Beginning Numerical Analysis question. Still calculus

lundi 30 septembre 2013

1. The problem statement, all variables and given/known data

Show f(x)=(x−2)sinxln(x+2) has f'(x)=0 somewhere on [-1,3]



3. The attempt at a solution

I tried using Rolle's theorem, but f(-1)≠f(3). Then I tried the mean value theorem, but didn't get 0 either.






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2 boxes stacked, determining forces on each other.

1. The problem statement, all variables and given/known data

The mass of the upper block in the stack is 0.85 kg. The mass of the lower block in the stack is 1.67 kg. The coefficients of friction between the two blocks are: static 0.75, and kinetic 0.61. The child's mother, who likes to encourage his experiments, has oiled a small strip of the horizontal floor so that it is very slick; the coefficient of kinetic friction between the oiled section of floor and the lower block is only 0.12 and the coefficient of static friction is insignificantly different.



Before the pushing starts, here are some questions about the vertical forces acting on the two blocks.



b) What is the vertical component of the contact force on the upper block by the lower block? HINT: You must apply Newton's First Law.



2. Relevant equations



ƩF=0

Since at this point in time the boxes are stationary



3. The attempt at a solution



I know the Fg of upper box is 8.33N, I also know that along with the normal force on the upper block there is also a FB2B1 block 2 being the upper block.

I believe Fg,total= 24.696N, after many other attempts I tried to say Fg,total = NB2, therefore

ƩF = n + FB2B1 - Fg,B2

= 24.696N + FB2B1 - 8.33N = 0

this gives me a negative result for FB2B1 which I know is incorrect.

Here are my free body diagrams, I believe I may be missing something in my FBD which is why I cannot get the answer I am looking for.




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Electron flow in live and neutral wires

Our Physics teacher used to tell us that in an ac circuit the current and hence the flow of electrons is reversed every half cycle as the polarity of the supply changes every half cycle. However I am still puzzled about the following. In the UK, the live is the wire that delivers electrical power from the power grid while the neutral is the return wire.



If this is so does it mean that the flow of electrons is reversed in BOTH live and neutral wires every half cycle?



Why does the direction of the current change if the live remains live while the neutral remains neutral all the time? Is there a good analogy to explain this concept better?




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Do Hilbert Space Isomorphism Map Dense Sets to Dense Sets?

Suppose that H, K are Hilbert spaces, and A : H -> K is a bounded linear operator and an isomorphism.



If X is a dense set in H, then is A(X) a dense set in K?



Any references to texts would also be helpful.






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Will thin steel bars really help prevent granite from breaking?

This construction practice made me curious. As soon as I lifted the 3/16 inch thick by 2 inch wide steel bars (now routed into the plywood subtop under our granite counter overhang) I noticed that these 12 foot long metal pieces bend considerably under their own weight.



It is common practice to place these under the granite, spaced about 1 foot apart perpendicular to the length of the overhang, to reduce or eliminate the need for corbels (those wood support pieces you hit your knees on at a bar).



Even a 4 foot section of steel bar will bend a little bit. I don't understand how this makes a significant difference in preventing the granite from cracking when someone decides to jump up and down on the countertop.. since the steel bends.



Is this because the steel bends more uniformly across the entire span, whereas plywood can bend at sharp points wherever the plywood has a weak spot? Is it because these steel bars routed into the plywood subtop and glued with epoxy help more with tension and compression, rather than just resisting bending?






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Finding the Semimajor Axis

A planet in another solar system orbits a star with a mass of 4.0 ×1030 kg. At one point in its

orbit it is 250×106 km from the star and is moving at 35km/s. Take the universal gravitational

constant to be 6.67 × 10−11 m2/s2 · kg and calculate the semimajor axis of the planet’s orbit.

The result is:

A. 79 × 106 km

B. 160 × 106 km

C. 240 × 106 km

D. 320 × 106 km

E. 590 × 106 km



I used the formula for the orbital speed v^2 = GM [2/r - 1/a].



Solving for a, I got 1/a=2/r-v^2/GM. Plugging in the given data I got 293x10^6 km. None of the options is relevant with mine. Can someone show me what I did wrong?






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Newton Raphson method and Fixed Point Iteration method ?

Hi everyone, I has been learning numerical method recently, i am very wonder how fixed point iteration method and newton raphson method works (a more insight explanation rather than mathematical proof ) thanks!






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Potential energy from force?

In my physics class, my teacher has been referring to Potential Energy in a 1D force field as the negative integral of the force with respect to position.



AKA:

U(x) = -Int(F(x) dx), where U is the potential energy at x and F is the force at x.



Can someone please explain this to me in conceptual terms?






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Projectile motion, throwing a ball at a coconut

1. The problem statement, all variables and given/known data

You throw a ball at a coconut on a stand 4.0 m in front of you and 1.0 m above the point at which you release the ball. If you throw the ball at 10.0 m/s, at what angle(s) should you throw it? How long is the ball in the air in each case?





2. Relevant equations

##v=v_o + at \\ x=x_o + v_o t + \dfrac{1}{2}at^2 ##





3. The attempt at a solution

I am given the horizontal distance (4.0m), vertical distance (1.0m), and the horizontal initial velocity (10.0m/s). I am looking for the angle θ. I have looked over some videos online and I know that there should be two angles where I can hit the coconut (they are complementary angles). I have trouble finding the angle θ because there are two unknowns in my equation (t and θ). I have split the problem into x and y components.



##v_x = v_ox \\ x = x_o + v_o t \\ v_y = v_oy + a_y t \\ y = y_o + y_o t + \dfrac{1}{2}a_y t^2##



I also used ##v_ox = v_o cosθ \\ v_oy = v_o sinθ## and substituted into the original equations. I have tried to cancel out t and solve for θ but I end up with a equation that involves the tangent and cosine function which I don't think is correct. Is this the correct approach to solving this problem?






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Fatal error: ... functions_autotagger line 279

On thread: http://www.physicsforums.com/showthread.php?p=4521866



I am getting the following error on any action:

Fatal error: Maximum execution time of 30 seconds exceeded in /home/physicsf/public_html/includes/functions_autotagger.php on line 279



Replies seem to be going through though I can't seem to delete the duplicates.



Put this here in case anyone else has seen this.






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Another Moment Problem

Help solve the problem please




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How does an object's velocity change if it's mass suddenly changes?

Let’s say we have two superheroes standing-off in a weightless environment. Assume that their masses are identical (100kg each). Hero-A gets catapulted at Hero-B – left to right. At the moment of collision, Hero-A’s inertia is transferred to Hero-B, and B hurtles off to the right while A is left behind (stationary) - just as it would in the pool-ball examples (conservation of momentum).



Now… instead of bouncing off of each other, let’s say that Hero-A tackles Hero-B and hangs on, effectively DOUBLING his mass at the moment of impact and beyond.

If the speed before impact was 100mph, does that mean that the speed is suddenly cut in half at and after impact (because the mass is doubled)?






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Moment Problem

The first part of the problem is asking moment about point B and the second part is asking moment about point O.




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dense subset and extension of uniformly continuous function

1. The problem statement, all variables and given/known data.

Let ##(X,d)## be a metric space, ##D \subset X## a dense subset, and ##f: D→ℝ## a uniformly continuous function. Prove that f has a unique extension to all ##X##.







3. The attempt at a solution.



I have some ideas but not the complete proof. If ##x \in D##, then I define ##f'(x)=f(x)##, so let ##x \in X \setminus D##. ##D## is a dense subset, so there exists ##(x_n)_{n≥1}## ##\subset D## such that ##x_n→x##. I define ##f'(x)=\lim_{n\rightarrow +\infty} {x_n}##. Observe that this limit makes sense since ##(f(x_n)_n≥1## is a Cauchy sequence (to prove this one has to use the fact that f is uniformly continuous) in ##ℝ##. ##ℝ## is complete, so the sequence is convergent. Then I should check that ##f'## is well defined, in other words, if there are two different sequences ##(x_n)_{n≥1}## and ##(y_n)_{n≥1}##in ##D## converging to a point ##x##, then it must be ##\lim_{n\rightarrow +\infty} {x_n}##=##\lim_{n\rightarrow +\infty} {y_n}## (this is easy to prove). Now I want to prove that f' is uniformly continuous, this means that for every ##ε>0## ##\exists δ_ε>0##:

##d(x,y)<δ_ε## implies ##|f'(x)-f'(y)|<ε##. Here I got totally stuck. This is an exercise belonging to the topic of compact metric spaces so I suppose I have to use something about compact spaces, the problem is that ##ℝ## is not compact, so I don't know where should I use some information about compactness.






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What is band bending and how does it relate to Fermi Energy?

1. The problem statement, all variables and given/known data

Consider a pn junction in Si at 300K (other parameters given), with doping NA = 1021/m3 and ND = 1023/m3. Assume all impurities are ionized. On this basis find the Fermi level on each side. From this find the band bending VB and make a sketch of the pn junction.



2. Relevant equations

[itex]N_e = N_C e^{\frac{-(E_G - E_F)}{k_B T}} [/itex]





3. The attempt at a solution

The Fermi energy calculation was fairly straightforward to solve for, since I just used the formula above for both sides and solved for EF. My question is about band bending. What is it and how do I calculate it? I looked through the relevant chapter in my text-book, but I couldn't find any reference to it. Can someone show me how it relates to the Fermi energy that I have already calculated?






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Magnetic structure

How we can distinguish between different type of magnetic structures by simply looking at neutron diffraction data??






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