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How to linearize equations to y = mx + b form (more information below)?
studiot replied to V21's topic in Homework Help
If one variable decreases as the other increases then they have an inverse relationship. Is this not true of L and f thus? [math]{\rm{L(plus}}\,{\rm{a}}\,{\rm{constant)}}\quad {\rm{ = }}\quad \frac{{{\rm{(a}}\,{\rm{constant)}}}}{{\rm{f}}}[/math] So do you know any relationship (for sound waves ?) involving any of the quantities in the original given equation ? You are looking for an equation of the form [math]{\rm{something = }}\frac{{{\rm{something}}\,{\rm{else}}}}{{\rm{f}}}[/math] -
How to linearize equations to y = mx + b form (more information below)?
studiot replied to V21's topic in Homework Help
I am assuming you want to achieve a straight line of the form y = mx + b, where m and b are constants. Strange though it may seem, this is not actually a 'linear' equation, so it is better not to use that description. 'Linear' has a special meaning in maths. y = mx is linear y= mx + b is what is known as affine. Back to your questions. starting with number 5 Your two variables are length L and frequency. f. the velocity, v and end correction, e are stated to be constants. But there is an inverse relationship between variables L and f. So you need to somehow introduce a new variable by inverting one of these. Can you think of a relationship (another equation) for either L or f that will do this? -
Well explain what your rules are and what your objectives are. Interaction of matter waves is an everyday common or garden event in this universe. The point is twofold (1) To have a wave you need a wave equation to be satisfied. There are varying degrees of sophistication of wave equations. (2) To pick out the appropriate solution to said wave equation you also need to apply boundary conditions. In both (1) and (2) we normally use appropriate versions to the situation.
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You are getting there. The tolerance standards refer to laboratory glassware in general and include glassware (flasks, pipettes etc) that have only one measuring line and no scale. As such they are designed to deliver the rated quantity /- rated tolerance. Since you compared this with engineering practice, consider this. A tape measure with one inch missing from the end will 'measure' a 10 foot wall as 10 feet and 1 inch, from the end. But by measuring from the 1foot marking to the 11 foot marking, the correct length of 10 feet will be obtained. This is because the tape has an error everywhere of 1 inch so using a mesurement by difference this cancels. Length of wall = (11' 0") - (1' 0") = 10 feet. The burette allows this measurement by difference so the resolution and accuracy are not necessarily limited by the overall tolerance. But inEngineering you also have 'limits and fits' tolerance. Suppose you are turning a bar down to 'just fit' through a particular hole. What tolerance would you enforce to turning the bar down? This is equivalent to using a measuring flask where you cannot measure volume by difference. Your tolerance refers to the whole diameter and again you cannot use difference. Remember also that there are other considerations that affect accuracy with a burette and if you try to get too accurate you need to start to consider air bubbles, temperature, liquid density and the scale accuracy of the burette and techniques to ensure that all the liquid you think is transferred actually reaches the receiving vessel. At this point you might move to weight measurement rather than volume.
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You need to distinguish between tolerance (which affects accuracy) and reading resolution (which affects precision). Tolerance is a specification of full scale ie a nominal delivery of 50ml will be within the range 49.95mL to 50.05 mL. This is a characteristic of the instrument (in this case a burette or buret in US) This gives a relative tolerance of 0.13% The actual scale can be read more finely than this. This effect is common in many instruments where a scale is read rather than a digital readout obtained. For example mechanical verniers, analogue voltmeters. For both of these latter tolerance is usually given as the relative (of full scale) %. Such a voltmeter would always be specified as 1% (very good) 5% (good) 10%(El cheapo variety). Remember for readings that are made by difference (as in a burette) the tolerance is a systematic error that affects both reading equally and with the same sign so cancels out on subtraction. That leaves reading resolution. This is measured as the smallest scale graduated interval (usually 0.1mL for a 50 mL burette), or some fraction of it. (ASTM E287-02) has half of this at 0.05mL. Vogel suggests this for "all ordinary work", but reading to 0.01 or 0.02 mL with the aid of a lens, "for precision work". Precision work could also entail establishing a calibration curve for use over the whole length of the burette or alternatively repeating the measurement over several different parts of the sscale and averaging.
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FLUIDS (Pressure in a fluid of uniform density
studiot replied to Lizwi's topic in Classical Physics
Timo's posh explanation is just fine but try this simplified one. Looking at the diagram I see that upwards is defined positive. Looking at your equation and the diagram pA - (p+dp) A - ρgAdy So I see that the arrow on the underside is pointing up so pA is positive. But on the top, p and dp point downwards so are negative so (p+dp) is negative on the top dy is positive and g is negative so the third term is also negative. does this help? -
Relativity (split from Can relativity be applied to light speed?)
studiot replied to MPMin's topic in Relativity
Enough pseudomathematics. "more accurately" is a mathematical statement but I see no mathematics. Furthermore the rules here require answers to polite questions and comments from other members -
Relativity (split from Can relativity be applied to light speed?)
studiot replied to MPMin's topic in Relativity
A point is not a frame (hint that is why we have separate words). Besides which the Universe as a whole has no centre. Swansont's reference to a centre was referring to a finite system of bodies not the whole universe. -
Relativity (split from Can relativity be applied to light speed?)
studiot replied to MPMin's topic in Relativity
Well the original question says that the body never experiences a force. But it does not say for how long this period of grace last in the history of the body. I also mentioned momentary conjunctions of the generators of forces acting on the body where the net force is zero. Obviously, in a universe where nothing is moving, no matter how far apart (in space) two bodies are, the 'force field' generated by one will eventually affect the other, though there will be a time lag. The bodies may however be moving so that causal connection comes into play, as Mordred comments. But I would add a rider to his comment that causal connection is not immune from disturbance by a third body which may push something into or out of the connection light cone region. -
Relativity (split from Can relativity be applied to light speed?)
studiot replied to MPMin's topic in Relativity
Thank you for the response, but it is not necessary to consider gravity. Unless the bodies are at exactly the same temperature, there will exist some sort of radiation pressure between them. -
Relativity (split from Can relativity be applied to light speed?)
studiot replied to MPMin's topic in Relativity
I have three points nobody seems to have considered, to add to this discussion. Firstly this idea of a virgin body that has never felt a force. That’s why they might actually be stationary, in other words, no momentum. If an object has experienced a force to make it move surely it has momentum, wouldn’t it make sense to then choose a frame of reference that hasn’t had a force applied to it? Within the bounds aof all known mathematics this requires a single body in an otherwise empty universe. As soon as you introduce more than one body there will always be some sort of force between them. Secondly zero momentum could be momentary (and frame dependant), but the requirement has always been zero net force, not zero force. Thirdly there is no magic in pair production from radiation. -
Maxwell equations vs Lorentz transformation of fields
studiot replied to Danijel Gorupec's topic in Physics
Yes I think it is oft forgotten that relativity acts (directly) only on space and time so affects things only insofar as they link to have a connection to these variables. So for electrodynamics the charges remain the same but the space and tinme interval between them alters, thus altering density (scalar) and rate of change properties (vector). I can post another short extract (from Grant and Phillips) detailing the oblateness you referred to if you like. -
Maxwell equations vs Lorentz transformation of fields
studiot replied to Danijel Gorupec's topic in Physics
Yes I understood that, which is why I asked for more detail. Whenever you have relative motion you must, of necessity, have (at least) two frames. One for each of the objects in relative motion. The rest frame of one of these is chosen as the 'rest frame' and the rest frame of the other, the moving frame. Furthermore the observer's frame also needs some charge to be able to interact with (and thus observe) any fields generated by the moving charge. You have introduced 'relativity'. Have you considered whether the observers in the observer frame will measure the same charge as observers in the frame of the moving charge? This is indeed the case - charge is invariant under the Lorenz transformation so both will agree the value of the charge. However it is variation of charge density that produces the fields. Charge density is not Lorenz invariant so each will measure a different charge density. This is often handled by using Maxwell's equations to introduce what are known as vector potentials. Now Maxwell's equations are (simultaneous) partial differential equations and when we solve them for the fields or potentials we do not obtain unique solutions. Solutions differ by arbitrary (vector) functions. The required solutions are picked out by applying further conditions (boundary conditions) and inparticular what is known as The Lorenz Condition. https://en.wikipedia.org/wiki/Lorenz_gauge_condition Note this is not the Lorenz transformation. Classically this leads to what are known as 'retarded potentials'. When we introduce relativity, it is often easier to use four-vectors than work directly. Here is a simple non four-vector explanation due to Grant and Phillips that may help. Notice their footnote as to how positive and negative charge do not necessarily transform the same under Lorenz. -
Maxwell equations vs Lorentz transformation of fields
studiot replied to Danijel Gorupec's topic in Physics
What do you mean by "the particle is moving in his frame of reference" ? Can you rephrase this properly identifying the frames you wish to employ? -
Best lattice structure/geometry for strength and minimal heat transfer?
studiot replied to Engineer43's topic in Engineering
This is an interesting question to discuss although it is probably too late since you haven't look back since the day after you first posted. I think this is key and I would add to that the question What do is meant by lattice? Does this refer to the physical arrangement of atoms or a truss arrangement of structural components of some sort? Various deductions as to the use can be made from the all too limited information provided, especially since the main load is described as compression / shear, which will be at direct odds with the low thermal conductivity requirement. Various lamination schemes may be proposed to address this, but details will depend upon more complete and exact information being supplied. To others: Is it worth continuing this discussion? -
OK that looks a whole lot better. Hopefully you feel good too since I didn't do it for you, just offered a hint. One small niggle. My calculator says that 35/18 = 1.94 not 1.95. In fact there is no need to work this out at all. Just leave the common acceleration* as [math]\left( {\frac{{35}}{{18}}} \right)[/math] Then you can multiply it all out at the end. Very often something will cancel out and make it even easier. [math]F = ma = 8000*\left( {\frac{{35}}{{18}}} \right)[/math] * Notice also how to spell acceleration.
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Agreed dimension is not the best word. Yes realm if you like: that is unused. Since you are now listening +1 for encouragement. To carry on the discussion can you tell me what you understand by 'detection' or 'observation' please? These terms do have a specific meaning which roughly corresponds to 'any interaction' with the rest of the universe'. Also you need to discuss boundary conditions when using a wave function.
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Thank you for this useful reply. What would also be useful would be some feedback about my thoughts on your posts. I really have no idea what you have understood or agreed. Also some idea of the level of maths you can cope with would be useful. You can't do this without some maths. So consider again a simplified 2D x-y system. Now let x = Acos(t) and y = Asin(t) I have used t, since it is conventional. t is known as a parameter or sometimes a running variable. t is used because the running variable is often time. What it does is reduces a 2D system to a 1D system at the cost of introducing conditions by way of the two equations. And time is used to link the (spatial) dimensions as you requested. Conventional time has the same properties as a parameter vaiable. It 'runs' evenly, with no gaps or jumps - the same property as real numbers and the calibration on our x and y axes. But do real objects behave in this manner? Well the East Coast Main (railway) line in Scotland is single track, North of Edinburgh. This means that if an express train is 'stuck' behind a slow train it has to follow at the speed of the slow train. It cannot pass. In fact all the trains on the railway must follow at same speed to avoid collisions. This must also be the case with a single time axis. Everything travels at a constant even rate through the single time axis. Perhaps this is why you have proposed more than one? Of course in space different objects can travel at different speeds without collisions because a faster object can move sideways around a slower one, and also because there are relatively enormous gaps between objects in space. So far as I know we have never observed this type of behaviour involving the single time axis we can observe. In fact it seems choc-a-bloc with objects. I look forward to your comments.