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Page 695: Standardized Test Practice
In order to solve this problem let’s write the EMF equation which is given as
$$
EMF=BLv
$$
The dimension analysis of each term gives that
$$
B=textrm{T}=frac{textrm{N}}{textrm{m}cdottextrm{A}}
$$
$$
L=textrm{m}
$$
$$
v=frac{textrm{m}}{textrm{s}}
$$
After we insert this into the EMF equation we get
$$
textrm{V}=frac{textrm{N}}{textrm{m}cdottextrm{A}}cdot mcdotfrac{textrm{m}}{textrm{s}}
$$
So the correct answer should be B, if we assume that there is a typo in the problem.
$$
EMF=BLv
$$
From here, one can express the magnetic field as
$$
B=frac{EMF}{Lv}=frac{4.2}{0.427times 0.186}
$$
Finally, one obtains that
$$
boxed{B=52.9textrm{ T}}
$$
So the correct answer is D.
$$
EMF=BLv
$$
Which after we plug in the values gives
$$
EMF=1.4times 0.15times 0.12
$$
Finally, we have that
$$
boxed{EMF=0.025textrm{ V}}
$$
So the correct answer is C.
$frac{I_s}{I_p}=frac{V_p}{V_s}=frac{N_p}{N_s}$
Now, we can express the current in the primary circuit
$$
I_p=frac{V_s}{V_p}I_s=frac{13}{91}times 1.9
$$
Which gives that
$$
boxed{I_p=0.27textrm{ A}}
$$
So the correct answer is A.
We start from the formula for the effective voltage which says
$$
V_{eff}=frac{sqrt{2}}{2}V_{max}
$$
So after we plug the values
$$
V_{eff}=frac{sqrt{2}}{2}202
$$
$V_{eff}=142.8textrm{V}$
Now, we can use Ohm’s law to find the effective current
$$
I_{eff}=frac{V_{eff}}{R}=frac{142.8}{480}
$$
Finally
$$
boxed{I_{eff}=0.298textrm{A}}
$$
So the correct answer is A.
$$
I_1=frac{P}{V_1}=frac{800}{160}=5textrm{ A}
$$
Now, the dissipated power is given as
$$
P_1=RI_1^2=2times 5^2=50textrm{W}
$$
In the second case we have that
$$
I_2=frac{P}{V_2}=frac{800}{960}=0.833textrm{ A}
$$
and the dissipated power is given as
$$
P_2=RI_2^2=2times 0.83^2=1.4textrm{W}
$$
We conclude that higher voltages yield with lower power loss which explains the high-voltage power lines connecting large distances.