For an $N$-turn circular coil, $B=N\mu_0I/(2R)$. With $N=100$, $I=0.40\,\text{A}$ and $R=0.080\,\text{m}$, $B=100(4\pi\times10^{-7})(0.40)/(2\times0.080)=3.1\times10^{-4}\,\text{T}$.
$3.1\times10^{-4}\,\text{T}$.
For a long straight wire, $B=\mu_0I/(2\pi r)$. Thus $B=(4\pi\times10^{-7})(35)/(2\pi\times0.20)=3.5\times10^{-5}\,\text{T}$.
$3.5\times10^{-5}\,\text{T}$.
Magnitude is $B=\mu_0I/(2\pi r)=2\times10^{-7}(50)/2.5=4.0\times10^{-6}\,\text{T}$. Using the right-hand rule with current from north to south, the magnetic field at a point east of the wire is vertically upward.
$4.0\times10^{-6}\,\text{T}$, vertically upward.
The magnitude is $B=\mu_0I/(2\pi r)=2\times10^{-7}(90)/1.5=1.2\times10^{-5}\,\text{T}$. With current from east to west, the right-hand rule gives the field below the wire towards south.
$1.2\times10^{-5}\,\text{T}$, towards south.
Force per unit length is $F/l=IB\sin\theta$. Thus $F/l=8(0.15)\sin30^\circ=0.60\,\text{N m}^{-1}$.
$0.60\,\text{N m}^{-1}$.
The wire is perpendicular to the solenoid axis and hence perpendicular to the magnetic field, so $F=IlB$. With $l=0.030\,\text{m}$, $I=10\,\text{A}$ and $B=0.27\,\text{T}$, $F=10(0.030)(0.27)=8.1\times10^{-2}\,\text{N}$.
$8.1\times10^{-2}\,\text{N}$.
Force on length $l$ of one parallel wire is $F=\mu_0I_1I_2l/(2\pi d)$. Substituting $I_1=8.0\,\text{A}$, $I_2=5.0\,\text{A}$, $l=0.10\,\text{m}$ and $d=0.040\,\text{m}$ gives $F=2\times10^{-7}(8)(5)(0.10)/0.040=2.0\times10^{-5}\,\text{N}$. Same-direction currents attract, so the force on A is towards B.
$2.0\times10^{-5}\,\text{N}$, towards wire B.
Total turns are $5\times400=2000$, and length is $0.80\,\text{m}$, so $n=2000/0.80=2500\,\text{m}^{-1}$. For a long solenoid, $B=\mu_0nI=(4\pi\times10^{-7})(2500)(8.0)=2.5\times10^{-2}\,\text{T}$.
$2.5\times10^{-2}\,\text{T}$.
Torque on a current loop is $\tau=NIAB\sin\theta$. Here $A=(0.10)^2=0.010\,\text{m}^2$, $N=20$, $I=12\,\text{A}$, $B=0.80\,\text{T}$ and $\theta=30^\circ$. Thus $\tau=20(12)(0.010)(0.80)(0.5)=0.96\,\text{N m}$.
$0.96\,\text{N m}$.
Current sensitivity is proportional to $NAB/k$. Since $k$ is the same, $S_{I2}/S_{I1}=(N_2A_2B_2)/(N_1A_1B_1)=42(1.8\times10^{-3})(0.50)/[30(3.6\times10^{-3})(0.25)]=1.4$. Voltage sensitivity is current sensitivity divided by resistance, so $S_{V2}/S_{V1}=1.4(R_1/R_2)=1.4(10/14)=1.0$.
(a) $1.4$; (b) $1.0$.
Because $\mathbf{v}\perp\mathbf{B}$, the magnetic force $e vB$ is perpendicular to the velocity at every instant and does no work; it only changes the direction of motion, producing circular motion. Equating $evB=mv^2/r$ gives $r=mv/(eB)$. With $B=6.5\times10^{-4}\,\text{T}$, $r=(9.1\times10^{-31})(4.8\times10^6)/[(1.5\times10^{-19})(6.5\times10^{-4})]=4.5\times10^{-2}\,\text{m}$.
The magnetic force is always perpendicular to the velocity and acts as centripetal force; the radius is $4.5\times10^{-2}\,\text{m}$.
The cyclotron frequency is $f=eB/(2\pi m)$. Using the printed constants, $f=(1.5\times10^{-19})(6.5\times10^{-4})/[2\pi(9.1\times10^{-31})]=1.7\times10^7\,\text{Hz}$. The speed cancels in the derivation because $r=mv/(eB)$ and $f=v/(2\pi r)$.
$1.7\times10^7\,\text{Hz}$; it does not depend on the electron's speed.
The counter torque must equal the magnetic torque $\tau=NIAB\sin\theta$. The area is $A=\pi R^2=\pi(0.080)^2=2.01\times10^{-2}\,\text{m}^2$. Hence $\tau=30(6.0)(2.01\times10^{-2})(1.0)\sin60^\circ=3.1\,\text{N m}$. The torque on a planar current loop in a uniform field depends on $NIA$ and the angle between area vector and field, not on the detailed shape, so the answer would not change.
(a) $3.1\,\text{N m}$. (b) No, if the area and all other particulars remain the same.