12
The highest energy level for each electron you could afford was T²² 6 2mL2. You have a 3D infinite well of Lx = 20 pm, Ly = 30 pm, and Lz = 20 pm. Assuming that this system will be in its ground state, calculate the maximum number of electrons that you can add for your pet electron, including spin, and excluding Elecpatra.
The highest energy level for each electron you could afford was T²² 6 2mL2. You have a 3D infinite well of Lx = 20 pm, Ly = 30 pm, and Lz = 20 pm. Assuming that this system will be in its ground state, calculate the maximum number of electrons that you can add for your pet electron, including spin, and excluding Elecpatra. We can use the formula for the total number of states as follows: N = (2j + 1)N1N2N3, where N1, N2, N3 are the numbers of nodes in each dimension, and j is the spin quantum number. Here, we have Lx = Ly = 20 pm, and Lz = 30 pm. Since the wave function vanishes at the walls of the well, we have nodes at x = 0, Lx, y = 0, Ly, z = 0, Lz. This gives us N1 = 1, N2 = 1, and N3 = 2.
The spin quantum number j = 1/2 for electrons, and the maximum number of electrons that can fit into each state is 2 (Pauli exclusion principle). The number of states is given by the formula:
N = 2 × (1/2 + 1) × 1 × 1 × 2 = 4
The maximum number of electrons that can be added is therefore: N = 4 × (20 pm / 5.29 × 10⁻¹¹ m)³ × (9.11 × 10⁻³¹ kg) / (2 × 1.05 × 10⁻³⁴ J s)² × (6.626 × 10⁻³⁴ J s / 2π)² = 1.79 × 10⁸ or 179 million electrons
We can find the maximum number of electrons that can be added to the 3D infinite well by calculating the total number of states allowed by the system. The wave function for each state must vanish at the walls of the well, which gives us nodes at the edges of the box. The number of nodes in each dimension is given by N1, N2, N3. The total number of states is given by the formula: N = (2j + 1)N1N2N3, where j is the spin quantum number.
The maximum number of electrons that can be added to each state is 2, due to the Pauli exclusion principle. The highest energy level for each electron is T²² 6 2mL2, where m is the mass of an electron and L = Lx = 20 pm. In this problem, we have Lx = Ly = 20 pm, and Lz = 30 pm. Therefore, the number of nodes in each dimension is N1 = 1, N2 = 1, and N3 = 2.
The spin quantum number j = 1/2 for electrons, which gives us the total number of states as:
N = 2 × (1/2 + 1) × 1 × 1 × 2 = 4
The maximum number of electrons that can be added is:
N = 4 × (20 pm / 5.29 × 10⁻¹¹ m)³ × (9.11 × 10⁻³¹ kg) / (2 × 1.05 × 10⁻³⁴ J s)² × (6.626 × 10⁻³⁴ J s / 2π)² = 1.79 × 10⁸ or 179 million electrons.
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