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Jeremy Burke
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Jeremy Burke said:the question is to solve Vx. chegg did a kvl in the middle mesh and it turned out to be -2+Vx+8=0, i was wondering why they just ignored the 6 amp source in the kvl. i understand no voltage can be dropped across an ideal current source so why can we just skip over the 6 amp source and go to the 2 ohm resistor![]()
Current sources don't care about voltage polarity. They simply maintain the required current in the specified direction. Again, an ideal current source will produce any potential difference necessary in order that it maintains its specified current. Even if that potential change is negative in the direction of the current.Jeremy Burke said:then i don't understand why the solution was showing -2. since the current is point upward, wouldn't that make the positive end on the bottom, making it +2 and not -2
In this case, taking your "KVL walk" around the loop including the 2 Ω resistor does the trick. In the figure below, the first potential change is -2 V as you "walk" through that resistor:Jeremy Burke said:then how do we decide whether or not the 2 is positive or negative
KVL stands for Kirchhoff's Voltage Law, which is a fundamental law in circuit analysis that states that the algebraic sum of voltages in a closed loop of a circuit must be equal to zero.
KVL is used to analyze and solve complex circuits by applying the law to different loops in the circuit and setting up equations to solve for unknown voltages or currents.
Yes, KVL can be applied to any circuit, whether it is a simple or complex circuit. It is a fundamental law that applies to all types of circuits.
KVL is based on the assumption that all the components in a circuit are connected in series and that there are no parallel branches. This means that it cannot be applied to circuits with parallel components or non-linear components.
KVL is based on the principle of conservation of energy, which states that energy cannot be created or destroyed, only transferred. KVL ensures that the sum of voltages in a circuit is equal to the total energy supplied by the voltage source.