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You've probably heard of Einstein's famous equation: $$e = mc^2$$ This states that mass and energy are equivalent, and indeed the LHC turns energy into matter every day. So to find the mass equivalent to an electron volt just convert eV to Joules and divide by $c^2$. 1 electron volt = $1.60217646 \times 10^{-19}$ joules, so 125 GeV is: $$125 \times ... 9 The way you convert between units is really just multiplying by several factors of 1. But it's 1 written in a slightly unusual way. Think about this: you're probably familiar with conversion factors in the form$$(\text{number})(\text{unit}) = (\text{other number})(\text{other unit})$$But of course, you can divide both sides of any equation by the same ... 9 Short Answer You've hit upon the quirk that the SI and CGS systems not only measure electric charge with different units, but also assign them different dimensionality. In SI, the Ampere is a base unit. Amperes are not made out of anything else - they are primitive, like meters, kilograms, and seconds. One Ampere is one Coulomb per second, so the unit of ... 7 A picture, as they say, is worth a thousand words: See that, in fact, the ratio of Fahrenheit to Celsius is:$$ \dfrac{32 + \frac{9}{5}x}{x}$$where x is the temperature in degrees Celsius. Clearly, the reason the ratio is not constant is the presence of the constant offset 32. Only in the limit of arbitrarily high temperature does the ratio ... 6 Which units are fundamental and which are derived is pretty much a matter of arbitrary convention, not an objective fact about the world. You might think that the number of fundamental units would be well-defined, but even that's not true. Take electric charge for example. In the SI system of units (i.e., the "standard" metric system), charge cannot be ... 6 It's an energy. The SI unit for energy is a Joule. If the theory is going to predict an energy-mass correspondance, then it better give the energy in units of energy. If the units of mc^{2} didn't work out, for the equation to make any sense, you'd have to include some constant \alpha so that E=\alpha mc^{2} would have units of energy on both sides. ... 6 Yes the dimension is different. In SI the current (A) a base unit independent from length (m), mass (kg) and time (s) because we choose to, but in CGS Gaussian unit this is not (1 unit of current = 1 g1/2 cm3/2 s-2), by setting \epsilon_{0,SI} = \frac1{4\pi}. This also leads to some perhaps unintuitive results, like the unit capacitance in CGS Gaussian is ... 6 An electron volt is just the energy acquired when an electron of charge e falls through a potential of 1 volt, which means$$1eV = e \times 1 = 1.6 \times 10^{-19} J$$When you lift up your 2.5Kg laptop (a 15-inch apple macbook pro, for example) by a foot, you do a work of approximately 2.5 Kg \times 10 ms^{-2} \times 0.3 m = 7.5 J which is about 4.7 ... 5 It is the convention of setting the velocity of light c=1 that allows for this, the natural units, otherwise it is \mathrm{GeV}/c^2 The rest mass energy connection$$E^2=p^2+m^2$$at rest then the mass is identified with energy in natural units. 5 As far as I can tell, you went wrong in a couple of places: instead of converting from \mathrm{g} to \mathrm{mg} your converting to \mathrm{kg} in your first term, and in your fourth term, the units should be \mathrm{g\, O_2} and \mathrm{ nmol\, O_2}, for consistency. This would've let you know that you've inverted your conversion from \mathrm{ ... 5 As lurscher mentioned in a comment, you're using the wrong units for magnetic susceptibility. \chi is actually a dimensionless number that is related to the magnetic permeability of a material relative to that of a vacuum. I think you were mixing it up with the molar magnetic susceptibility, which is \chi_\text{mol} = \mathcal{M}\chi/\rho, where ... 5 Pure convention. There is no reason alternative conventions couldn't be used, apart from the need to avoid confusion. Newton introduced the constant to make the force law simple, whereas the electrostatic definition with the 4\pi is designed to make Poisson's equation (one of the equations for the electric field) look simple. You can write a Poisson ... 5 The natural way to write it in this notation is$$F = q(E + \beta \times B)$$where \beta is the velocity measured in natural units - the velocity as a fraction of the speed of light. In the CGS system, we instead write \beta = \frac{v}{c} and the equation becomes$$F = q(E + \frac{v}{c} \times B)$$That's not silly enough, though, so we go really ... 4 If the height difference between the mercury level in the two arms is h (it's called \Delta h on the figure), then$$P_1 - P_2 = h\rho g$$where P_1,P_2 are the pressures in both wings (called P,P_{\rm ref} on the figure). One of them is the measured atmospheric pressure. The two pressures are being subtracted because the air pushes the liquid ... 4 I suppose (or hope, for I'd agree) he means equations where the variables are plain numbers rather than physical values, and the units are written out in the equations. Like$$ F\:\mathrm{N} = \frac{E\:\mathrm{J}}{s\:\mathrm{m}} $$i.e. "F Newtons equal E Joules over s meters". Which is a really horrible way of writing equations, and particularly ... 4 The unit can be anything as long as you carry out the proper conversion. If you're using KeV and MeV, there isn't any complete unit system that specifies the units of speed (which we need to convert to mass). Usually, particle physicists use MeV as a mass unit as well as energy (thereby setting c=1 in this unit system). Later on stuff can be ... 4 Defining the symbol k in Coulomb's law,$$F=k\frac{q_1q_2}{r^2},$$to be k=1/4\pi\epsilon_0, is perfectly allowed when one understands it simply as a definition of \epsilon_0. The motivation for this definition is that when you work out the forces between two oppositely charged plates of area A and charge Q a distance d apart, they come out as ... 3 I think it has something to do with old electromagnetism units, which was vastly more complex than centimetres to inches conversion. I'm too young to have been exposed to the horrors of -cgs--units in electromagnetism so all the following is only an educated guess. My guess is due to some googling, with "measure equation" coming up in old papers associated ... 3 The unit of the second is defined is the time duration of a certain number of periods of radiation emitted from a particular type of electron transition between energy levels in an isotype of Cesium (see here). It is an assumption that light travels at a constant speed c independent of one's reference frame, so now that we have fixed a unit of time, we ... 3 The simplest way to think of Avogadro's number is as a unit conversion factor. Just as there are 2.54 centimeters in an inch, there are Avogadro's number atomic mass units in a gram. Accordingly, if you know the atomic mass of an element you can count the number of atoms in one gram of it. Let's take carbon as an example. The most common isotope of carbon ... 3 This is difference in the unit system. The former uses SI units, where the latter uses cgs/Gauss system. In Gaussian units, unlike SI units, the electric field E and the magnetic field B have the same dimension. This amounts to a factor of c difference between how B is defined in the two unit systems, on top of the other differences. ... 3 What RedGrittyBrick said in his comment is correct, but as you need to understand kWh I'll try to explain a bit more. There are two main things you need to take into account: the total energy in your fuel cell (in kWh) and the maximum power it can deliver (in kW). Power is the rate at which energy is used. In electricity, 1W is equal to 1V times ... 3 Linearity does not necessarily mean a ratio exists. Linearity in this case means that a given change in one variable causes the same change in the other variable no matter what the value of the variable was before the change. As explained by the other answers, F=32+\frac95 C. F is a linear polynomial in C (i.e, F(c)=aC+b), but F is not a linear map ... 2 The secret to unit conversions is to keep multiplying by 1. However, we need specially chosen values of 1. A common value of 1 we can use is 60 min/hour or 3600 sec/hour. Another commonly used value of 1 is 1000 m/km, and it's inverse, km/1000 m. In your case, we need to do two conversions. hm -> km. So our chosen value of 1 is km/10hm. The other one ... 2 I think David's answer is the right one. Here is the wrong one, but it's the way I actually think about unit conversions when I do them. (I mean "wrong" in the sense of "unofficial", not that it gives the wrong answer.) Suppose I tell you there are 5280 feet in a mile, and ask how many feet are in two miles. You don't need to think about what to do. ... 2 The units you mean are probably kg*cm (sometimes written kg.cm in robotics). Your original specification of 24 kgcm is a torque and not a force. The difference in practice is that, as the units imply, your resulting force at a point a distance from the "pivot point" decreases by the distance. So 24 kg*cm means that it can hold 24 kg at 1 cm or 12 kg at 2 cm ... 2 You can leave the 14hm/min just as it is, if you like. Convert the 6 hours to how many minutes there are in 6 hours, 6 hours times 60 minutes per hour = 360 minutes. The comments on your Question are beside the point, hm could be half-meters, hectometers, whatever, ... — if one travels 14 “hm”s in 1 minute, then one travels 360 times 14 ... 2 You can solve this by picking a simple, specific example and then generalizing it as necessary. Let’s start with a simple case, where the tempo is such that there are 120 quarter notes per minute. The frequency of quarter notes is then$$ \frac{\text{120 quarter notes}}{\text{1 minute}} \cdot \frac{\text{1 minute}}{\text{60 seconds}} \cdot \frac{\text{1 ...

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the line you wrote 105,000 $\frac{kg}{m*s^2}$ * 330 K * 287 $\frac{m^2}{s^2*K}$ has to read in fact $\frac{105,000 \frac{kg}{m*s^2} }{ 330 K * 287 \frac{m^2}{s^2*K}} = 1.11 \frac{kg}{m^3}$. This comes from the gas law $p=\rho \ R \ T$ where $p$ is the air pressure and $\rho$ is the air density. Solving for $\rho$ you get $\rho =\frac{p}{R T}$ ...

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A kilowatt is a unit of power, which has the dimensions of energy over time. A kilowatt-hour, then, has dimensions of energy. As a simple example, if you wanted to charge up a battery so as to operate a 1,000-watt (DC) heater for one hour, you'd need one kilowatt-hour of energy (assuming the mythical world of perfectly efficient batteries, lossless wires, ...

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