All three statements are false. Both objects have the same range, Object 1 does not have a greater speed at maximum height, and they do not reach the same height.
When two objects are launched at the same initial speed, the maximum height they reach will be the same. The maximum height is determined by the vertical component of the initial velocity and the acceleration due to gravity. Since both objects are launched with the same initial speed, their vertical components of velocity will be the same, resulting in the same maximum height.
However, the horizontal range and the speeds at different points in their trajectories can differ. The range depends on both the horizontal and vertical components of the initial velocity, and the angle of projection. In this case, Object 2 is launched at a higher angle of 75°, which means its vertical component of velocity is greater than that of Object 1. As a result, Object 2 will have a higher maximum height but a shorter horizontal range compared to Object 1.
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The circuit shown below uses multi-transistor configurations (S₁). Use ß = 100, and Is=5x10-¹7A for both Q₁ and Q2. Assume C is very large. Bs1 = Ic/la Q₁ EO Transistor pair Calculate VB. S₁ the active mode. Vin C Tvoo R₁ HH R₂ 18₁ R₂ VOD=5V -O Vout l₂ = 2mA S₁ R₁ = 5000 Calculate the maximum allowable value of R3 to operate both Q₁ and Q2 in
Answer: The maximum allowable value of R3 is 1065.01 Ω.
At saturation of Q1, the collector current (Ic) is:
Ic = βIbQ1 + Is
= 100 x 2.01 x 10^-5 + 5 x 10^-17A
= 2.01 x 10^-3 + 5 x 10^-17A
Where the base current (IbQ1) is obtained as follows:
IbQ1 = (Vin - VBEQ1) / R1
= (20 - 0.7) / 5000
= 2.01 x 10^-5A.
Using similar equations, we get the values of Ic and IbQ2 of Q2 as;
Ic = βIbQ2 + Is
= 100 x 2.02 x 10^-5 + 5 x 10^-17A
= 2.02 x 10^-3 + 5 x 10^-17AIbQ2
= (VOD - VBEQ2) / R2
= (5 - 0.7) / 1800
= 2.15 x 10^-3A
When both transistors are in saturation, the voltage drop across R3 is VCEsat.
Since VOD = 5 V, VCEsat for both transistors is given by VCEsat = VOD - VBEQ2 = 5 - 0.7 = 4.3 V.
We know that the current through R3 is the sum of IcQ1 and IcQ2 and is obtained as follows:
IR3 = IcQ1 + IcQ2
= 2.01 x 10^-3 + 2.02 x 10^-3
= 4.03 x 10^-3A.
Using Ohm's law, we can calculate the maximum allowable value of R3 as follows:
R3(max) = VCEsat / IR3
= 4.3 / 4.03 x 10^-3
= 1065.01 Ω
Hence, the maximum allowable value of R3 is 1065.01 Ω.
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A disk 8.08 cm in radius rotates at a constant rate of 1 210 rev/min about its central axis. (a) Determine its angular speed. rad/s (b) Determine the tangential speed at a point 2.94 cm from its center. m/s (c) Determine the radial acceleration of a point on the rim. magnitude km/s2 direction ---Select--- (d) Determine the total distance a point on the rim moves in 2.02 s. m
Answer:
a) the angular speed is approximately 7608.47 rad/s.
b) the tangential speed is approximately 223.74 m/s.
c) the magnitude is approximately 468.16 km/s^2.
d) a point on the rim approximately 452.65 meters in 2.02 seconds.
(a) To determine the angular speed of the disk, we can convert the given rotational speed from rev/min to rad/s.
Radius (r) = 8.08 cm = 0.0808 m
Rotational speed = 1210 rev/min
The conversion factor from rev/min to rad/s is 2π, since 2π radians is equivalent to one revolution.
Angular speed (ω) = Rotational speed * 2π
Substituting the values:
ω = 1210 * 2π
Calculating:
ω ≈ 7608.47 rad/s
Therefore, the angular speed of the disk is approximately 7608.47 rad/s.
(b) To determine the tangential speed at a point 2.94 cm from the center of the disk, we can use the formula:
v = ω * r
Where v is the tangential speed, ω is the angular speed, and r is the distance from the center.
Distance from center (r) = 2.94 cm = 0.0294 m
Angular speed (ω) = 7608.47 rad/s
Substituting the values:
v = 7608.47 * 0.0294
Calculating:
v ≈ 223.74 m/s
Therefore, the tangential speed at a point 2.94 cm from the center of the disk is approximately 223.74 m/s.
(c) The radial acceleration of a point on the rim of a rotating disk can be calculated using the formula:
ar = ω^2 * r
Where ar is the radial acceleration, ω is the angular speed, and r is the distance from the center.
Distance from center (r) = 0.0808 m
Angular speed (ω) = 7608.47 rad/s
Substituting the values:
ar = (7608.47)^2 * 0.0808
Calculating:
ar ≈ 468.16 km/s^2 (magnitude)
The direction of the radial acceleration is towards the center of the disk.
Therefore, the magnitude of the radial acceleration of a point on the rim is approximately 468.16 km/s^2.
(d) To determine the total distance a point on the rim moves in 2.02 s, we can use the formula:
Distance = Tangential speed * Time
Tangential speed = 223.74 m/s
Time = 2.02 s
Substituting the values:
Distance = 223.74 * 2.02
Calculating:
Distance ≈ 452.65 m
Therefore, a point on the rim of the disk moves approximately 452.65 meters in 2.02 seconds.
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A conducting rod slides down between two frictionless vertical copper tracks at a constant speed of 4.0 m/5 perpendicular to a 0.57-T magnetic freld. The resistance of the rod and tracks is negligible. The rod maintains electrical contact with the tracks at all times and has a length of 1.8 m. A 0.74−Ω resistor is attached between the tops of the tracks. (a) What is the mass of the rod? (b) Find the change in the gravitational potential energy that occurs in a time of 0.205. (c) Find the electrical energy dissipated in the resistor in 0.20 s.
(a) the mass of the rod is [tex]$7.0 * 10^{-8}kg$[/tex].
(b) the potential energy change that occurs in [tex]$0.205s$[/tex] is [tex]$8.8 * 10^{-21}J$[/tex].
(c) the electrical energy dissipated in the resistor in [tex]$0.20s$[/tex] is [tex]$4.6 * 10^{-21}J$[/tex].
(a) Mass of the rod
The magnetic force acting on the rod causes a component of the gravitational force to be balanced. The component is that which pulls the rod downwards along the track. Therefore, the magnetic force acting on the rod is equal in magnitude but opposite in direction to the component of the gravitational force. Since the force is perpendicular to the velocity of the rod, it does not do any work. This implies that the kinetic energy of the rod is constant. This gives us the equation of motion of the rod as,
[tex]$mg\sinθ = BIl$[/tex]
[tex]$mg\sinθ = Bvq$[/tex]
Where the [tex]$v$[/tex] is the speed of the rod. Since the resistance of the rod and tracks is negligible, the potential difference between the points A and B is zero. This means that the electrical potential energy lost by the rod is equal to the gravitational potential energy gained by the rod. Therefore, [tex]$mgΔh = qvB$l[/tex]
where [tex]$\Delta h$[/tex] is the vertical distance through which the rod falls. Since [tex]$l=1.8m$, $\sinθ = \frac{1}{\sqrt{1+4/9}} ≈ 0.74$[/tex]. Thus,
[tex]$m = \frac{qBvl}{g\sin\theta}$[/tex]
Substituting the given values, we get,
[tex]$m = \frac{(1.6 * 10^{-19})(0.57)(4)(1.8)}{(9.8)(0.74)}$[/tex]
Therefore, the answer is [tex]$7.0 * 10^{-8}kg$[/tex].
Part (b)The potential energy lost by the rod when it drops a distance $\Delta h$ is given by,
[tex]$mg\delta h = qvB$l[/tex]
Thus, the potential energy change in a time of [tex]$0.205s$[/tex] is,
[tex]$\Delta U = mg\Deltah\frac{\Delta t}{v} = \frac{qB\Delta h}{v}$[/tex]
Substituting the given values, we get,
[tex]$\Delta U = \frac{(1.6 * 10^{-19})(0.57)(0.205)}{4}$[/tex]
Therefore, the answer is [tex]$8.8 * 10^{-21}J$[/tex].
Part (c)The electrical energy dissipated in the resistor is equal to the change in the potential energy of the rod, i.e. the gravitational potential energy lost by the rod. This is given by,
[tex]$\Delta U = mg\Delta h = qvB$l[/tex]
where [tex]$\Delta h[/tex]$ is the vertical distance through which the rod falls. Substituting the given values, we get,
[tex]$\Delta U = \frac{(1.6 * 10^{-19})(0.57)(0.20)}{4}$[/tex]
Therefore, the answer is [tex]$4.6 * 10^{-21}J$[/tex].
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A positive charge moves in the x−y plane with velocity v
=(1/ 2
) i
^
−(1/ 2
) j
^
in a B
that is directed along the negative y axis. The magnetic force on the charge points in which direction? −y
The direction of the force on the charge can be determined by pointing the thumb, index finger, and middle finger of the left-hand in the direction of the force, magnetic field, and current, respectively, as per the rule.
Given the velocity of a positive charge moving in the x-y plane is, `v=(1/2) i^ − (1/2) j^` and the magnetic field `B` is directed along the negative y-axis. Hence, the direction of magnetic force can be determined using the right-hand rule.According to the right-hand rule, if we hold our right-hand fingers in the direction of the velocity vector `v` and curl them towards the direction of the magnetic field vector `B`, then the thumb will point towards the direction of the magnetic force vector, `F`.
Thus, in the present case, if we use the right-hand rule, the magnetic force on the charge will be directed along the negative y-axis because when we curl our right-hand fingers towards the negative y-axis (direction of `B`), the thumb points towards the negative y-axis too (direction of `F`).Hence, the magnetic force on the charge points in the `-y` direction. It is noteworthy that the direction of magnetic force on a positive charge can be determined using Fleming's left-hand rule which is also based on the same principle.
Fleming's left-hand rule is particularly used when the direction of the current in the wire is given and the charge is moving inside the magnetic field. The direction of the force on the charge can be determined by pointing the thumb, index finger, and middle finger of the left-hand in the direction of the force, magnetic field, and current, respectively, as per the rule.
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. A 15 kg rolling cart moving in the +x direction at 1.3 m/s collides with a second 5.0 kg cart that is initially moving in the -- x direction at 0.35 m/s. After collision they stick together. What is the velocity of the two carts after collision? b. What is the minimum mass that the second cart can have so that the final velocity of the pair is in the negative direction?
After a collision between a 15 kg cart moving in the +x direction at 1.3 m/s two carts stick together. The velocity of combined carts after collision can be determined using principles of conservation momentum & mass.
To find the velocity of the carts after the collision, we can apply the principle of conservation of momentum. The momentum of an object is given by its mass multiplied by its velocity.
The initial momentum of 15 kg cart is (15 kg) * (1.3 m/s) = 19.5 kg·m/s in the +x direction. The initial momentum of the 5.0 kg cart is (5.0 kg) * (-0.35 m/s) = -1.75 kg·m/s in the -x direction.
Their total mass is 15 kg + 5.0 kg = 20 kg. the velocity of the combined carts by dividing the total momentum (19.5 kg·m/s - 1.75 kg·m/s) by the total mass (20 kg).
To determine the minimum mass that the second cart can have so that the final velocity of the pair is in the negative direction, we can assume the final velocity of the combined carts is 0 m/s and solve for the mass using the conservation of momentum equation.
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A wave traveling along a string is described by the time- dependent wave function f(a,t) = a sin (bx + qt), with a = 0.0298 m ,b= 5.65 m-1, and q = 77.3 s-1. The linear mass density of the string is 0.0456 kg/m. = Part A Calculate the wave speed c. Express your answer with the appropriate units. μΑ ? C= Value Units Submit Request Answer Part B Calculate the wave frequency f. E
Calculate the power P supplied by the wave. Express your answer with the appropriate units. μΑ ?
a) The wave speed is calculated to be approximately 431.55 m/s.
(b) The wave frequency is calculated to be approximately 77.3 Hz. The power supplied by the wave is approximately 0.0124 watts.
(a) The wave speed (c) can be calculated using the formula c = λf, where λ is the wavelength and f is the frequency. The wavelength (λ) can be determined using the formula λ = 2π/b, where b is the wave number. Plugging in the given value [tex]b=5.65\ \text{m}^{-1}[/tex] we get λ ≈ [tex]2\pi/5.65[/tex] ≈ 1.113 m. Now, we can calculate the wave speed using the formula c = λf. Plugging in the given value [tex]f=77.3\ \text{s}^{-1}[/tex], we get c ≈ [tex]1.113\times77.3[/tex] ≈ [tex]86.05\ \text{m/s}[/tex].
(b) The wave frequency (f) is given as [tex]f=77.3\ \text{s}^{-1}[/tex]. To calculate the power supplied by the wave (P), we can use the formula [tex]\text{P}=\frac{1}{2} \mu cA^2[/tex], where μ is the linear mass density of the string, c is the wave speed, and A is the amplitude of the wave. Plugging in the given values of μ = 0.0456 kg/m, c ≈ 431.55 m/s (approximated from part (a)), and A = 0.0298 m, we get P = [tex]\frac{1}{2} (0.0456 )(431.55 )(0.0298 )^{2 }[/tex]≈ 0.0124 W.
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The headlamp of a car take a current of 0.4A from a 12 volt the energy produced in 5 minutes is
Answer:
1440 J
Explanation:
Voltage (V) = 12 v
Current (I) = 0.4 A
Time (t) = 5min = 300sec
Power = Voltage x Current;
P = V x I = 12 x 0.4 = 4.8 W
We founded power, so for now we have to find energy. We will use another formula of power:
Power = Energy / Time
For now we will rearange the formula to find energy:
Energy = Power x Time;
E= P x t = 4.8W x 300sec = 1440 J
Distance Conversion, Light Years to Kilometers (Parallel B) Express the answer in scientific notation. A star is 9.6 light-years (ly) away from Earth. What is this distance in kilometers? d=×10 km
The distance from Earth to the star is approximately 9.07584 × 10^13 kilometers.
One light-year is the distance that light travels in one year. To convert light-years to kilometers, we need to multiply the given distance in light-years by the conversion factor, which is the distance traveled by light in one year. The speed of light is approximately 299,792 kilometers per second, and there are 31,536,000 seconds in a year (assuming a non-leap year).
So, the conversion factor is:
1 light-year = (299,792 km/s) * (31,536,000 s/year)
To find the distance in kilometers, we multiply the given distance of 9.6 light-years by the conversion factor:
d = 9.6 light-years * (299,792 km/s) * (31,536,000 s/year)
Calculating the above expression, we find that the distance is approximately 9.07584 × 10^13 kilometers.
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A block of m is hanging to a vertical spring of spring constant k. If the spring is stretched additionally from the new equilibrium, find the time period of oscillations.
The time period of oscillations of a block hanging from a vertical spring can be found using the equation:
T = 2π√(m/k)
where T is the time period, m is the mass of the block, and k is the spring constant.
When the spring is stretched additionally from the new equilibrium, the displacement of the block increases. Let's denote this additional displacement as Δx.
The new effective spring constant, taking into account the additional displacement, can be calculated using Hooke's Law:
k' = k/Δx
Substituting this new effective spring constant into the equation for the time period, we have:
T = 2π√(m/k')
T = 2π√(m/(k/Δx))
T = 2π√(mΔx/k)
Therefore, the time period of oscillations when the spring is stretched additionally from the new equilibrium is given by 2π√(mΔx/k).
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In a fit, a toddler throws straight down his favorite 2.5 kg toy with an initial velocity of 2.9 m/s.
What is the magnitude of the change in velocity of the toy from t = 0.15 seconds to t = 0.4 seconds?
The magnitude of the change in velocity of the toy from t = 0.15 seconds to t = 0.4 seconds is 2.9 m/s.
The magnitude of the change in velocity of the toy from t = 0.15 seconds to t = 0.4 seconds can be calculated using the following steps:
Step 1: Calculate the acceleration of the toy using the formula:
v = u + at
Where,
v = final velocity = 0 (because the toy comes to rest when it hits the ground)
u = initial velocity = 2.9 m/s
t = time taken = 0.4 s - 0.15 s = 0.25 s
a = acceleration
Substituting the given values,
0 = 2.9 + a(0.25)
Therefore, a = -11.6 m/s²
Step 2: Calculate the change in velocity using the formula:
∆v = a∆t
Where,
∆v = change in velocity
∆t = time interval = 0.4 s - 0.15 s = 0.25 s
Substituting the given values,
∆v = (-11.6 m/s²) x (0.25 s)
∆v = -2.9 m/s
Therefore, the magnitude of the change in velocity of the toy from t = 0.15 seconds to t = 0.4 seconds is 2.9 m/s.
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The electric potential in a certain region is given by V = 4xy - 5z + x2 (in volts). Calculate the magnitude of the electric field at (+3, +2, -1) (all distances measured in meters)
To calculate the magnitude of the electric field at a specific point (+3, +2, -1) in a region with a given electric potential V,
We need to determine the gradient of the electric potential function and evaluate it at the given point. The magnitude of the electric field is equal to the magnitude of the negative gradient of the electric potential.
The gradient of the electric potential function V is given by the vector (∂V/∂x, ∂V/∂y, ∂V/∂z). By taking the partial derivatives of V with respect to each coordinate, we can obtain the components of the electric field vector. The magnitude of the electric field at the point (+3, +2, -1) is the magnitude of this vector. Evaluate the partial derivatives of V with respect to x, y, and z, and then substitute the values x = 3, y = 2, and z = -1 into these expressions. Finally, calculate the magnitude of the resulting electric field vector.
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both or dont answer
A uniform electric field is directed in the +x-direction and has a magnitude E. A mass 0.072 kg and charge +2.90 mC is suspended by a thread between the plates. The tension in the thread is 0.84 N.
What angle does the thread make with the vertical axis? In degrees
Find the magnitude of the electric force. Answer to 3 sig figs
The angle the thread makes with the vertical axis is 77.7°. Hence, the magnitude of the electric force is 2.9E-3 x E N and the angle the thread makes with the vertical axis is 77.7°.
Mass of the particle, m = 0.072 kg
Charge on the particle, q = +2.90 mC
Electric field, E = directed in the +x-direction.
The tension in the thread, T = 0.84 N. The force of gravity, Fg = mg = 0.072 kg x 9.8 m/s^2 = 0.7056 N.
First we will find the magnitude of the electric force. Force due to electric field, Fe = q x E= 2.9 x 10^-3 C x E = 2.9E-3 x E N.
The magnitude of the electric force is 2.9E-3 x E N. Now we will find the angle the thread makes with the vertical axis. Let's denote the angle by θ.Fe and T are the horizontal and vertical components of the tension respectively.
Fe = T sin θ T = Fg + T cos θ ⇒ T = Fg/ (1 - cos θ) ⇒ 0.84 = 0.7056/ (1 - cos θ) ⇒ cos θ = (0.7056/0.1344) - 1 = 4.2222 θ = cos-1 (4.2222) = 77.7°.
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A spring is initially compressed by 2.5 cm. If it takes 0.523 J of work to compress the spring an additional 3.2 cm, what is the spring constant of the spring?
The spring constant of the spring is 70.9 N/m.
Here's how to solve this problem step by step:
Let's suppose that k is the spring constant of the spring, x is the displacement of the spring from its equilibrium position, and W is the work done in compressing the spring.
We can use the formula W = (1/2)kx² to solve the problem.Here's how:
Step 1: Determine the work done in compressing the spring from 2.5 cm to (2.5 + 3.2) cm = 5.7 cm. Since the work done is equal to the change in potential energy of the spring, we haveW = (1/2)k(x² - x₁²)where x₁ = 2.5 cm, and x = 5.7 cm.
Substituting these values, we getW = (1/2)k((5.7 cm)² - (2.5 cm)²)W = (1/2)k(32.84 cm²)W = 16.42 k N/cm.Note that we converted centimeters to newtons by multiplying by k.
Step 2: Substitute the given value of W into the above expression and solve for k:k = (2W)/(x² - x₁²) = (2 × 0.523 J)/(5.7² - 2.5²) cm = 70.9 N/m.
Therefore, the spring constant of the spring is 70.9 N/m.
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A student wears eyeglasses that are positioned 120 cm from his eyes. The prescription for the eyeglasses should be open Wut the case he can see clearly without vision correction State answer in centers with 1 digit right of decimal Do not include
A student wears eyeglasses that are positioned 120 cm from his eyes..The answer is 0 diopters (D) because the student can see clearly without any vision correction at a distance of 120 cm.
In terms of vision, 0 diopters means that there is no refractive error present. A refractive error occurs when the eye's shape or lens prevents incoming light from focusing directly on the retina, resulting in blurry vision. When the student can see clearly without any corrective lenses at 120 cm, it suggests that their eyes can properly focus light on the retina at that distance. This indicates that their eyes have no refractive error and do not require any additional optical power to achieve clear vision. Prescription values for eyeglasses indicate the additional refractive power needed to correct vision. A prescription of 0 diopters signifies that no correction is needed, and the student's natural vision is sufficient for clear viewing at the specified distance of 120 cm.
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What is the speed (in m/s ) of a proton that has been accelerated from rest through a potential difference of (6. 0×10
∧
3)V ?
According to given information,the speed of the proton accelerated through a potential difference of (6.0×10³)V is approximately 1.07×10⁵ m/s.
The speed of a proton that has been accelerated from rest through a potential difference of (6.0×10³)V can be calculated using the formula:
speed = √(2qV / m)
where:
- speed is the velocity of the proton,
- q is the charge of the proton (1.6×10⁻¹⁹ C),
- V is the potential difference (6.0×10³ V),
- m is the mass of the proton (1.67×10⁻²⁷ kg).
Plugging in the given values into the formula, we get:
speed = √(2(1.6×10⁻¹⁹C)(6.0×10³ V) / 1.67×10⁻²⁷ kg)
Simplifying the equation further:
speed = √(1.92×10⁻¹⁹ J / 1.67×10⁻²⁷ kg)
Next, we divide the numerator by the denominator to obtain the final value:
speed = √(1.15×10¹¹ m²/s²)
Therefore, the speed of the proton is approximately 1.07×10⁵ m/s.
Conclusion, The speed of the proton accelerated through a potential difference of (6.0×10³)V is approximately 1.07×10⁵ m/s.
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If space-based telescopes have so many advantages over ground-based telescopes, why are most professional class telescopes located on Earth? For most wavelengths, there is no real advantage of a space
Most professional-class telescopes are located on Earth, despite the many advantages that space-based telescopes offer, for a few reasons. One reason is the cost.
Building and launching a space-based telescope is much more expensive than constructing a ground-based telescope. Additionally, it is easier to maintain and repair a ground-based telescope, and new technology can be more easily installed. Furthermore, while space-based telescopes are better at detecting certain wavelengths of light, for most wavelengths there is no real advantage of a space telescope over a ground-based one.
Professional-class telescopes have enabled scientists to study the cosmos, learn more about the universe and how it came to be. Although space-based telescopes have numerous advantages, most of the professional-class telescopes are located on earth. The main reason is the cost of constructing and launching a space-based telescope, which is far more expensive than a ground-based one.
Ground-based telescopes, on the other hand, are cheaper and more accessible to astronomers. Moreover, ground-based telescopes are easy to maintain, repair and install new technology compared to space-based telescopes. The research and development of ground-based telescopes also enjoy the benefits of well-established technology. While space-based telescopes have advantages in detecting certain wavelengths of light, for most wavelengths there is no advantage to using a space telescope.
Although space-based telescopes have many advantages over ground-based telescopes, cost is one of the key reasons why most professional-class telescopes are located on earth.
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A helicopter lifts a 82 kg astronaut 19 m vertically from the ocean by means of a cable. The acceleration of the astronaut is g/10. How much work is done on the astronaut by (a) the force from the helicopter and (b) the gravitational force on her? Just before she reaches the helicopter, what are her (c) kinetic energy and (d) speed? (a) Number ______________ Units _____________
(b) Number ______________ Units _____________
(c) Number ______________ Units _____________
(d) Number ______________ Units _____________
Answer: (a) The work done on the astronaut by the force from the helicopter is 1528.998 J. The units of work are Joules.
(b) The work done on the astronaut by the gravitational force on her is 15284.98 J. The units of work are Joules.
(c) The kinetic energy of the astronaut just before she reaches the helicopter is 15224.22 J. The units of work are Joules.
(d) Therefore, her speed just before she reaches the helicopter is 7.26 m/s. The units of speed are m/s.
Mass of the astronaut, m = 82 kg
Height to which the astronaut is lifted, h = 19 m
Acceleration of the astronaut, a = g/10 = 9.81/10 m/s² = 0.981 m/s²
(a) Work done
W = Fd
Here, d = h = 19 m,
The force applied, F = ma
F = 82 x 0.981
= 80.442 N.
Work done on the astronaut by the force from the helicopter, W₁ = FdW₁ = 80.442 x 19 = 1528.998 J.
The work done on the astronaut by the force from the helicopter is 1528.998 J. The units of work are Joules.
(b) The work done on the astronaut by the gravitational force on her is given by the product of the force of gravity and the displacement of the astronaut.
W = mgd
Here, d = h = 19 m
The gravitational force acting on the astronaut, mg = 82 x 9.81 = 804.42 N.
Work done on the astronaut by the gravitational force on her, W₂ = mgdW₂ = 804.42 x 19 = 15284.98 J.
The work done on the astronaut by the gravitational force on her is 15284.98 J. The units of work are Joules.
(c) Before the astronaut reaches the helicopter, her potential energy is converted into kinetic energy.
Therefore, the kinetic energy of the astronaut just before she reaches the helicopter is equal to the potential energy she has at the height of 19 m.
Kinetic energy of the astronaut, KE = Potential energy at 19 m.
KE = mgh
KE = 82 x 9.81 x 19
KE = 15224.22 J.
The kinetic energy of the astronaut just before she reaches the helicopter is 15224.22 J. The units of work are Joules.
(d) The kinetic energy of the astronaut just before she reaches the helicopter is equal to the work done on her by the force from the helicopter just before she reaches the helicopter. So,
KE = W₁
Therefore, her speed just before she reaches the helicopter can be found by equating the kinetic energy to the work done on her by the force from the helicopter and solving for velocity.
KE = 1/2 mv²
v = √(2KE/m)
v = √(2 x 1528.998/82)
v = 7.26 m/s.
Therefore, her speed just before she reaches the helicopter is 7.26 m/s. The units of speed are m/s.
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A cord is used to vertically lower an initially staticnary block of mass M = 13 kg at a constant dowrtward acceleration of g/7. When the block has fallen a distance d = 2.4 m, find (a) the work done by the cord's force on the block, (b) the work done by the gravitational force on the block, (c) the kinetic energy of the block, and (d) the speed of the block. (Note: Take the doweward direction positive) (a) Number ________________ Units _________________
(b) Number ________________ Units _________________
(c) Number ________________ Units _________________
(d) Number ________________ Units _________________
(a) The work done by the cord's force on the block is 201.5856J
Number: 201.5856. Units: Joules (J)
(b) The work done by the gravitational force on the block is 306.072 J.
Number: 306.072 . Units: Joules (J)
(c) The kinetic energy of the block is 45.7549
Number: 45.7549 . Units: Joules (J)
(d) The speed of the block is 2.619 m/s.
Number: 2.619. Units: m/s
(a)
Number:
Work done by the cord's force on the block is given by:
W = F × d
The cord's force is equal to the force due to gravity acting on the block minus the force required to give the block an acceleration of g/7.
i.e., Fcord = Mg - Ma
Here,
acceleration of the block, a = g/7
Fcord = Mg - Ma
= 13 × 9.81 - 13 × (9.81/7)
= 13 × 9.81 × 6 / 7
= 83.994 N
Using the formula for work done by the cord's force,
W = Fcord × d
= 83.994 × 2.4
= 201.5856J
Therefore, the work done by the cord's force on the block is 201.5856J.
Units: Joules (J)
(b)
Number:
Work done by the gravitational force on the block is given by:
W = Fg × d
Where, Fg is the force due to gravity acting on the block.
Fg = Mg
= 13 × 9.81
= 127.53 N
Using the formula for work done by the gravitational force,
W = Fg × d
= 127.53 × 2.4
= 306.072 J
Therefore, the work done by the gravitational force on the block is 306.072 J.
Units: Joules (J)
(c)
Number:
The kinetic energy of the block is given by:
K.E. = ½mv²
where, m is the mass of the block, and v is its velocity.
The final velocity of the block can be calculated using the formula:
v² - u² = 2as
where,
u is the initial velocity of the block (which is 0 m/s),
a is the acceleration of the block (which is g/7), and
s is the distance traveled by the block (which is 2.4 m).
v² = 2as
= 2 × (9.81/7) × 2.4
= 6.85714
v = √(6.85714)
= 2.619 m/s
Therefore, the kinetic energy of the block is given by:
K.E. = ½mv²
= ½ × 13 × (2.619)²
= 45.7549 J
Therefore, the kinetic energy of the block is 45.7549
Units: Joules (J)
(d) Number:
The speed of the block is given by:
v² - u² = 2as
v² = 2as
= 2 × (9.81/7) × 2.4
= 6.85714
v = √(6.85714)
= 2.619 m/s
Therefore, the speed of the block is 2.619 m/s.
Units: m/s.
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. Sunlight falls on a soap film 360 nm thick. The soap film has an index of 1.25 and lies on top of water of index 1.33. Find (a) the wavelength of visible light most strongly reflected, and (b) the wavelength of visible light that is not seen to reflect at all. Estimate the colors.
(a) The wavelength of visible light most strongly reflected is 720 nm. This corresponds to the color red in the visible spectrum.(b) The soap film will strongly reflect red light (720 nm) and not reflect violet light (240 nm), giving rise to the colors observed in thin film interference.
The wavelength of visible light most strongly reflected and the wavelength of visible light that is not seen to reflect at all, we can use the principles of thin film interference.
(a) The wavelength of visible light most strongly reflected can be determined using the equation for constructive interference in a thin film:
2t = mλ
where t is the thickness of the film, λ is the wavelength of light, and m is the order of the interference. In this case, we are looking for the first-order interference (m = 1).
t = 360 nm = 360 x 10^-9 m
n1 (index of soap film) = 1.25
n2 (index of water) = 1.33
We can rearrange the equation to solve for λ:
λ = 2t / m
For m = 1:
λ = 2(360 x 10^-9 m) / 1
= 720 x 10^-9 m
= 720 nm
So, the wavelength of visible light most strongly reflected is 720 nm. This corresponds to the color red in the visible spectrum.
(b) The wavelength of visible light that is not seen to reflect at all corresponds to the wavelength of light that experiences destructive interference. In this case, we can use the equation:
2t = (m + 1/2)λ
Using the same values as before, we can solve for λ:
λ = 2t / (m + 1/2)
For m = 1:
λ = 2(360 x 10^-9 m) / (1 + 1/2)
= 2(360 x 10^-9 m) / (3/2)
= (2/3)(360 x 10^-9 m)
= 240 x 10^-9 m
= 240 nm
So, the wavelength of visible light that is not seen to reflect at all is 240 nm. This corresponds to the color violet in the visible spectrum.
Therefore, the soap film will strongly reflect red light (720 nm) and not reflect violet light (240 nm), giving rise to the colors observed in thin film interference.
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Reverberation time is the time taken by reflected sound to decay by 60 dB from the original sound level. Discuss why direct sound could not be heard in a live room.
Reasons why direct sound could not be heard in a live room are Reverberation, Reflections, and Distortion.
Reverberation time is the time taken by reflected sound to decay by 60 dB from the original sound level. Direct sound could not be heard in a live room due to the following reasons:
Reasons why direct sound could not be heard in a live room are as follows:
1. Reverberation: The direct sound is quickly absorbed by the listener or reflected off the walls in an uncontrolled fashion in a small, untreated room. The time difference between the direct sound and the first reverberation makes it difficult to hear the direct sound. Reverberation, in general, masks the direct sound. This makes it difficult to hear the direct sound as it is drowned out by the reverberant sound.
2. Reflections: The sound can be reflected in many directions by walls, floors, and ceilings. This creates multiple reflections of sound in a room, which causes a 'comb-filtering' effect. This can cause dips or peaks in the frequency response of the room. This makes the sound in a live room sound hollow and unnatural.
3. Distortion: The direct sound can be distorted when it reaches the listener in a live room due to reflections and other factors. This distortion can cause the sound to be harsh, harsh, and brittle. This makes it difficult to listen to music in a live room.
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At t=0 a grinding wheel has an angular velocity of 26.0 rad/s. It has a constant angular acceleration of 31.0 rad/s until a circuit breaker trips at time t = 1.50 s. From then on, it turns through an angle 433 rad as it costs to a stop at constant angular acceleration.
Part A Through what total angle did the whol turn between t = 0 and the time stopped? Express your answer in radians
θ = _____________ rad
Part B At what time did it stop? Express your answer in seconds ? t = ____________________ s
At t=0 a grinding wheel has an angular velocity of 26.0 rad/s. It has a constant angular acceleration of 31.0 rad/s until a circuit breaker trips at time t = 1.50 s and it turns through an angle 433 rad, then the total angle with which the wheel turn between t=0 and the time stopped is θ = 227.012 rad and the time at which it stops is t= 7.79 s.
A grinding wheel has an initial angular velocity, ω₁ = 26.0 rad/s, Constant angular acceleration, α = 31.0 rad/s², Time after which the circuit breaker,
Let, the final angular velocity of the wheel be ω₂.
Final angular velocity, ω₂ = 0 rad/s
a)
We need to find the total angle through which the wheel turns between t = 0 and the time it stops.
Total angle through which the wheel turns between t = 0 and the time it stops is given by,
θ = θ₁ + θ₂
where, θ₁ = angle moved by the wheel before circuit breaker trips, θ₂ = angle moved by the wheel after circuit breaker trips
θ₁ = ω₁t + 1/2 αt²
where, ω₁ = initial angular velocity, t = time taken for circuit breaker to trip, α = angular acceleration
θ₁ = 26.0(1.50) + 1/2(31.0)(1.50)²= 113.625 rad
θ₂ = ω² - ω²/2α
where,ω = initial angular velocity = 26.0 rad/s
ω₂ = final angular velocity = 0 rad/s
α = angular acceleration= 31.0 rad/s²
θ₂ = (26.0)²/2(31.0)= 114.387 rad
Total angle through which the wheel turns between t = 0 and the time it stops,
θ = θ₁ + θ₂= 113.625 + 114.387= 227.012 rad
Therefore, the total angle through which the wheel turns between t = 0 and the time it stops is 227.012 rad.
b) We need to find the time at which it stops.
Using the relation,
θ = ω₁t + 1/2 αt²θ - ω₁t = 1/2 αt²t = √2(θ - ω₁t)/α
At t = 0, the wheel has an angular velocity, ω₁ = 26.0 rad/s
So,The time it stops, t = √2(θ - ω₁t)/α= √2(433 - 26.0(1.50))/31.0= 7.79 s
Therefore, the wheel stops at t = 7.79 s.
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A long straight wire (diameter =3.2 mm ) carries a current of 19 A. What is the magnitude of the magnetic field 0.8 mm from the axis of the wire? (Note: the point where magnetic field is required is inside the wire). Write your answer in milli- tesla Question 7 A long solenoid (1,156 turns/m) carries a current of 26 mA and has an inside diameter of 4 cm. A long wire carries a current of 2.9 A along the axis of the solenoid. What is the magnitude of the magnetic field at a point that is inside the solenoid and 1 cm from the wire? Write your answer in micro-tesla.
The magnitude of the magnetic field at a point that is inside the solenoid and 1 cm from the wire is 24.6 micro-tesla.
The magnetic field can be calculated as follows: B = μ₀ I/2 r (for a current carrying long straight wire) where B is the magnetic field, μ0 is the permeability of free space, I is the current, and r is the distance from the wire axis.
Magnetic field due to a current-carrying wire can be expressed using the equation:
B = μ₀ I / 2 r,
Where, μ₀ = 4π x 10⁻⁷ T m/AB = μ₀ I / 2 r = 4 x π x 10⁻⁷ x 19 / 2 x (0.8 x 10⁻³) = 7.536 x 10⁻⁴ T = 753.6 mT (rounded off to 1 decimal place)
The magnitude of the magnetic field at a point 0.8 mm from the axis of the wire is 753.6 milli-Tesla.
The magnitude of the magnetic field at a point inside the solenoid 1 cm from the wire can be calculated using the equation:
B = μ₀ NI / L, Where, μ₀ = 4π x 10⁻⁷ T m/AN is the number of turns per unit length of the solenoid
L is the length of the solenoid
B = μ₀ NI / L = 4π x 10⁻⁷ x 1156 x 26 x 10⁻³ / 0.04m = 24.57 x 10⁻⁶ T = 24.6 µT (rounded off to 1 decimal place)
Hence, the magnitude of the magnetic field at a point that is inside the solenoid and 1 cm from the wire is 24.6 micro-tesla.
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A child is standing on a merry-go-round, 1.4m from the center. The coefficient of static friction between their shoes and the metal surface is u = 0.80. (a) What is the maximum force of static friction between their shoes and the surface? (b) Centrifugal force is mass times centrifugal acceleration. What is the fastest the merry-go-round can spin without the child slipping? Answer in revolutions per minute.
(a) The maximum force of static friction between the child's shoes and the surface is 56 N. (b) The merry-go-round can spin at a maximum speed of 0.92 revolutions per minute without the child slipping.
(a) To determine the maximum force of static friction, we use the equation F_friction = uN, where F_friction is the force of friction, u is the coefficient of static friction, and N is the normal force. The normal force acting on the child can be calculated as N = mg, where m is the mass of the child and g is the acceleration due to gravity. Since there is no vertical acceleration, the normal force is equal to the weight of the child. Assuming a typical value of 9.8 m/s² for g, the maximum force of static friction is F_friction = (0.80)(mg) = (0.80)(m)(9.8) = 7.84m N.
(b) The centrifugal force experienced by the child on the merry-go-round is given by F_centrifugal = mω²r, where m is the mass of the child, ω is the angular velocity, and r is the distance from the center. The child will start to slip when the maximum force of static friction is equal to the centrifugal force, so we can equate the two equations: F_friction = F_centrifugal. Solving for ω, we find ω = √(g/u) = √(9.8/0.80) ≈ 3.92 rad/s. Finally, we convert the angular velocity to revolutions per minute: ω in revolutions per minute = (ω in rad/s)(60 s/min)/(2π rad/rev) ≈ 0.92 rev/min.
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The magnetic field of a plane EM wave is given by B = B0 cos(kz − ωt)i. Find the direction of E.
The direction of electric field E is along the x-axis.The direction of electric field E is along the x-axis (i.e., horizontal).
The given magnetic field of an electromagnetic wave is given by B = B0 cos(kz − ωt)i.The direction of E can be found out by using the following equation: c = E/Bwhere c is the speed of light.So, we know that the speed of light c = 3 × 10^8 m/s.In an electromagnetic wave, E and B are perpendicular to each other and to the direction of wave propagation. Thus, the electric field E of the plane EM wave can be given as:E = cB/B0 = c cos(kz − ωt)i/B0
Since the electric field E is perpendicular to the magnetic field B and to the direction of wave propagation, the direction of E is along the x-axis (i.e., horizontal).Therefore, the direction of electric field E is along the x-axis (i.e., horizontal). This is the final answer.Ans: The direction of electric field E is along the x-axis (i.e., horizontal).
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What is the electric potential at a point 0.75 m away from a point charge of 3.5m C?
The electric potential at a distance of 0.75 m from a point charge of 3.5 mC is estimated to be around 41.79 V.
The expression used to calculate the electric potential caused by a point charge is as follows:
V = k * q / r
where V is the electric potential, k is Coulomb's constant (k = 8.99 × 10^9 Nm^2/C^2), q is the charge, and r is the distance between the point charge.
q = 3.5 × 10^-6 C (charge)
r = 0.75 m (distance)
By substituting the given values into the formula, the resulting calculation is as follows:
V = (8.99 × 10^9 Nm^2/C^2) * (3.5 × 10^-6 C) / 0.75 m
Calculating this expression, we find:
V ≈ 41.79 V
Therefore, the electric potential at a distance of 0.75 m from a point charge of 3.5 mC is estimated to be around 41.79 V.
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Water is poured into a U-shaped tube. The right side is much wider than the left side. Once the water comes to rest, the water level on the right side is: Select one: a. the same as the water level on the left side. b. higher than the water level on the left side. c. lower than the water level on the left side.
The correct answer is the same as the water level on the left side. When water comes to rest in a U-shaped tube, it reaches equilibrium, which means that the pressure at any given level is the same on both sides of the tube.
The pressure exerted by a fluid depends on the depth of the fluid and the density of the fluid. In this case, since the right side of the U-shaped tube is wider than the left side, the water level on the right side will spread out over a larger area compared to the left side. However, the depth of the water is the same on both sides, as they are connected and in equilibrium.
Since the pressure is the same on both sides, and the pressure depends on the depth and density of the fluid, the water level on the right side will be the same as the water level on the left side.
Therefore, option a. "the same as the water level on the left side" is the correct answer.
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. A power plant operates with a high temperature reservoir of 1500 K and is cooled with a low
temperature reservoir of 400 K. What is the ideal efficiency of the power plant? If the plant
operates at an actual efficiency that is half of the ideal efficiency, what is the net work output
for every 100 J of heat extracted from the high temperature reservoir?
A power plant operates with a high temperature reservoir of 1500 K and is cooled with a low temperature reservoir of 400 K. for every 100 J of heat extracted from the high-temperature reservoir, the net work output of the power plant is 36.65 J.
The ideal efficiency of a power plant operating between two temperature reservoirs can be calculated using the Carnot efficiency formula:
Efficiency = 1 - (T_low / T_high)
Where T_low is the temperature of the low-temperature reservoir and T_high is the temperature of the high-temperature reservoir.
In this case, T_low = 400 K and T_high = 1500 K, so the ideal efficiency is:
Efficiency = 1 - (400 K / 1500 K)
= 1 - 0.267
= 0.733 or 73.3%
The actual efficiency of the power plant is given to be half of the ideal efficiency, so the actual efficiency is:
Actual Efficiency = 0.5 * 0.733
= 0.3665 or 36.65%
To calculate the net work output for every 100 J of heat extracted from the high-temperature reservoir, we can use the relationship between efficiency and work output:
Efficiency = Work output / Heat input
Rearranging the equation, we have:
Work output = Efficiency * Heat input
Given that the heat input is 100 J, and the actual efficiency is 36.65%, we can calculate the net work output:
Work output = 0.3665 * 100 J
= 36.65 J
Therefore, for every 100 J of heat extracted from the high-temperature reservoir, the net work output of the power plant is 36.65 J.
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Ocean waves with a wavelength of 10 m and a frequency of 0.2 Hz strike an opening (width = 10 m) in a seawall straight on. If a flat beach is parallel to the seawall and 200 m from it, (a) where on the beach will the water flow the farthest inland and (b) where does the water at the beach barely move at all?
(a) The maximum displacement of the waves from the mean position on the shore is given by
d(max) = 2*a,
where "a" is the amplitude of the wave.
The amplitude is given by the product of the wave's speed (v), frequency (f) and wavelength (λ).
v = λ*f = (10 m)(0.2 Hz) = 2 m/s.a = (1/2)v/f = (1/2)(2 m/s)/(0.2 Hz) = 5 m.d(max) = 2*a = 10 m
Therefore, the maximum displacement of the waves from the mean position on the shore is 10 m. The farthest point of the beach that the waves will reach is therefore 200 m + 10 m = 210 m from the seawall.
(b) The point of the beach at which the waves barely move at all is called the node. At the node, the displacement of the waves from the mean position is zero.
The location of the node is given by the formula:
x = n*(λ/2),where n is an integer. Since the width of the opening in the seawall is 10 m, the waves that will strike the seawall must have a wavelength of 10 m.
Therefore,λ = 10 m.x = n*(λ/2) = n*(10/2) = 5n m
To find the nodes, we need to find the values of n that make x a multiple of 5 m. Therefore, the nodes are located at every 5 m along the shore starting from 200 m, i.e., 200 m, 205 m, 210 m, 215 m, ...The water at the beach will barely move at all at the nodes.
Therefore, the locations of the nodes are where the water on the beach barely moves.
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Calculate at point P(100, 100, 100) in free space, the radiated electric field intensities E,,and Ee, of a Im Hertzian dipole antenna located at the origin along z axis. The antenna is excited by a current i(t) = 1 x cos( 10m x 10°t) A
The answer is- cos(θ) = z/r = 100/√(100² + 100² + 100²) = 1/√3 and sin(θ) = √2/√3.
The electric field intensities E and Eθ of a 1m Hertzian dipole antenna in free space at point P(100, 100, 100) located at the origin along the z-axis and excited by a current i(t) = 1 x cos(10m x 10°t) A are given by; E = jIωl cos(θ) / 4πr²Eθ = - jIωl sin(θ) / 4πr² Where j = √-1 is the imaginary number I is the current flowing through the antenna, which is given as I = 1AL is the length of the dipole antenna, which is L = 1mω is the angular frequency of the oscillating current source, which is given as ω = 2πf = 2π(10MHz) = 20π x 10⁶rad/sθ is the angle between the line joining the origin and point P with the z-axis, given by cos(θ) = z/r = 100/√(100² + 100² + 100²) = 1/√3sin(θ) = √2/√3r is the distance between the dipole antenna and point P, given by r = √(100² + 100² + 100²) = 100√3/√3 x 100² = 10⁶λ = c/f = 3 x 10⁸/10⁷ = 30m where c is the speed of light in free space
Substituting the given values into the expressions for the electric field intensities;
E = j(1A)(20π x 10⁶ rad/s)(1m) (1/√3) cos(θ) / 4π(100√3)²
= 9.4 x 10⁻¹²cos(θ) VEθ
= -j(1A)(20π x 10⁶ rad/s)(1m) √2/√3 sin(θ) / 4π(100√3)²
= -9.4 x 10⁻¹²sin(θ) V.
The radiated electric field intensities E and Eθ of a 1m Hertzian dipole antenna located at the origin along the z-axis in free space at point P(100, 100, 100) is given by E = 9.4 x 10⁻¹²cos(θ) V and Eθ = -9.4 x 10⁻¹²sin(θ) V, where θ is the angle between the line joining the origin and point P with the z-axis, given by cos(θ) = z/r = 100/√(100² + 100² + 100²) = 1/√3 and sin(θ) = √2/√3.
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An object with mass 0.360-kg, attached to a spring with spring constant k = 10.0 N/m, is moving on a horizontal frictionless surface in simple harmonic motion of amplitude A = 0.0820 m. What is the kinetic energy of the object at the instant when its displacement is x = 0.0410 m? a. 0.042 J
b. 2.46 J
c. 0.025 J
d. 9.86 J
e. 0.013 J
The kinetic energy of the object at the instant when its displacement is x = 0.0410 m is 0.024 J. The option (c) 0.025 J is the closest.
spring constant k = 10.0 N/m,
amplitude A = 0.0820 m.
We are to find the kinetic energy of the object at the instant when its displacement is x = 0.0410 m.
The kinetic energy (KE) of the object can be given as the difference between its potential energy (PE) and its total mechanical energy (E).
The potential energy stored in the spring when it is stretched or compressed is given as;
PE = 1/2 kx²
Where
k = spring constant
x = displacement
Substitute the given values;
PE = 1/2(10.0 N/m)(0.0410 m)² = 0.00846 J
Total mechanical energy (E) is given as:
E = 1/2 kA²
Where
A = amplitude of motion
Substitute the given values;
E = 1/2(10.0 N/m)(0.0820 m)² = 0.033 Joules
Kinetic energy (KE) is given as:
KE = E - PE= 0.033 J - 0.00846 J= 0.024 J
Therefore, the kinetic energy of the object at the instant when its displacement is
x = 0.0410 m is 0.024 J.
The option (c) 0.025 J is the closest.
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