Question

In: Physics

By making the following substitutions x becomes θ v becomes ω a becomes α F becomes...

By making the following substitutions

  • x becomes θ
  • v becomes ω
  • a becomes α
  • F becomes τ
  • m becomes I

we get a whole new physics that tells how rotating objects behave. Everything we have done all semester flips over to explain rotational physics

1. The moment of inertia is the quantity that replaces mass in all the old formulas. Not only is the mass of an object important, but also how that mass is distributed.

Find the moment of inertia of a 4 meter long stick with a mass of 23 kg, if it is spun about the center of the stick

ISphere = 2/5 MR2

ICylinder = 1/2 MR2

IRing = MR2

IStick thru center = 1/12 ML2

IStick thru end = 1/3 ML2

2. An ice skater with a moment of inertia of 10 kg m2spinning at 14 rad/s extends her arms, thereby changing her moment of inertia to 26 kg m2. Find the new angular velocity.

Hint: conserve angular momentum!

3. Find the rotational kinetic energy of a spinning (not rolling) bowling ball that has a mass of 10 kg and a radius of 0.17 m moving at 12 m/s.

(Fun fact: How can this problem be done if r isn't given?)

v = rω

ISphere = 2/5 MR2

ICylinder = 1/2 MR2

IRing = MR2

IStick thru center = 1/12 ML2

IStick thru end = 1/3 ML^2


Recall: when rolling, the ball is both moving forward and rotating, so the total KE = the linear KE + the rotational KE

4. Find the total kinetic energy of a rolling bowling ball that has a mass of 8 kg and a radius of 0.19 m moving at 16 m/s.

v = rω

ISphere = 2/5 MR2

ICylinder = 1/2 MR2

IRing = MR2

IStick thru center = 1/12 ML2

IStick thru end = 1/3 ML2


Recall: E1 = E2

5. Find the height a rolling bowling ball that has a mass of 4 kg and a radius of 0.15 m moving at 7 m/s can roll up a hill.

v = rω

ISphere = 2/5 MR2

ICylinder = 1/2 MR2

IRing = MR2

IStick thru center = 1/12 ML2

IStick thru end = 1/3 ML^2


Hint: force at a distance is torque

6. A coke can is suspended by a string from the tab so that it spins with a vertical axis. A 17 N perpendicular force at the edge causes rotation. Find the angular acceleration if the can has a radius of 5 cm and a mass of 929 grams.

Hint: force at a distance is torque

ISphere = 2/5 MR2

ICylinder = 1/2 MR2

IRing = MR2

IStick thru center = 1/12 ML2

IStick thru end = 1/3 ML2

Solutions

Expert Solution

All the problems are standard rotarional dynamics problems and can be solved by using standard formulas in terms of moment of inertia and angular velocity. All the 6 parts are solved step by step. please find the attached solution and provide your valuable feedback.


Related Solutions

Let f(x; θ) = θxθ−1 for 0 < x < 1 and θ ∈ Ω =...
Let f(x; θ) = θxθ−1 for 0 < x < 1 and θ ∈ Ω = {θ : 0 < θ < ∞}. Let X1, . . . , Xn denote a random sample of size n from this distribution. (a) Sketch the pdf of X for (i) θ = 1/2, (ii) θ = 1 and (iii) θ = 2. (b) Show that ˆθ = −n/ ln (Qn i=1 Xi) is the maximum likelihood estimator of θ. (c) Determine the...
is 1. f(x/θ) = 2x/θ^2 complete sufficient statistic 2. f(x/θ) =((logθ) θ^x  ) / (θ -1) complete...
is 1. f(x/θ) = 2x/θ^2 complete sufficient statistic 2. f(x/θ) =((logθ) θ^x  ) / (θ -1) complete sufficient statistic?
Let X1. . . . Xn be i.i.d f(x; θ) = θ(1 − θ)^x x =...
Let X1. . . . Xn be i.i.d f(x; θ) = θ(1 − θ)^x x = 0.. Is there a function of θ for which there exists an unbiased estimator of θ whose variance achieves the CRLB? If so, find it
A force F⃗ of magnitude F making an angle θ with the x axis is applied...
A force F⃗ of magnitude F making an angle θ with the x axis is applied to a particle located along axis of rotation A, at Cartesian coordinates (0,0) in the figure. The vector F⃗ lies in the xy plane, and the four axes of rotation A, B, C, and D all lie perpendicular to the xy plane. (Figure 1) A particle is located at a vector position r⃗ with respect to an axis of rotation (thus r⃗ points from...
Consider a Bernoulli distribution f(x|θ) = θ^x (1 − θ)^(1−x) for x = 0 and x...
Consider a Bernoulli distribution f(x|θ) = θ^x (1 − θ)^(1−x) for x = 0 and x = 1. Let the prior distribution for θ be f(θ) = 6θ(1 − θ) for θ ∈ (0, 1). (a) Find the posterior distribution for θ. (b) Find the Bayes’ estimator for θ.
One obervation is taken from the probability model. f(x;θ)=((θ/2)^|x|)*((1-θ)^(1-|x|)) for x=-1,0,1 and θ ∈ [0,1]. We...
One obervation is taken from the probability model. f(x;θ)=((θ/2)^|x|)*((1-θ)^(1-|x|)) for x=-1,0,1 and θ ∈ [0,1]. We find that the MLE of θ is |x|. Now consider T(X) where T(X)=2 when x=1 and T(X)=0 otherwise. Show that the MLE of θ has a smaller variance than T(X).
For f(x; θ) = θ exp(-xθ) , x>0 1a) Determine the most powerful critical region for...
For f(x; θ) = θ exp(-xθ) , x>0 1a) Determine the most powerful critical region for testing H0 θ=θ0 against H1 θ=θ1 (θ1 > θ0) using a random sample of size n. 1b) Find the uniformly most powerful H0 θ<θ0 against H1 θ>θ1
Let X1, ..., Xn be i.i.d random variables with the density function f(x|θ) = e^(θ−x) ,...
Let X1, ..., Xn be i.i.d random variables with the density function f(x|θ) = e^(θ−x) , θ ≤ x. a. Find the Method of Moment estimate of θ b. The MLE of θ (Hint: Think carefully before taking derivative, do we have to take derivative?)
Let V be a Hilbert space. Let f(x) = ∥x∥ for x ∈ V. Using the...
Let V be a Hilbert space. Let f(x) = ∥x∥ for x ∈ V. Using the definition of Frechet differentiation, show that ∇f(x) = x for all x ̸= 0. Furthermore, show that f(x) is not Frechet differentiable at x = 0.
Suppose X is a Gamma random variable with shape parameter α and scale parameter θ >...
Suppose X is a Gamma random variable with shape parameter α and scale parameter θ > 0, i.e., the pdf is given as, f(x|α, θ) = 1 Γ(α)θ α x α−1 e −x/θ , 0 < x < ∞, (1) where α > 0, θ > 0 and Γ(a) = Z ∞ 0 x a−1 e −x dx. HINT: see section 3.2 of the textbook. (a) What is the support of X? That is, X = ? (b) Show that...
ADVERTISEMENT
ADVERTISEMENT
ADVERTISEMENT