Profile
Settings
Refer your friends
Sign out
In the physics lab, we have a variety of measuring devices that we utilize to measure different parameters. Some of the instruments utilised in the lab include a voltmeter, an ammeter, a vernier calliper, a screw gauge, and telescopes, among other things. Electricity is measured with the help of instruments such as ammeters and voltmeters. Let us have a look at the ammeter and its specifications in this post to gain a better understanding of them.
VOM (voltage metre) is an instrument that measures the voltage or potential difference between two points of an electronic or electrical circuit, also known as the potential difference metre or potential metre. Typically, the voltmeter is used to measure the voltage of either alternating current (AC) or direct current (DC) circuits. Specialized voltmeters can also be used to measure Radio Frequency (RF) voltage, as an alternative.
Ammeter: An overview
Ammeters were laboratory equipment whose operation was reliant on the earth’s magnetic field to function properly. The invention of the ammeter in the nineteenth century, which had the ability to make exact measurements and could be mounted in any position, was revolutionary.
When it comes to measuring current, an ammeter can be used to measure either alternating or direct current. We are all aware that the ampere is the unit of current measurement. The term “ammeter” refers to the fact that this instrument measures the value in amperes.
In order to measure the current, the ammeter is often connected in series with the circuitry being measured. This device is mostly used for measuring small amounts of current, with the current being measured in the milliampere or microampere ranges of measurement. The milliampere metre is a device that is used to measure current in milliamperes, and the microampere metre is a device that is used to measure extremely small electric currents that are calibrated in microamperes. The ammeter is denoted by the letter “A” in a circuit representation.
Voltmeter: An overview
An electronic voltmeter measures voltages, which are commonly measured in volts, millivolts (0.001 volt), or thousand volts (1,000 volts) (1,000 volts). In order to measure the voltage of a device, a voltmeter must be connected in parallel with the device. This is critical because objects operating in parallel are more likely than not to experience the same potential difference. It is linked in parallel with the circuit primarily because the voltage drop across it is the same as the voltage drop across the circuit.
The internal resistance of a voltmeter is likewise quite high. Most of the time, this is done because it is necessary for measuring the potential difference between the two points of the circuit. As a result, the current flowing through the measuring equipment remains constant. That is to say, the high resistance of the voltmeter will make it difficult for current to flow freely through it. This enables the device to collect accurate voltage readings in the future.
Difference Between Ammeter and Voltmeter
The ammeter is used for measuring small amounts of current, and the result is displayed in milliamperes when the ammeter is connected in series with the circuit to be tested, allowing the full circuit’s current to pass through it.
For the purpose of measuring the potential, a voltmeter is connected in parallel with the electric circuit. Both devices have the same connection polarity, which means that the negative terminal of the device is connected to the negative polarity of the supply and the positive terminal is connected to the positive polarity of the supply.
The voltmeter is connected in parallel since it is only through this configuration that we can measure the potential difference or voltage drop in that element or circuit, as in the case of parallel resistances, the voltage across them will be the same.
The ammeter is linked in series because only the current will properly pass through it in this configuration, but in the case of series resistance, all resistance will have the same current passing through it.
Given that it should enable current to travel through it, the internal resistance of an ideal ammeter will be zero in nature. The ammeter is linked in series with the circuit in order to measure the current flowing through the system. For the perfect voltmeter, the internal resistance should be infinity, as it should not allow any current to flow through the voltmeter. The potential difference is measured by a voltmeter, which is linked in parallel.
Among the most significant differences between the ammeter and the voltmeter is that the ammeter measures current flow, whereas the voltmeter measures the emf or voltage across every two points of the electrical circuit. To increase the resistance of the ammeter, it is necessary to convert it from an ammeter to a voltmeter. This is accomplished by putting a high resistance in series with the ammeter. Let’s say the ammeter range is 0-I0 amps, and we want to convert that to a voltmeter range of 0-V0 volts.
The voltmeter calculates the difference in voltage between two separate points (i.e., on opposite sides of the resistor), but the amount of current flowing through the element between the two sites does not change as a result of this calculation.. The resistance of the device should be extremely high in order to prevent current from being drawn into it.
When it comes to electric circuits, both of these devices are useful, but the fundamental difference between them lies in the fact that an ammeter is useful for measuring current flow, whereas a voltmeter is useful for measuring voltage or emf across two points in an electric circuit.
Motion in a curved line
When the body moves in a curved path, this is the motion. It’s also two- and three-dimensional motion. As a result, pure translational motion does not have to be in a straight line all of the time. If an object goes in a curved path without changing its orientation, this situation is feasible.
Example. Motion of a projectile
Motion that is translatory (type curvilinear)
A parabolic path is followed by a ball.
The ball in question is thrown from point O and travels through points A and B to arrive at point C, as shown in the diagram. Projectile motion is the name for this type of movement. Curvilinear motion is the nature of projectile motion. To get from point O to point C, the ball is moving in a curved path rather than a straight line.
Conclusion
The number of various perceptions of rotation on the body that may be produced is zero. As a result, when the net force and net torque acting on the body is zero, we can deduce that the rigid body is in mechanical equilibrium. The directions must be taken with suitable sign conventions because the forces and torques are vector quantities.
