Chapter 5: Problem 1
Why is the number of independent dimensionless groups never more than the number of quantities?
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Chapter 5: Problem 1
Why is the number of independent dimensionless groups never more than the number of quantities?
These are the key concepts you need to understand to accurately answer the question.
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Use the dimensions of \(B\) (Problem5.4.5) and of the permeability of free space \(\mu_{0}\) (Problem \(5.4 .6\) ) to find the magnetic field \(B\) at a distance \(r\) from an infinitely long wire carrying a current \(I .\) The missing dimensionless prefactor, which dimensional analysis cannot tell us, turns out to be \(1 / 2 \pi\). Magnetic-resonance imaging (MRI) machines for medical diagnosis use fields of the order of 1 tesla. If this field were produced by a current-carrying wire \(0.5\) meters away, what current would be required? Therefore, explain why these magnetic fields are produced by superconducting magnets.
Express the dimensions of capacitance and inductance using \(\mathrm{L}, \mathrm{M}, \mathrm{T}\), and \(\mathrm{Q}\). Then write them using \([V]\) (the dimensions of voltage) along with any fundamental dimensions that you need.
In this problem, you apply dimensional analysis to the low-pass \(R C\) circuit that we introduced in Section 2.4.4. In particular, make the input voltage \(V_{\text {in }}\) zero for time \(t<0\) and a fixed voltage \(V_{0}\) for \(t \geq 0 .\) The goal is the most general dimensionless statement about the output voltage \(V\), which depends on \(V_{0}, t, R\), and \(C\). a. Using \([V]\) to represent the dimensions of voltage, fill in a dimensional- analysis table for the quantities \(V, V_{0}, t, R\), and C. b. How many independent dimensions are contained in these five quantities? c. Form independent dimensionless groups and write the most general statement in the form group containing \(V\) but not \(t=f(\) group containing \(t\) but not \(V, \ldots)\) where the ... stands for the third dimensionless group (if it exists). Compare your expression to the analysis of the \(R C\) circuit in Section 2.4.4.
Just as electric fields depend on \(\epsilon_{0}\), the permittivity of free space, magnetic fields depend on the constant \(\mu_{0}\) called the permeability of free space. It is defined as $$\mu_{0} \equiv 4 \pi \times 10^{-7} N A^{-2}$$ where \(\mathrm{N}\) is a newton and \(\mathrm{A}\) is an ampere (a coulomb per second). Express the dimensions of \(\mu_{0}\) in terms of \(\mathrm{M}, \mathrm{L}, \mathrm{T}\), and Q. Then use the dimensions of magnetic field (Problem \(5.4 .5\) ) to find the energy density in a magnetic field \(B\). (As with the electric field, the dimensionless prefactor will be \(1 / 2\), but dimensional analysis does not give us that information.) What analogies can you make between electrostatics and magnetism?
A magnetic field \(\mathbf{B}\) produces a force on a moving charge \(q\) given by $$\mathbf{F}=q(\mathbf{v} \times \mathbf{B})$$ where \(\mathbf{v}\) is the charge's velocity. Use this relation to find the dimensions of magnetic field in terms of \(\mathrm{M}, \mathrm{L}, \mathrm{T}\), and \(\mathrm{Q}\). Therefore, give the definition of a tesla, the SI unit of magnetic field.
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