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Scilla [17]
3 years ago
11

A ladder 10 ft long rests against a vertical wall. If the bottom of the ladder slides away from the wall at a rate of 1.0 ft/s,

how fast is the angle between the ladder and the ground changing when the bottom of the ladder is 6 ft from the wall? (That is, find the angle's rate of change when the bottom of the ladder is 6 ft from the wall.)

Physics
2 answers:
kirill115 [55]3 years ago
7 0

Answer:

\frac{d\theta}{dt} = -0.125 rad/s

Explanation:

Let at any moment of time the foot of the ladder is at distance "x" from the wall and if the length of the ladder is L = 10 ft

so we have

\frac{x}{L} = cos\theta

now we have

x = L cos\theta

now differentiate the above equation with time

\frac{dx}{dt} = -L sin\theta\frac{d\theta}{dt}

so we have

\frac{d\theta}{dt} = \frac{-v_x}{L sin\theta}

\frac{d\theta}{dt} = \frac{-1 ft/s}{10 sin\theta}

as we know that

cos\theta = \frac{6}{10} = 0.6

\theta = 53 degree

\frac{d\theta}{dt} = \frac{-1 ft/s}{10 sin53}

\frac{d\theta}{dt} = \frac{-1 ft/s}{10 sin\theta}

\frac{d\theta}{dt} = -0.125 rad/s

natka813 [3]3 years ago
4 0

Answer:

The angle's rate of change is: -0.125 (degree/feet).

Explanation:

In this case of problem we need to find the angle's rate (α) of change when x=6 ft. First we need to relate (α) with x and y and the expression that do it is: \alpha =Arctan(\frac{y}{x}) where (α) is the angle between the ladder and the ground, x is the horizontal distance and y the vertical distance, now we need to have the variable y at function of x, so we can do it using the Pythagorean theorem and gets:y^{2} +x^{2} =10^{2} solving for y(x) we get:y(x)=\sqrt{100-x^{2}}. Replacing all we have got in the first equation: \alpha =Arctan(\frac{\sqrt{100-x^{2} } }{x}). Finally we derivate this equation at function of variable x and gets this result:\frac{d\alpha }{dx} =\frac{-1}{\sqrt{100-x^{2} } } evaluating at x=6 ft we get: -0.125(degree/feet). The negative signal means that the angle is decreasing.

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Explanation:

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A capacitor is formed from two concentric spherical conducting shells separated by vacuum. The inner sphere has radius 11.0 cm ,
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Part A)
First of all, let's convert the radii of the inner and the outer sphere:
r_A = 11.0 cm = 0.110 m
r_B = 16.5 cm=0.165 m
The capacitance of a spherical capacitor which consist of two shells with radius rA and rB is
C=4 \pi \epsilon _0  \frac{r_A r_B}{r_B- r_A}=4\pi(8.85 \cdot 10^{-12}C^2m^{-2}N^{-1}) \frac{(0.110m)(0.165m)}{0.165m-0.110m}=
=3.67\cdot 10^{-11}F

Then, from the usual relationship between capacitance and voltage, we can find the charge Q on each sphere of the capacitor:
Q=CV=(3.67\cdot 10^{-11}F)(100 V)=3.67\cdot 10^{-9}C

Now, we can find the electric field at any point r located between the two spheres, by using Gauss theorem:
E\cdot (4 \pi r^2) =  \frac{Q}{\epsilon _0}
from which
E(r) =  \frac{Q}{4 \pi \epsilon_0 r^2}
In part A of the problem, we want to find the electric field at r=11.1 cm=0.111 m. Substituting this number into the previous formula, we get
E(0.111m)=2680 N/C

And so, the energy density at r=0.111 m is
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Part B) The solution of this part is the same as part A), since we already know the charge of the capacitor: Q=3.67 \cdot 10^{-9}C. We just need to calculate the electric field E at a different value of r: r=16.4 cm=0.164 m, so
E(0.164 m)= \frac{Q}{4 \pi \epsilon_0 r^2}=1228 N/C

And therefore, the energy density at this distance from the center is
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