Root Mean Squared Voltage

Posted by Mr Mallon on January 7, 2014

Try out this simulation exploring out the relationship between the peak voltage of an a.c. source and the d.c. equivalent voltage.

[kml_flashembed movie=”http://www.helpmyphysics.co.uk/RMS.swf” height=”450″ width=”550″ /kml]

Categories: Higher Physics
7Jan
Comments Off on Root Mean Squared Voltage

The Wheatstone Bridge.

Posted by Mr Mallon on December 17, 2013

[kml_flashembed movie=”http://www.helpmyphysics.co.uk/wheatstonebridge.swf” height=”450″ width=”550″ /kml]

Roll the mouse over the instructions and the think physics button for more information.

The Wheatstone Bridge is used to find the value of an unknown resistor.

When there is no p.d. across the bridge the we say the Wheatstone Bridge is balanced.

If the value of resistance in the decade box is changed then it follows there is a direct proportional change in the current that will flow across the bridge.

wheatstonepractical02.clipular

Provided the resistance is not changed too much away from the balance point then it can be written

daum_equation_1387234537953

Further info about the Wheatstone Bridge
BBC Bitesize Higher Physics: Wheatstone Bridge.

17Dec
Comments Off on The Wheatstone Bridge.

Internal Resistance of an electric cell.

Posted by Mr Mallon on December 14, 2013

InternalResistance

In the simulation below it can be seen that when electric current is taken from an electric cell the potential difference between the terminals decreases.

[kml_flashembed movie=”http://www.helpmyphysics.co.uk/internal_resistance.swf” height=”450″ width=”550″ /kml]

When no current is taken the tpd is at its maximum. This is the EMF of the electric cell.

The EMF of an electric cell is the maximum energy given to each Coulomb of electric charge.

This lost energy per coulomb, usually called “lost volts” is lost in the internal resistance of the electric cell.

You can download a poster for your notebook below.

InternalResistance

14Dec
Comments Off on Internal Resistance of an electric cell.

Internal Resistance of an electric cell.

Posted by Mr Mallon on December 7, 2013

Hi physics lovers. Check these two videos below on internal resistance.

How to calculate the internal resistance of a cell.

Investigating the internal resistance of a cell.

You can download the physics simulation from the here:

PhET Electrical Circuit Simulation

7Dec
Comments Off on Internal Resistance of an electric cell.

Moving Charges in an Electric Field.

Posted by Mr Mallon on November 28, 2013

[kml_flashembed movie=”http://www.helpmyphysics.co.uk/movingcharge.swf” height=”450″ width=”550″ /kml]

Roll mouse over the V, W and Q for definition of these terms.

28Nov
Comments Off on Moving Charges in an Electric Field.

Electric Fields

Posted by Mr Mallon on November 28, 2013

[kml_flashembed movie=”http://www.helpmyphysics.co.uk/electricfield.swf” height=”450″ width=”550″ /kml]

When a physicist talks about a field they are not talking about the green ones with
cows in it.

Rather they mean regions of space where objects experience a force without being touched.

To picture these regions in space physicists use arrowed lines.

The direction of the arrows show the direction where the objects experience the force.

28Nov
Comments Off on Electric Fields

Higher Starter Questions Set 3

Posted by Mr Mallon on November 18, 2013

18Nov
Comments Off on Higher Starter Questions Set 3

Starter Questions Set 02

Posted by Mr Mallon on November 10, 2013

Categories: Higher Physics
10Nov
Comments Off on Starter Questions Set 02

Higher Starter Questions of the Week.

Posted by Mr Mallon on October 31, 2013

Here are the Higher physics starter questions of the week.
You can make the questions full screen by pressing the appropriate controls on the slide.
Clicking the slide will reveal the answers

Categories: Higher Physics
31Oct
Comments Off on Higher Starter Questions of the Week.

Impulse and change of momentum

Posted by Mr Mallon on October 30, 2013

[kml_flashembed movie=”http://www.helpmyphysics.co.uk/impulse.swf” height=”450″ width=”550″ /kml]

When a car is in collision with a wall which brings it to a stop its momentum must be reduced to zero.

The change of momentum of the car is equal to the impulse it receives.

Impulse = change of momentum.
Ft = change of momentum

Now this change of momentum can come about with a LARGE FORCE acting over a small time or a small force acting over a LONG TIME.

The above movie shows the force time graph of two collisions of a car with a wall and then a collapsible wall.

Assuming the car is travelling at the same speed before each collision the change of momentum will be the same in each case.
You can calculate the change of momentum from the area of the force time graph. Note each graph has the same area but the time to change the momentum is different.

You will notice that in the collision with the collapsible barrier the time for the change in momentum is longer. This means that to keep the same area the peak force will be lower.

So to survive collisions it is important to increase the time you take to come to a stop. That is why car safety needs airbags, seat belts and crushable car fronts.

30Oct
Comments Off on Impulse and change of momentum