Answer:
ωB = 300 rad/s
ωC = 600 rad/s
Explanation:
The linear velocity of the belt is the same at pulley A as it is at pulley D.
vA = vD
ωA rA = ωD rD
ωD = (rA / rD) ωA
Pulley B has the same angular velocity as pulley D.
ωB = ωD
The linear velocity of the belt is the same at pulley B as it is at pulley C.
vB = vC
ωB rB = ωC rC
ωC = (rB / rC) ωB
Given:
ω₀A = 40 rad/s
αA = 20 rad/s²
t = 3 s
Find: ωA
ω = αt + ω₀
ωA = (20 rad/s²) (3 s) + 40 rad/s
ωA = 100 rad/s
ωD = (rA / rD) ωA = (75 mm / 25 mm) (100 rad/s) = 300 rad/s
ωB = ωD = 300 rad/s
ωC = (rB / rC) ωB = (100 mm / 50 mm) (300 rad/s) = 600 rad/s
Answer:
The wavelength of that tone in air at standard condition is 0.96 m.
Explanation:
Given that, a trombone can produce pitches ranging from 85 Hz to 660 Hz approximately. We need to find the wavelength of that tone in air when the trombone is producing a 357 Hz tone.
We know that the speed of sound in air is approximately 343 m/s. Speed of a wave is given by :
So, the wavelength of that tone in air at standard condition is 0.96 m. Hence, this is the required solution.
Answer:
Volume of gasoline spills out is 0.943 L.
Explanation:
Volumetric expansion of both gasoline and steel tank is :
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We know expansion due to temperature change is :
For gasoline:
Similarly for Steel tank:
.
Now, volume of gasoline spills out is equal to difference between expansion in volume.
Answer:
a)
b)
Explanation:
Given:
(a)
Using the equation of motion :
..............................(1)
where:
v=final velocity of the body
u=initial velocity of the body
here, since the body starts from rest state:
putting the values in eq. (1)
Now, the momentum of the body just before the jump onto the tyre will be:
Now using the conservation on momentum, the momentum just before climbing on the tyre will be equal to the momentum just after climbing on it.
(b)
Now, from the case of a swinging pendulum we know that the kinetic energy which is maximum at the vertical position of the pendulum gets completely converted into the potential energy at the maximum height.
So,
above the normal hanging position.
Answer:
UG (x) = m*g*x*sin(Q)
Vx,f (x)= sqrt (2*g*x*sin(Q))
Explanation:
Given:
- The length of the friction less surface L
- The angle Q is made with horizontal
- UG ( x = L ) = 0
- UK ( x = 0) = 0
Find:
derive an expression for the potential energy of the block-Earth system as a function of x.
determine the speed of the block at the bottom of the incline.
Solution:
- We know that the gravitational potential of an object relative to datum is given by:
UG = m*g*y
Where,
m is the mass of the object
g is the gravitational acceleration constant
y is the vertical distance from datum to the current position.
- We will consider a right angle triangle with hypotenuse x and angle Q with the base and y as the height. The relation between each variable can be given according to Pythagoras theorem as follows:
y = x*sin(Q)
- Substitute the above relationship in the expression for UG as follows:
UG = m*g*x*sin(Q)
- To formulate an expression of velocity at the bottom we can use an energy balance or law of conservation of energy on the block:
UG = UK
- Where UK is kinetic energy given by:
UK = 0.5*m*Vx,f^2
Where Vx,f is the final velocity of the object @ x:
m*g*x*sin(Q) = 0.5*m*Vx,f^2
-Simplify and solve for Vx,f:
Vx,f^2 = 2*g*x*sin(Q)
Hence, Velocity is given by:
Vx,f = sqrt (2*g*x*sin(Q))
Answer:
Explanation:
Area of crossection, A = 7.80 cm²
Initial magnetic field, B = 0.5 T
Final magnetic field, B' = 3.3 T
Time, t = 1 s
resistance of the coil, R = 1.2 ohm
The induced emf is given by
where, Ф is the rate of change of magnetic flux.
e = 7.80 x 10^-4 x (3.3 - 0.5) / 1
e = 2.184 mV
i = e/R
i = 2.184/1.2
i = 1.82 mA
What is the normal force exerted by the surface on the bottom block? (Use the following as necessary: m and g as necessary.)
(a) The normal force exerted by the surface on the bottom block is N1 = 2mg.
Given that,
Based on the above information, we can say that the N1 is 2mg.
Learn more: brainly.com/question/17429689
Answer:
N = 2mg
Explanation:
Assuming the surface is horizontal
The surface must provide enough normal force to prevent the masses from accelerating in the vertical direction.