Physics 272 March 4 Spring 2014 http://www.phys.hawaii.edu/~philipvd/pvd_14_spring_272_uhm.html Prof. Philip von Doetinchem philipvd@hawaii.edu Phys272 - Spring 14 - von Doetinchem - 1 Summary ● Example: rectangular loop in a uniform magnetic field – The total force on the loop is zero – But the total torque is generally not zero 0 µ Phys272 - Spring 14 - von Doetinchem - 2 Summary Phys272 - Spring 14 - von Doetinchem - 3 Summary ● ● ● Greatest torque when magnetic dipole moment and magnetic field are perpendicular Torque is zero when magnetic dipole moment and magnetic field are (anti)parallel Analogue to electric dipole moment and electric field Phys272 - Spring 14 - von Doetinchem - 4 Summary ● Conductor strip perpendicular to a magnetic field ● Magnetic force causes polarization effect in material ● Electric field between lower and upper side of strip builds up Phys272 - Spring 14 - von Doetinchem - 5 Sources of magnetic fields ● 2002 2009 Current carrying coils (solenoids) can produce massive uniform magnetic fields ← particle physics experiment CMS at CERN in Geneva uses a solenoid Phys272 - Spring 14 - von Doetinchem - 6 Magnetic field of a moving charge ● ● ● ● ● How are magnetic fields created? Permanent magnets and electric currents create magnetic fields Magnetic field exerts a force only on moving charge Moving charges inside atoms feel magnetic forces, but can also act as sources Start simple: single point charge moving with a constant velocity Phys272 - Spring 14 - von Doetinchem - 7 Magnetic field of a moving charge ● ● Similar approach to electric field with point charges → be careful similarities and differences exist Magnetic field magnitude 2 is proportional to charge and 1/r , but the direction of magnetic field is not along the line of the charge and the point of interest Phys272 - Spring 14 - von Doetinchem - 8 Vector magnetic field Phys272 - Spring 14 - von Doetinchem - 9 Moving charge: magnetic field lines ● ● ● ● Moving point charge has electric field and magnetic field Electric field lines point radially inwards or outwards Magnetic field lines are circles around centered on the line of the velocity and lying in perpendicular planes to this line Ignore acceleration of charges in bends of wires because the drift velocity in conductors is so small → stick to assumption of constant velocity Phys272 - Spring 14 - von Doetinchem - 10 Forces between two moving protons Phys272 - Spring 14 - von Doetinchem - 11 Forces between two moving protons Phys272 - Spring 14 - von Doetinchem - 12 Forces between two moving protons Phys272 - Spring 14 - von Doetinchem - 13 Forces between two moving protons Force the upper proton → feels from the magnetic field of the lower proton (repulsive) Phys272 - Spring 14 - von Doetinchem - 14 Forces between two moving protons ● ● ● Two protons moving in the same direction. Magnetic force on the upper proton from the magnetic field of the lower proton: attractive Magnetic force on the lower proton from the magnetic field of the upper proton: attractive Phys272 - Spring 14 - von Doetinchem - 15 Force between moving charges http://www.youtube.com/watch?v=43AeuDvWc0k ● Moving in the same direction for likewise signed charges creates an attractive force and moving in the opposite direction creates a repulsive force Phys272 - Spring 14 - von Doetinchem - 16 Magnetic field of a current element ● Superposition principle works for magnetic fields as well: – ● ● The total magnetic field caused by several moving charges is the vector sum of the fields caused by the individual charges. Use to find magnetic field produced by a current in a conductor Chop charge-carrying conductor in short segments: Phys272 - Spring 14 - von Doetinchem - 19 Magnetic field of a current element ● ● Charges travel at average drift velocity (random motions cancel out): Magnetic field of a current element (vector version): Phys272 - Spring 14 - von Doetinchem - 20 Magnetic field of a current element ● ● Law of Biot and Savart: Important law to find the total magnetic field of at any point in space due to the current in a complete circuit Phys272 - Spring 14 - von Doetinchem - 21 Magnetic field calculations ● ● ● ● ● ● ● Make a representative sketch of the current element Draw current element dl → does it point in the direction of the current? Draw the unit vector for the straight connection between the current element and the point you are interested in What is your target variable? Use the superposition principle to find the total magnetic field. Are there any symmetries? Which magnetic field components are zero? Does your result make sense? For instance, is the magnetic field larger or smaller if you are further away from the current element? Phys272 - Spring 14 - von Doetinchem - 22 Magnetic field of a current segment ● Copper wire carries a steady current of 125A to a electroplating tank. What is the magnetic field of 1.0cm long segment in 1.2m distance? Phys272 - Spring 14 - von Doetinchem - 23 Magnetic field of a current segment ● Copper wire carries a steady current of 125A to a electroplating tank. What is the magnetic field of 1.0cm long segment in 1.2m distance? Phys272 - Spring 14 - von Doetinchem - 24 Magnetic field of a straight current-carrying conductor ● ● Straight conducting wires are found in essentially all electric and electronic devices Conductor of a certain length a curring a current I. Find magnetic field along the x axis: Phys272 - Spring 14 - von Doetinchem - 25 Magnetic field of a straight current-carrying conductor ● ● Straight conducting wires are found in essentially all electric and electronic devices Conductor of a certain length a curring a current I. Find magnetic field along the x axis: Phys272 - Spring 14 - von Doetinchem - 26 Magnetic field of a straight current-carrying conductor ● ● ● ● Axial symmetry around the y axis → magnetic field has the same magnitude on all points around a circle centered on the conductor and lying in a plane perpendicular to it Magnetic field direction is always a tangent on the circle Magnetic field lines enclose the current and do not have end points Calculation analog to an infinite sheet of current in the case of electric fields, but magnetic field lines have a different shape Phys272 - Spring 14 - von Doetinchem - 27 Magnetic field of a single wire ● ● Long straight conductor carries 1.0A: at what distance is the magnetic field 50µT (~strength of Earth magnetic field)? Magnetic fields produced by household appliances are typically small → only in close proximity to the conductor the magnetic field is roughly as strong as Earth's magnetic field → falls of as 1/r Phys272 - Spring 14 - von Doetinchem - 28 Magnetic field of two wires ● Two wires carry current in opposite directions. How does the magnetic field on x along the x axis? Phys272 - Spring 14 - von Doetinchem - 29 Magnetic field of two wires ● ● ● At larger distances the magnetic field from the 2wire setup falls of as 1/r2. → The magnetic field from 2 wires carrying current in opposite directions falls of quicker than from a single wire (1/r). Useful effect to minimize the distortion from currentcarrying wires on other cables carrying information In this regard: it can be important to run cables of different types (e.g., cables carrying tiny analog signals and power supply cables) at either larger distances or perpendicular to each other Phys272 - Spring 14 - von Doetinchem - 30